Field of the Invention
[0001] The present invention relates to a smoking substitute apparatus and, in particular,
a smoking substitute apparatus that is able to deliver nicotine to a user in an effective
manner.
Background
[0002] The smoking of tobacco is generally considered to expose a smoker to potentially
harmful substances. It is thought that a significant amount of the potentially harmful
substances are generated through the burning and/or combustion of the tobacco and
the constituents of the burnt tobacco in the tobacco smoke itself.
[0003] Low temperature combustion of organic material such as tobacco is known to produce
tar and other potentially harmful by-products. There have been proposed various smoking
substitute systems in which the conventional smoking of tobacco is avoided.
[0004] Such smoking substitute systems can form part of nicotine replacement therapies aimed
at people who wish to stop smoking and overcome a dependence on nicotine.
[0005] Known smoking substitute systems include electronic systems that permit a user to
simulate the act of smoking by producing an aerosol (also referred to as a "vapour")
that is drawn into the lungs through the mouth (inhaled) and then exhaled. The inhaled
aerosol typically bears nicotine and/or a flavourant without, or with fewer of, the
health risks associated with conventional smoking.
[0006] In general, smoking substitute systems are intended to provide a substitute for the
rituals of smoking, whilst providing the user with a similar, or improved, experience
and satisfaction to those experienced with conventional smoking and with combustible
tobacco products.
[0007] The use of smoking substitute systems has grown rapidly in the past few years as
an aid to assist habitual smokers wishing to quit tobacco smoking. There are a number
of different categories of smoking substitute systems, each utilising a different
smoking substitute approach. Some smoking substitute systems are designed to resemble
a conventional cigarette and are cylindrical in form with a mouthpiece at one end.
Other smoking substitute devices do not generally resemble a cigarette (for example,
the smoking substitute device may have a generally box-like form, in whole or in part).
[0008] One approach is the so-called "vaping" approach, in which a vaporisable liquid, or
an aerosol former, sometimes typically referred to herein as "e-liquid", is heated
by a heating device (sometimes referred to herein as an electronic cigarette or "e-cigarette"
device) to produce an aerosol vapour which is inhaled by a user. The e-liquid typically
includes a base liquid, nicotine and may include a flavourant. The resulting vapour
therefore also typically contains nicotine and/or a flavourant. The base liquid may
include propylene glycol and/or vegetable glycerine.
[0009] A typical e-cigarette device includes a mouthpiece, a power source (typically a battery),
a tank for containing e-liquid and a heating device. In use, electrical energy is
supplied from the power source to the heating device, which heats the e-liquid to
produce an aerosol (or "vapour") which is inhaled by a user through the mouthpiece.
[0010] E-cigarettes can be configured in a variety of ways. For example, there are "closed
system" vaping smoking substitute systems, which typically have a sealed tank and
heating element. The tank is prefilled with e-liquid and is not intended to be refilled
by an end user. One subset of closed system vaping smoking substitute systems include
a main body which includes the power source, wherein the main body is configured to
be physically and electrically couplable to a consumable including the tank and the
heating element. In this way, when the tank of a consumable has been emptied of e-liquid,
that consumable is removed from the main body and disposed of. The main body can then
be reused by connecting it to a new, replacement, consumable. Another subset of closed
system vaping smoking substitute systems are completely disposable, and intended for
one-use only.
[0011] There are also "open system" vaping smoking substitute systems which typically have
a tank that is configured to be refilled by a user. In this way the entire device
can be used multiple times.
[0012] An example vaping smoking substitute system is the myblu™ e-cigarette. The myblu™
e-cigarette is a closed system which includes a main body and a consumable. The main
body and consumable are physically and electrically coupled together by pushing the
consumable into the main body. The main body includes a rechargeable battery. The
consumable includes a mouthpiece and a sealed tank which contains e-liquid. The consumable
further includes a heater, which for this device is a heating filament coiled around
a portion of a wick. The wick is partially immersed in the e-liquid, and conveys e-liquid
from the tank to the heating filament. The system is controlled by a microprocessor
on board the main body. The system includes a sensor for detecting when a user is
inhaling through the mouthpiece, the microprocessor then activating the device in
response. When the system is activated, electrical energy is supplied from the power
source to the heating device, which heats e-liquid from the tank to produce a vapour
which is inhaled by a user through the mouthpiece.
Summary of the Invention
[0013] For a smoking substitute system it is desirable to deliver nicotine into the user's
lungs, where it can be absorbed into the bloodstream. However, the present disclosure
is based in part on a realisation that some prior art smoking substitute systems,
such delivery of nicotine is not efficient. In some prior art systems, the aerosol
droplets have a size distribution that is not suitable for delivering nicotine to
the lungs. Aerosol droplets of a large particle size tend to be deposited in the mouth
and/or upper respiratory tract. Aerosol particles of a small (e.g. sub-micron) particle
size can be inhaled into the lungs but may be exhaled without delivering nicotine
to the lungs. As a result the user would require drawing a longer puff, more puffs,
or vaporising e-liquid with a higher nicotine concentration in order to achieve the
desired experience.
[0014] For example, droplets in the 2 to 3µm range tend to deposit in deep lung, where absorption
of nicotine is the most efficient due to the large surface area and the abundant capillary
distribution in the deep lung. Therefore, aerosols with droplet size distribution
centred in the 2 to 3µm range will deliver an immediate "nicotine hit". Droplets in
the 3 to 10µm range tend to deposit in the upper pulmonary area of the lung, where
nicotine will be absorbed into blood stream in a slower fashion. As a result, the
user will receive a mild but long-lasting nicotine stimulation.
[0015] It is of interest to allow the user of a smoking substitute system a degree of control
over the aerosol particle size inhaled, in part to take advantage over the phenomena
reported above concerning the effect of aerosol particle size on the deposition location
within the user's respiratory system.
[0016] The present disclosure has been devised in the light of the above considerations.
[0017] In a general aspect, the present invention provides suitable user-based control over
the aerosol characteristics by the provision of an occlusion member for covering at
least one air inlet of a smoking substitute apparatus, the configuration of the occlusion
member being determined by a user-selectable engagement of the smoking substitute
apparatus with a main body, the smoking substitute apparatus and the main body together
constituting a smoking substitute system.
[0018] According to a first preferred aspect there is provided a smoking substitute apparatus
comprising:
at least two air inlets;
an aerosol generator for generating an aerosol from an aerosol precursor for inhalation
by a user;
an outlet;
at least one air flow path between the air inlet and the outlet for conveying the
aerosol to the user;
an occlusion member being selectively configurable between a first configuration in
which a first one of said at least two air inlets is covered and a second configuration
in which the first one of the at least two air inlets is uncovered;
wherein the first configuration is selectable by the user based on a first engagement
arrangement between the smoking substitute apparatus and the main body, and the second
configuration is selectable by the user based on a second engagement arrangement between
the smoking substitute apparatus and the main body.
[0019] According to a second preferred aspect, there is provided a method of using a smoking
substitute apparatus including the step of engaging the smoking substitute apparatus
with a main body to provide a smoking substitute system, the smoking substitute apparatus
comprising:
at least two air inlets;
an aerosol generator for generating an aerosol from an aerosol precursor for inhalation
by a user;
an outlet;
at least one air flow path between the air inlet and the outlet for conveying the
aerosol to the user;
and
an occlusion member;
wherein the method further comprises the steps of selectively configuring the occlusion
member between:
- (i) a first configuration in which a first one of the at least two air inlets is covered,
wherein the first configuration is selected by the user based on a first engagement
arrangement between the smoking substitute apparatus and the main body, and
- (ii) a second configuration in which the said first one of the at least two air inlets
in uncovered, wherein the second configuration is selected by the user based on a
second engagement arrangement between the smoking substitute apparatus and the main
body.
[0020] According to a third preferred aspect, there is provided a smoking substitute system
comprising a smoking substitute apparatus and a main body, the smoking substitute
apparatus being engageable with the main body to provide said smoking substitute system,
the smoking substitute apparatus comprising:
at least two air inlets;
an aerosol generator for generating an aerosol from an aerosol precursor for inhalation
by a user;
an outlet;
at least one air flow path between the air inlet and the outlet for conveying the
aerosol to the user;
and
an occlusion member;
wherein the occlusion member is selectively configurable between:
- (i) a first configuration in which a first one of the at least two air inlets is covered,
wherein the first configuration is selected by the user based on a first engagement
arrangement between the smoking substitute apparatus and the main body, and
- (ii) a second configuration in which the said first one of the at least two air inlets
in uncovered, wherein the second configuration is selected by the user based on a
second engagement arrangement between the smoking substitute apparatus and the main
body.
[0021] The aerosol generator may be provided within a vaporisation chamber, discussed in
more detail below. In use, at least a part of the air flow from the air inlet to the
outlet may bypasses the vaporisation chamber. This is also discussed in further detail
below.
[0022] In use, substantially all of the air flow from the air inlet to the outlet may bypass
the vaporisation chamber, the vaporisation chamber having a vaporisation chamber outlet
in communication with a passage along which air flows from the air inlet to the outlet.
This allows particles of aerosol generated by vaporisation of the aerosol precursor
to grow to a suitable size prior to becoming entrained in the air flow and inhaled
by a user. This provides more efficient nicotine delivery to the user. The vaporisation
chamber may be substantially sealed against air flow except for the vaporisation chamber
outlet. This further ensures that the particles of the aerosol enter the air flow
at substantially the same point in time, ensuring a more homogenous distribution of
particle sizes in the air flow.
[0023] A first passage may lead from the air inlet to the outlet, the aerosol generator
being arranged in fluid communication with the first passage, the apparatus may further
comprise an auxiliary passage leading from the air inlet (or from an auxiliary air
inlet) to the outlet, wherein the auxiliary passage bypasses the first passage downstream
of the aerosol generator. This allows the rate of air flow over the aerosol generator
to be maintained at a level low enough to entrain sufficiently sized aerosol particles,
even for a user with a high inhalation flow rate.
[0024] The smoking substitute apparatus may be comprised by or within a cartridge configured
for engagement with the main body, the cartridge and main body together forming a
smoking substitute system. The smoking substitute apparatus may be removably engageable
with the main body (which may also be referred to herein as the base unit).
[0025] The smoking substitute apparatus may be in the form of a consumable. The consumable
may be configured for engagement with a main body. When the consumable is engaged
with the main body, the combination of the consumable and the main body may form a
smoking substitute system such as a closed smoking substitute system. For example,
the consumable may comprise components of the system that are disposable, and the
main body may comprise non-disposable or non-consumable components (e.g. power supply,
controller, sensor, etc.) that facilitate the generation and/or delivery of aerosol
by the consumable. In such an embodiment, the aerosol precursor (e.g. e-liquid) may
be replenished by replacing a used consumable with an unused consumable.
[0026] Alternatively, the smoking substitute apparatus may be a non-consumable apparatus
(e.g. that is in the form of an open smoking substitute system). In such embodiments
an aerosol former (e.g. e-liquid) of the system may be replenished by re-filling,
e.g. a reservoir of the smoking substitute apparatus, with the aerosol precursor (rather
than replacing a consumable component of the apparatus).
[0027] In light of this, it should be appreciated that some of the features described herein
as being part of the smoking substitute apparatus may alternatively form part of a
main body for engagement with the smoking substitute apparatus. This may be the case
in particular when the smoking substitute apparatus is in the form of a consumable.
[0028] Where the smoking substitute apparatus is in the form of a consumable, the main body
and the consumable may be configured to be physically coupled together. For example,
the consumable may be at least partially received in a recess of the main body, such
that there is an interference fit between the main body and the consumable. Alternatively,
the main body and the consumable may be physically coupled together by screwing one
onto the other, or through a bayonet fitting, or the like.
[0029] Thus, the smoking substitute apparatus may comprise one or more engagement portions
for engaging with a main body. In this way, one end of the smoking substitute apparatus
may be coupled with the main body, whilst an opposing end of the smoking substitute
apparatus may define a mouthpiece of the smoking substitute system.
[0030] The smoking substitute apparatus may comprise a reservoir configured to store an
aerosol precursor, such as an e-liquid. The e-liquid may, for example, comprise a
base liquid. The e-liquid may further comprise nicotine. The base liquid may include
propylene glycol and/or vegetable glycerine. The e-liquid may be substantially flavourless.
That is, the e-liquid may not contain any deliberately added additional flavourant
and may consist solely of a base liquid of propylene glycol and/or vegetable glycerine
and nicotine.
[0031] The reservoir may be in the form of a tank. At least a portion of the tank may be
light-transmissive. For example, the tank may comprise a window to allow a user to
visually assess the quantity of e-liquid in the tank. A housing of the smoking substitute
apparatus may comprise a corresponding aperture (or slot) or window that may be aligned
with a light-transmissive portion (e.g. window) of the tank. The reservoir may be
referred to as a "clearomizer" if it includes a window, or a "cartomizer" if it does
not.
[0032] The outlet may be at a mouthpiece of the smoking substitute apparatus. In this respect,
a user may draw fluid (e.g. air) into and through the passage by inhaling at the outlet
(i.e. using the mouthpiece). The passage may be at least partially defined by the
tank. The tank may substantially (or fully) define the passage, for at least a part
of the length of the passage. In this respect, the tank may surround the passage,
e.g. in an annular arrangement around the passage.
[0033] The vaporisation chamber may be arranged to be in fluid communication with the inlet
and outlet of the passage. The vaporisation chamber may be an enlarged portion of
the passage. In this respect, the air as drawn in by the user may entrain the generated
vapour in a flow away from heater. The entrained vapour may form an aerosol in the
vaporisation chamber, or it may form the aerosol further downstream along the passage.
The vaporisation chamber may be at least partially defined by the tank. The tank may
substantially (or fully) define the vaporisation chamber, and thus may form the enclosure.
In this respect, the tank may surround the vaporisation chamber, e.g. in an annular
arrangement around the vaporisation chamber.
[0034] In use, the user may puff on a mouthpiece of the smoking substitute apparatus, i.e.
draw on the smoking substitute apparatus by inhaling, to draw in an air stream therethrough.
The part of the air flow which bypasses the vaporisation chamber (dilution air flow)
may combine with the other part of the air flow (main air flow) for diluting the aerosol
contained therein. The dilution air flow may be directly inhaled by the user without
passing through the passage of the smoking substitute apparatus.
[0035] As a user puffs on the mouthpiece, vaporised e-liquid entrained in the passing air
flow may be drawn towards the outlet of the passage. The vapour may cool, and thereby
nucleate and/or condense along the passage to form a plurality of aerosol droplets,
e.g. nicotine-containing aerosol droplets. A portion of these aerosol droplets may
be delivered to and be absorbed at a target delivery site, e.g. a user's lung, whilst
a portion of the aerosol droplets may instead adhere onto other parts of the user's
respiratory tract, e.g. the user's oral cavity and/or throat. Typically, in some known
smoking substitute apparatuses, the aerosol droplets as measured at the outlet of
the passage, e.g. at the mouthpiece, may have a droplet size, dso, of less than 1
µm.
[0036] In some embodiments of the invention, the dso particle size of the aerosol particles
is preferably at least 1 µm, more preferably at least 2 µm. Typically, the dso particle
size is not more than 10 µm, preferably not more than 9 µm, not more than 8 µm, not
more than 7 µm, not more than 6 µm, not more than 5 µm, not more than 4 µm or not
more than 3 µm. It is considered that providing aerosol particle sizes in such ranges
permits improved interaction between the aerosol particles and the user's lungs.
[0037] The particle droplet size, dso, of an aerosol may be measured by a laser diffraction
technique. For example, the stream of aerosol output from the outlet of the passage
may be drawn through a Malvern Spraytec laser diffraction system, where the intensity
and pattern of scattered laser light are analysed to calculate the size and size distribution
of aerosol droplets. As will be readily understood, the particle size distribution
may be expressed in terms of d
10, d
50 and d
90, for example. Considering a cumulative plot of the volume of the particles measured
by the laser diffraction technique, the d
10 particle size is the particle size below which 10% by volume of the sample lies.
The d
50 particle size is the particle size below which 50% by volume of the sample lies.
The d
90 particle size is the particle size below which 90% by volume of the sample lies.
Unless otherwise indicated herein, the particle size measurements are volume-based
particle size measurements, rather than number-based or mass-based particle size measurements.
[0038] The spread of particle size may be expressed in terms of the span, which is defined
as (d
90-d
10)/d
50. Typically, the span is not more than 20, preferably not more than 10, preferably
not more than 8, preferably not more than 4, preferably not more than 2, preferably
not more than 1, or not more than 0.5.
[0039] The smoking substitute apparatus (or main body engaged with the smoking substitute
apparatus) may comprise a power source. The power source may be electrically connected
(or connectable) to a heater of the smoking substitute apparatus (e.g. when the smoking
substitute apparatus is engaged with the main body). The power source may be a battery
(e.g. a rechargeable battery). A connector in the form of e.g. a USB port may be provided
for recharging this battery.
[0040] When the smoking substitute apparatus is in the form of a consumable, the smoking
substitute apparatus may comprise an electrical interface for interfacing with a corresponding
electrical interface of the main body. One or both of the electrical interfaces may
include one or more electrical contacts. Thus, when the main body is engaged with
the consumable, the electrical interface of the main body may be configured to transfer
electrical power from the power source to a heater of the consumable via the electrical
interface of the consumable.
[0041] The electrical interface of the smoking substitute apparatus may also be used to
identify the smoking substitute apparatus (in the form of a consumable) from a list
of known types. For example, the consumable may have a certain concentration of nicotine
and the electrical interface may be used to identify this. The electrical interface
may additionally or alternatively be used to identify when a consumable is connected
to the main body.
[0042] Again, where the smoking substitute apparatus is in the form of a consumable, the
main body may comprise an identification means, which may, for example, be in the
form of an RFID reader, a barcode or QR code reader. This identification means may
be able to identify a characteristic (e.g. a type) of a consumable engaged with the
main body. In this respect, the consumable may include any one or more of an RFID
chip, a barcode or QR code, or memory within which is an identifier and which can
be interrogated via the identification means.
[0043] The smoking substitute apparatus or main body may comprise a controller, which may
include a microprocessor. The controller may be configured to control the supply of
power from the power source to the heater of the smoking substitute apparatus (e.g.
via the electrical contacts). A memory may be provided and may be operatively connected
to the controller. The memory may include non-volatile memory. The memory may include
instructions which, when implemented, cause the controller to perform certain tasks
or steps of a method.
[0044] The main body or smoking substitute apparatus may comprise a wireless interface,
which may be configured to communicate wirelessly with another device, for example
a mobile device, e.g. via Bluetooth®. To this end, the wireless interface could include
a Bluetooth® antenna. Other wireless communication interfaces, e.g. WiFi®, are also
possible. The wireless interface may also be configured to communicate wirelessly
with a remote server.
[0045] A puff sensor may be provided that is configured to detect a puff (i.e. inhalation
from a user). The puff sensor may be operatively connected to the controller so as
to be able to provide a signal to the controller that is indicative of a puff state
(i.e. puffing or not puffing). The puff sensor may, for example, be in the form of
a pressure sensor or an acoustic sensor. That is, the controller may control power
supply to the heater of the consumable in response to a puff detection by the sensor.
The control may be in the form of activation of the heater in response to a detected
puff. That is, the smoking substitute apparatus may be configured to be activated
when a puff is detected by the puff sensor. When the smoking substitute apparatus
is in the form of a consumable, the puff sensor may be provided in the consumable
or alternatively may be provided in the main body.
[0046] The term "flavourant" is used to describe a compound or combination of compounds
that provide flavour and/or aroma. For example, the flavourant may be configured to
interact with a sensory receptor of a user (such as an olfactory or taste receptor).
The flavourant may include one or more volatile substances.
[0047] The flavourant may be provided in solid or liquid form. The flavourant may be natural
or synthetic. For example, the flavourant may include menthol, liquorice, chocolate,
fruit flavour (including e.g. citrus, cherry etc.), vanilla, spice (e.g. ginger, cinnamon)
and tobacco flavour. The flavourant may be evenly dispersed or may be provided in
isolated locations and/or varying concentrations.
[0048] The present inventors consider that a flow rate of 1.3 L min
-1 is towards the lower end of a typical user expectation of flow rate through a conventional
cigarette and therefore through a user-acceptable smoking substitute apparatus. The
present inventors further consider that a flow rate of 2.0 L min
-1 is towards the higher end of a typical user expectation of flow rate through a conventional
cigarette and therefore through a user-acceptable smoking substitute apparatus. Embodiments
of the present invention therefore provide an aerosol with advantageous particle size
characteristics across a range of flow rates of air through the apparatus.
[0049] The aerosol may have a Dv50 of at least 1.1 µm, at least 1.2 µm, at least 1.3 µm,
at least 1.4 µm, at least 1.5 µm, at least 1.6 µm, at least 1.7 µm, at least 1.8 µm,
at least 1.9 µm or at least 2.0 µm.
[0050] The aerosol may have a Dv50 of not more than 4.9 µm, not more than 4.8 µm, not more
than 4.7 µm, not more than 4.6 µm, not more than 4.5 µm, not more than 4.4 µm, not
more than 4.3 µm, not more than 4.2 µm, not more than 4.1 µm, not more than 4.0 µm,
not more than 3.9 µm, not more than 3.8 µm, not more than 3.7 µm, not more than 3.6
µm, not more than 3.5 µm, not more than 3.4 µm, not more than 3.3 µm, not more than
3.2 µm, not more than 3.1 µm or not more than 3.0 µm.
[0051] A particularly preferred range for Dv50 of the aerosol is in the range 2-3 µm.
[0052] The air inlet, flow passage, outlet and the vaporisation chamber may be configured
so that, when the air flow rate inhaled by the user through the apparatus is 1.3 L
min
-1, the average magnitude of velocity of air in the vaporisation chamber is in the range
0-1.3 ms
-1. The average magnitude velocity of air may be calculated based on knowledge of the
geometry of the vaporisation chamber and the flow rate.
[0053] When the air flow rate inhaled by the user through the apparatus is 1.3 L min
-1, the average magnitude of velocity of air in the vaporisation chamber may be at least
0.001 ms
-1, or at least 0.005 ms
-1, or at least 0.01 ms
-1, or at least 0.05 ms
-1.
[0054] When the air flow rate inhaled by the user through the apparatus is 1.3 L min
-1, the average magnitude of velocity of air in the vaporisation chamber may be at most
1.2 ms
-1, at most 1.1 ms
-1, at most 1.0 ms
-1, at most 0.9 ms
-1, at most 0.8 ms
-1, at most 0.7 ms
-1 or at most 0.6 ms
-1.
[0055] The air inlet, flow passage, outlet and the vaporisation chamber may be configured
so that, when the air flow rate inhaled by the user through the apparatus is 2.0 L
min
-1, the average magnitude of velocity of air in the vaporisation chamber is in the range
0-1.3 ms
-1. The average magnitude velocity of air may be calculated based on knowledge of the
geometry of the vaporisation chamber and the flow rate.
[0056] When the air flow rate inhaled by the user through the apparatus is 2.0 L min
-1, the average magnitude of velocity of air in the vaporisation chamber may be at least
0.001 ms
-1, or at least 0.005 ms
-1, or at least 0.01 ms
-1, or at least 0.05 ms
-1.
[0057] When the air flow rate inhaled by the user through the apparatus is 2.0 L min
-1, the average magnitude of velocity of air in the vaporisation chamber may be at most
1.2 ms
-1, at most 1.1 ms
-1, at most 1.0 ms
-1, at most 0.9 ms
-1, at most 0.8 ms
-1, at most 0.7 ms
-1 or at most 0.6 ms
-1.
[0058] When the calculated average magnitude of velocity of air in the vaporisation chamber
is in the ranges specified, it is considered that the resultant aerosol particle size
is advantageously controlled to be in a desirable range. It is further considered
that the configuration of the apparatus can be selected so that the average magnitude
of velocity of air in the vaporisation chamber can be brought within the ranges specified,
at the exemplary flow rate of 1.3 L min
-1 and/or the exemplary flow rate of 2.0 L min
-1.
[0059] The aerosol generator may comprise a vaporiser element loaded with aerosol precursor,
the vaporiser element being heatable by a heater and presenting a vaporiser element
surface to air in the vaporisation chamber. A vaporiser element region may be defined
as a volume extending outwardly from the vaporiser element surface to a distance of
1 mm from the vaporiser element surface.
[0060] The air inlet, flow passage, outlet and the vaporisation chamber may be configured
so that, when the air flow rate inhaled by the user through the apparatus is 1.3 L
min
-1, the average magnitude of velocity of air in the vaporiser element region is in the
range 0-1.2 ms
-1. The average magnitude of velocity of air in the vaporiser element region may be
calculated using computational fluid dynamics.
[0061] When the air flow rate inhaled by the user through the apparatus is 1.3 L min
-1, the average magnitude of velocity of air in the vaporiser element region may be
at least 0.001 ms
-1, or at least 0.005 ms
-1, or at least 0.01 ms
-1, or at least 0.05 ms
-1.
[0062] When the air flow rate inhaled by the user through the apparatus is 1.3 L min
-1, the average magnitude of velocity of air in the vaporiser element region may be
at most 1.1 ms
-1, at most 1.0 ms
-1, at most 0.9 ms
-1, at most 0.8 ms
-1, at most 0.7 ms
-1 or at most 0.6 ms
-1.
[0063] The air inlet, flow passage, outlet and the vaporisation chamber may be configured
so that, when the air flow rate inhaled by the user through the apparatus is 2.0 L
min
-1, the average magnitude of velocity of air in the vaporiser element region is in the
range 0-1.2 ms
-1. The average magnitude of velocity of air in the vaporiser element region may be
calculated using computational fluid dynamics.
[0064] When the air flow rate inhaled by the user through the apparatus is 2.0 L min
-1, the average magnitude of velocity of air in the vaporiser element region may be
at least 0.001 ms
-1, or at least 0.005 ms
-1, or at least 0.01 ms
-1, or at least 0.05 ms
-1.
[0065] When the air flow rate inhaled by the user through the apparatus is 2.0 L min
-1, the average magnitude of velocity of air in the vaporiser element region may be
at most 1.1 ms
-1, at most 1.0 ms
-1, at most 0.9 ms
-1, at most 0.8 ms
-1, at most 0.7 ms
-1 or at most 0.6 ms
-1.
[0066] When the average magnitude of velocity of air in the vaporiser element region is
in the ranges specified, it is considered that the resultant aerosol particle size
is advantageously controlled to be in a desirable range. It is further considered
that the velocity of air in the vaporiser element region is more relevant to the resultant
particle size characteristics than consideration of the velocity in the vaporisation
chamber as a whole. This is in view of the significant effect of the velocity of air
in the vaporiser element region on the cooling of the vapour emitted from the vaporiser
element surface.
[0067] Additionally or alternatively is it relevant to consider the maximum magnitude of
velocity of air in the vaporiser element region.
[0068] Therefore, the air inlet, flow passage, outlet and the vaporisation chamber may be
configured so that, when the air flow rate inhaled by the user through the apparatus
is 1.3 L min
-1, the maximum magnitude of velocity of air in the vaporiser element region is in the
range 0-2.0 ms
-1.
[0069] When the air flow rate inhaled by the user through the apparatus is 1.3 L min
-1, the maximum magnitude of velocity of air in the vaporiser element region may be
at least 0.001 ms
-1, or at least 0.005 ms
-1, or at least 0.01 ms
-1, or at least 0.05 ms
-1.
[0070] When the airflow rate inhaled by the user through the apparatus is 1.3 L min
-1, the maximum magnitude of velocity of air in the vaporiser element region may be
at most 1.9 ms
-1, at most 1.8 ms
-1, at most 1.7 ms
-1, at most 1.6 ms
-1, at most 1.5 ms
-1, at most 1.4 ms
-1, at most 1.3 ms
-1 or at most 1.2 ms
-1.
[0071] The air inlet, flow passage, outlet and the vaporisation chamber may be configured
so that, when the air flow rate inhaled by the user through the apparatus is 2.0 L
min
-1, the maximum magnitude of velocity of air in the vaporiser element region is in the
range 0-2.0 ms
-1.
[0072] When the air flow rate inhaled by the user through the apparatus is 2.0 L min
-1, the maximum magnitude of velocity of air in the vaporiser element region may be
at least 0.001 ms
-1, or at least 0.005 ms
-1, or at least 0.01 ms
-1, or at least 0.05 ms
-1.
[0073] When the air flow rate inhaled by the user through the apparatus is 2.0 L min
-1, the maximum magnitude of velocity of air in the vaporiser element region may be
at most 1.9 ms
-1, at most 1.8 ms
-1, at most 1.7 ms
-1, at most 1.6 ms
-1, at most 1.5 ms
-1, at most 1.4 ms
-1, at most 1.3 ms
-1 or at most 1.2 ms
-1.
[0074] It is considered that configuring the apparatus in a manner to permit such control
of velocity of the airflow at the vaporiser permits the generation of aerosols with
particularly advantageous particle size characteristics, including Dv50 values.
[0075] Additionally or alternatively is it relevant to consider the turbulence intensity
in the vaporiser chamber in view of the effect of turbulence on the particle size
of the generated aerosol. For example, the air inlet, flow passage, outlet and the
vaporisation chamber may be configured so that, when the air flow rate inhaled by
the user through the apparatus is 1.3 L min
-1, the turbulence intensity in the vaporiser element region is not more than 1%.
[0076] When the air flow rate inhaled by the user through the apparatus is 1.3 L min
-1, the turbulence intensity in the vaporiser element region may be not more than 0.95%,
not more than 0.9%, not more than 0.85%, not more than 0.8%, not more than 0.75%,
not more than 0.7%, not more than 0.65% or not more than 0.6%.
[0077] It is considered that configuring the apparatus in a manner to permit such control
of the turbulence intensity in the vaporiser element region permits the generation
of aerosols with particularly advantageous particle size characteristics, including
Dv50 values.
[0078] Following detailed investigations, the inventors consider, without wishing to be
bound by theory, that the particle size characteristics of the generated aerosol may
be determined by the cooling rate experienced by the vapour after emission from the
vaporiser element (e.g. wick). In particular, it appears that imposing a relatively
slow cooling rate on the vapour has the effect of generating aerosols with a relatively
large particle size. The parameters discussed above (velocity and turbulence intensity)
are considered to be mechanisms for implementing a particular cooling dynamic to the
vapour.
[0079] More generally, it is considered that the air inlet, flow passage, outlet and the
vaporisation chamber may be configured so that a desired cooling rate is imposed on
the vapour. The particular cooling rate to be used depends of course on the nature
of the aerosol precursor and other conditions. However, for a particular aerosol precursor
it is possible to define a set of testing conditions in order to define the cooling
rate, and by extension this imposes limitations on the configuration of the apparatus
to permit such cooling rates as are shown to result in advantageous aerosols. Accordingly,
the air inlet, flow passage, outlet and the vaporisation chamber may be configured
so that the cooling rate of the vapour is such that the time taken to cool to 50 °C
is not less than 16 ms, when tested according to the following protocol. The aerosol
precursor is an e-liquid consisting of 1.6% freebase nicotine and the remainder a
65:35 propylene glycol and vegetable glycerine mixture, the e-liquid having a boiling
point of 209 °C. Air is drawn into the air inlet at a temperature of 25 °C. The vaporiser
is operated to release a vapour of total particulate mass 5 mg over a 3 second duration
from the vaporiser element surface in an air flow rate between the air inlet and outlet
of 1.3 L min
-1.
[0080] Additionally or alternatively, the air inlet, flow passage, outlet and the vaporisation
chamber may be configured so that the cooling rate of the vapour is such that the
time taken to cool to 50 °C is not less than 16 ms, when tested according to the following
protocol. The aerosol precursor is an e-liquid consisting of 1.6% freebase nicotine
and the remainder a 65:35 propylene glycol and vegetable glycerine mixture, the e-liquid
having a boiling point of 209 °C. Air is drawn into the air inlet at a temperature
of 25 °C. The vaporiser is operated to release a vapour of total particulate mass
5 mg over a 3 second duration from the vaporiser element surface in an air flow rate
between the air inlet and outlet of 2.0 L min
-1.
[0081] Cooling of the vapour such that the time taken to cool to 50 °C is not less than
16 ms corresponds to an equivalent linear cooling rate of not more than 10 °C/ms.
[0082] The equivalent linear cooling rate of the vapour to 50 °C may be not more than 9
°C/ms, not more than 8 °C/ms, not more than 7 °C/ms, not more than 6 °C/ms or not
more than 5 °C/ms.
[0083] Cooling of the vapour such that the time taken to cool to 50 °C is not less than
32 ms corresponds to an equivalent linear cooling rate of not more than 5 °C/ms.
[0084] The testing protocol set out above considers the cooling of the vapour (and subsequent
aerosol) to a temperature of 50 °C. This is a temperature which can be considered
to be suitable for an aerosol to exit the apparatus for inhalation by a user without
causing significant discomfort. It is also possible to consider cooling of the vapour
(and subsequent aerosol) to a temperature of 75 °C. Although this temperature is possibly
too high for comfortable inhalation, it is considered that the particle size characteristics
of the aerosol are substantially settled by the time the aerosol cools to this temperature
(and they may be settled at still higher temperature).
[0085] Accordingly, the air inlet, flow passage, outlet and the vaporisation chamber may
be configured so that the cooling rate of the vapour is such that the time taken to
cool to 75 °C is not less than 4.5 ms, when tested according to the following protocol.
The aerosol precursor is an e-liquid consisting of 1.6% freebase nicotine and the
remainder a 65:35 propylene glycol and vegetable glycerine mixture, the e-liquid having
a boiling point of 209 °C. Air is drawn into the air inlet at a temperature of 25
°C. The vaporiser is operated to release a vapour of total particulate mass 5 mg over
a 3 second duration from the vaporiser element surface in an air flow rate between
the air inlet and outlet of 1.3 L min
-1.
[0086] Additionally or alternatively, the air inlet, flow passage, outlet and the vaporisation
chamber may be configured so that the cooling rate of the vapour is such that the
time taken to cool to 75 °C is not less than 4.5 ms, when tested according to the
following protocol. The aerosol precursor is an e-liquid consisting of 1.6% freebase
nicotine and the remainder a 65:35 propylene glycol and vegetable glycerine mixture,
the e-liquid having a boiling point of 209 °C. Air is drawn into the air inlet at
a temperature of 25 °C. The vaporiser is operated to release a vapour of total particulate
mass 5 mg over a 3 second duration from the vaporiser element surface in an air flow
rate between the air inlet and outlet of 2.0 L min
-1.
[0087] Cooling of the vapour such that the time taken to cool to 75 °C is not less than
4.5 ms corresponds to an equivalent linear cooling rate of not more than 30 °C/ms.
[0088] The equivalent linear cooling rate of the vapour to 75 °C may be not more than 29
°C/ms, not more than 28 °C/ms, not more than 27 °C/ms, not more than 26 °C/ms, not
more than 25 °C/ms, not more than 24 °C/ms, not more than 23 °C/ms, not more than
22 °C/ms, not more than 21 °C/ms, not more than 20 °C/ms, not more than 19 °C/ms,
not more than 18 °C/ms, not more than 17 °C/ms, not more than 16 °C/ms, not more than
15 °C/ms, not more than 14 °C/ms, not more than 13 °C/ms, not more than 12 °C/ms,
not more than 11 °C/ms or not more than 10 °C/ms.
[0089] Cooling of the vapour such that the time taken to cool to 75 °C is not less than
13 ms corresponds to an equivalent linear cooling rate of not more than 10 °C/ms.
[0090] It is considered that configuring the apparatus in a manner to permit such control
of the cooling rate of the vapour permits the generation of aerosols with particularly
advantageous particle size characteristics, including Dv50 values.
[0091] The first and second configurations of the smoking substitute apparatus permit the
user to control aspects of the air flow conditions within the apparatus that affect
the aerosol particle size for the reasons discussed in detail above. In the first
configuration, in which a first one of said at least two air inlets is covered, the
air flow path is between an uncovered air inlet and the outlet. Depending on the positioning
of the air inlets relative to the vaporisation chamber and depending on whether there
is one or more auxiliary air inlets, the effect of the first configuration can be
that there is reduced air flow and/or reduced turbulence at or immediately downstream
from the vaporisation chamber. This allows an aerosol to be formed with larger droplet
sizes. In the second configuration, in which both of the at least two air inlets are
uncovered, the effect of the second configuration can be that there is increased air
flow and/or increased turbulence at or immediately downstream from the vaporisation
chamber. This allows an aerosol to be formed with smaller droplet sizes. Similarly,
the control over the air flow characteristics from the air inlets permits control
over the total particulate mass (TPM) of aerosol delivered to the user.
[0092] The apparatus is configured to have at least two air inlets. For example, the apparatus
may have, for example, two, three, four or five air inlets. In use, at least one of
the at least two air inlets typically provides at least one air flow path between
the air inlet and the outlet for conveying the aerosol to the user. For example, two
air inlets may provide one or two air flow paths, three air inlets may provide one,
two or three air flow paths etc. When the occlusion member is in a first configuration,
one of the at least two air inlets is covered, for example, in an apparatus comprising
two air inlets, one of the air inlets is covered, and in an apparatus comprising three
air inlets, one or two of the air inlets is covered. When the occlusion member is
in a second configuration, at least one of the air inlets is uncovered. This is to
ensure that the apparatus is operable when the occlusion member is in a first configuration
and in a second configuration.
[0093] A further advantage of the present invention is that the smoking substitute apparatus
can be used with an existing main body, because the occlusion member is provided as
part of the smoking substitute apparatus.
[0094] In a preferred embodiment, the occlusion member is biased towards the second configuration.
The second configuration, as a default position, for the reasons explained above may
in some embodiments provide a smaller aerosol droplet size (to provide a "nicotine
hit" to the user) and an increased TPM. The occlusion member may be biased towards
the second configuration by, for example, the occlusion member comprising a resilient
material.
[0095] Preferably, the occlusion member is a deformable plate. This enables the occlusion
member to be changed from its original shape so that it can be configured between
the first configuration and the second configuration. The first configuration may
therefore be a substantially flat configuration of the plate, covering the air inlet.
The second configuration may by a curved configuration of the plate, the curvature
of the plate allowing air ingress between at least part of the plate and the air inlet.
In this way, the degree of deformation of the occlusion member determines the degree
of occlusion of the air inlet and therefore the degree to which air flow at the air
inlet is restricted.
[0096] Preferably, the occlusion member is arranged such that when the user pushes the smoking
substitute apparatus towards the main body, from the second engagement arrangement
to the first engagement arrangement, the occlusion member is forced into the first
configuration.
[0097] The smoking substitute apparatus and the main body may be brought into engagement
by insertion of part of the smoking substitute apparatus into a corresponding recess
of the main body. The difference between the second and first engagement arrangements
may therefore amount to a difference in the insertion distance of the smoking substitute
apparatus into the main body.
[0098] There may be defined a minimum configuration distance for the smoking substitute
apparatus with respect to the main body. This is intended to define the difference
in relative distance between the first engagement arrangement and the second engagement
arrangement. Starting from the first engagement arrangement, the user may pull the
smoking substitute apparatus the minimum configuration distance away from the main
body to reach the second engagement arrangement so that the occlusion member reaches
(or return to) the second configuration. It is advantageous for the system to provide
the user with a haptic indication of reaching the first and/or second engagement arrangement.
For example, the user may feel or hear a 'click' to alert the user when the minimum
configuration distance is reached, indicating that the system is in the second engagement
arrangement and therefore that the occlusion member is in the second configuration.
The minimum configuration distance may for example be about 1mm, 2mm, 3mm, 4mm, 5mm,
6mm, 7mm, 8mm, 9mm or 1cm.
[0099] The invention includes the combination of the aspects and preferred features described
except where such a combination is clearly impermissible or expressly avoided.
Summary of the Figures
[0100] So that the invention may be understood, and so that further aspects and features
thereof may be appreciated, embodiments illustrating the principles of the invention
will now be discussed in further detail with reference to the accompanying figures,
in which:
Figure 1 illustrates a set of rectangular tubes for use in experiments to assess the
effect of flow and cooling conditions at the wick on aerosol properties. Each tube
has the same depth and length but different width.
Figure 2 shows a schematic perspective longitudinal cross sectional view of an example
rectangular tube with a wick and heater coil installed.
Figure 3 shows a schematic transverse cross sectional view an example rectangular
tube with a wick and heater coil installed. In this example, the internal width of
the tube is 12 mm.
Figures 4A-4D show air flow streamlines in the four devices used in a turbulence study.
Figure 5 shows the experimental set up to investigate the influence of inflow air
temperature on aerosol particle size, in order to investigate the effect of vapour
cooling rate on aerosol generation.
Figure 6 shows a schematic longitudinal cross sectional view of a first smoking substitute
apparatus (pod 1) used to assess influence of inflow air temperature on aerosol particle
size.
Figure 7 shows a schematic longitudinal cross sectional view of a second smoking substitute
apparatus (pod 2) used to assess influence of inflow air temperature on aerosol particle
size.
Figure 8A shows a schematic longitudinal cross sectional view of a third smoking substitute
apparatus (pod 3) used to assess influence of inflow air temperature on aerosol particle
size. Figure 8B shows a schematic longitudinal cross sectional view of the same third
smoking substitute apparatus (pod 3) in a direction orthogonal to the view taken in
Figure 8A.
Figure 9 shows a plot of aerosol particle size (Dv50) experimental results against
calculated air velocity.
Figure 10 shows a plot of aerosol particle size (Dv50) experimental results against
the flow rate through the apparatus for a calculated air velocity of 1 m/s.
Figure 11 shows a plot of aerosol particle size (Dv50) experimental results against
the average magnitude of the velocity in the vaporiser surface region, as obtained
from CFD modelling.
Figure 12 shows a plot of aerosol particle size (Dv50) experimental results against
the maximum magnitude of the velocity in the vaporiser surface region, as obtained
from CFD modelling.
Figure 13 shows a plot of aerosol particle size (Dv50) experimental results against
the turbulence intensity.
Figure 14 shows a plot of aerosol particle size (Dv50) experimental results dependent
on the temperature of the air and the heating state of the apparatus.
Figure 15 shows a plot of aerosol particle size (Dv50) experimental results against
vapour cooling rate to 50°C.
Figure 16 shows a plot of aerosol particle size (Dv50) experimental results against
vapour cooling rate to 75°C.
Figure 17 is a schematic front view of a smoking substitute system, according to a
first embodiment, in an engaged position;
Figure 18 is a schematic front view of the smoking substitute system of the first
embodiment in a disengaged position;
Figure 19 is a schematic longitudinal cross sectional view of a smoking substitute
apparatus of a first reference arrangement;
Figure 20 is an enlarged schematic cross sectional view of part of the air passage
and vaporisation chamber of the first reference arrangement;
Figure 21 shows a schematic cross sectional view of a smoking substitute apparatus
of a further reference arrangement;
Figure 22 shows a schematic cross sectional view of a smoking substitute apparatus
of another reference arrangement.
Figure 23 shows a schematic partial cross sectional view of a smoking substitute apparatus
according to an embodiment of the invention when the occlusion member is in a first
configuration.
Figure 24 shows the embodiment of Figure 23 but with the occlusion member removed,
corresponding to a second configuration.
Figure 25 shows a schematic partial perspective view of the base of the smoking substitute
apparatus of Figure 23 when the occlusion member is in the first configuration.
Figure 26 shows a schematic partial perspective view of the base of the smoking substitute
apparatus of Figure 23 when the occlusion member is in the second configuration.
Figure 27 is a perspective side view of a smoking substitute system according to an
embodiment of the invention when the smoking substitute apparatus is in a first engagement
arrangement with the main body.
Figure 28 is a perspective side view of a smoking substitute system according to an
embodiment of the invention when the smoking substitute apparatus is in a second engagement
arrangement with the main body.
Figure 29 shows an enlarged schematic perspective cross sectional view taken parallel
to the principal axis of the wick and parallel to the principal axis of the apparatus,
showing interior features of the smoking substitute apparatus and the main body when
the occlusion member is in the second configuration.
Figure 30 shows an enlarged schematic perspective cross sectional view taken parallel
to the principal axis of the wick and parallel to the principal axis of the apparatus,
showing interior features of the smoking substitute apparatus and the main body when
the occlusion member is in the first configuration.
Detailed Description of the Invention
[0101] Further background to the present invention and further aspects and embodiments of
the present invention will now be discussed with reference to the accompanying figures.
Further aspects and embodiments will be apparent to those skilled in the art. The
contents of all documents mentioned in this text are incorporated herein by reference
in their entirety.
[0102] Figures 17 and 18 illustrate a smoking substitute system in the form of an e-cigarette
system 110. The system 110 comprises a main body 120 of the system 110, and a smoking
substitute apparatus in the form of an e-cigarette consumable (or "pod") 150. In the
illustrated embodiment the consumable 150 (sometimes referred to herein as a smoking
substitute apparatus) is removable from the main body 120, so as to be a replaceable
component of the system 110. The e-cigarette system 110 is a closed system in the
sense that it is not intended that the consumable should be refillable with e-liquid
by a user.
[0103] As is apparent from Figures 17 and 18, the consumable 150 is configured to engage
the main body 120. Figure 17 shows the main body 120 and the consumable 150 in an
engaged state, whilst Figure 18 shows the main body 120 and the consumable 150 in
a disengaged state. When engaged, a portion of the consumable 150 is received in a
cavity of corresponding shape in the main body 120 and is retained in the engaged
position by way of a snap-engagement mechanism. In other embodiments, the main body
120 and consumable 150 may be engaged by screwing one into (or onto) the other, or
through a bayonet fitting, or by way of an interference fit.
[0104] The system 110 is configured to vaporise an aerosol precursor, which in the illustrated
embodiment is in the form of a nicotine-based e-liquid 160. The e-liquid 160 comprises
nicotine and a base liquid including propylene glycol and/or vegetable glycerine.
In the present embodiment, the e-liquid 160 is flavoured by a flavourant. In other
embodiments, the e-liquid 160 may be flavourless and thus may not include any added
flavourant.
[0105] Figure 19 shows a schematic longitudinal cross sectional view of a first reference
arrangement of the smoking substitute apparatus forming part of the smoking substitute
system shown in Figures 17 and 18. In Figure 19, the e-liquid 160 is stored within
a reservoir in the form of a tank 152 that forms part of the consumable 150. In the
illustrated first reference arrangement, the consumable 150 is a "single-use" consumable
150. That is, upon exhausting the e-liquid 160 in the tank 152, the intention is that
the user disposes of the entire consumable 150. The term "single-use" does not necessarily
mean the consumable is designed to be disposed of after a single smoking session.
Rather, it defines the consumable 150 is not arranged to be refilled after the e-liquid
contained in the tank 152 is depleted. The tank may include a vent (not shown) to
allow ingress of air to replace e-liquid that has been used from the tank. The consumable
150 preferably includes a window 158 (see Figures 17 and 18), so that the amount of
e-liquid in the tank 152 can be visually assessed. The main body 120 includes a slot
157 so that the window 158 of the consumable 150 can be seen whilst the rest of the
tank 152 is obscured from view when the consumable 150 is received in the cavity of
the main body 120. The consumable 150 may be referred to as a "clearomizer" when it
includes a window 158, or a "cartomizer" when it does not.
[0106] In some embodiments, the e-liquid (i.e. aerosol precursor) may be the only part of
the system that is truly "single-use". That is, the tank may be refillable with e-liquid
or the e-liquid may be stored in a non-consumable component of the system. For example,
in such embodiments, the e-liquid may be stored in a tank located in the main body
or stored in another component that is itself not single-use (e.g. a refillable cartomizer).
[0107] The external wall of tank 152 is provided by a casing of the consumable 150. The
tank 152 annularly surrounds, and thus defines a portion of, a passage 170 that extends
between a vaporiser inlet 172 and an outlet 174 at opposing ends of the consumable
150. In this respect, the passage 170 comprises an upstream end at the end of the
consumable 150 that engages with the main body 120, and a downstream end at an opposing
end of the consumable 150 that comprises a mouthpiece 154 of the system 110.
[0108] When the consumable 150 is received in the cavity of the main body 120 as shown in
Figure 19, a plurality of device air inlets 176 are formed at the boundary between
the casing of the consumable and the casing of the main body. The device air inlets
176 are in fluid communication with the vaporiser inlet 172 through an inlet flow
channel 178 formed in the cavity of the main body which is of corresponding shape
to receive a part of the consumable 150. Air from outside of the system 110 can therefore
be drawn into the passage 170 through the device air inlets 176 and the inlet flow
channels 178.
[0109] When the consumable 150 is engaged with the main body 120, a user can inhale (i.e.
take a puff) via the mouthpiece 154 so as to draw air through the passage 170, and
so as to form an airflow (indicated by the dashed arrows in Figure 19) in a direction
from the vaporiser inlet 172 to the outlet 174. Although not illustrated, the passage
170 may be partially defined by a tube (e.g. a metal tube) extending through the consumable
150. In Figure 19, for simplicity, the passage 170 is shown with a substantially circular
cross-sectional profile with a constant diameter along its length. In some embodiments,
the passage may have other cross-sectional profiles, such as oval shaped or polygonal
shaped profiles. Further, in other embodiments, the cross sectional profile and the
diameter (or hydraulic diameter) of the passage may vary along its longitudinal axis.
[0110] The smoking substitute system 110 is configured to vaporise the e-liquid 160 for
inhalation by a user. To provide this operability, the consumable 150 comprises a
heater having a porous wick 162 and a resistive heating element in the form of a heating
filament 164 that is helically wound (in the form of a coil) around a portion of the
porous wick 162. The porous wick 162 extends across the passage 170 (i.e. transverse
to a longitudinal axis of the passage 170 and thus also transverse to the air flow
along the passage 170 during use) and opposing ends of the wick 162 extend into the
tank 152 (so as to be immersed in the e-liquid 160). In this way, e-liquid 160 contained
in the tank 152 is conveyed from the opposing ends of the porous wick 162 to a central
portion of the porous wick 162 so as to be exposed to the airflow in the passage 170.
[0111] The helical filament 164 is wound about the exposed central portion of the porous
wick 162 and is electrically connected to an electrical interface in the form of electrical
contacts 156 mounted at the end of the consumable that is proximate the main body
120 (when the consumable and the main body are engaged). When the consumable 150 is
engaged with the main body 120, electrical contacts 156 make contact with corresponding
electrical contacts (not shown) of the main body 120. The main body electrical contacts
are electrically connectable to a power source (not shown) of the main body 120, such
that (in the engaged position) the filament 164 is electrically connectable to the
power source. In this way, power can be supplied by the main body 120 to the filament
164 in order to heat the filament 164. This heats the porous wick 162 which causes
e-liquid 160 conveyed by the porous wick 162 to vaporise and thus to be released from
the porous wick 162. The vaporised e-liquid becomes entrained in the airflow and,
as it cools in the airflow (between the heated wick and the outlet 174 of the passage
170), condenses to form an aerosol. This aerosol is then inhaled, via the mouthpiece
154, by a user of the system 110. As e-liquid is lost from the heated portion of the
wick, further e-liquid is drawn along the wick from the tank to replace the e-liquid
lost from the heated portion of the wick.
[0112] The filament 164 and the exposed central portion of the porous wick 162 are positioned
across the passage 170. More specifically, the part of passage that contains the filament
164 and the exposed portion of the porous wick 162 forms a vaporisation chamber. In
the illustrated example, the vaporisation chamber has the same cross-sectional diameter
as the passage 170. However, in some embodiments the vaporisation chamber may have
a different cross sectional profile compared with the passage 170. For example, the
vaporisation chamber may have a larger cross sectional diameter than at least some
of the downstream part of the passage 170 so as to enable a longer residence time
for the air inside the vaporisation chamber.
[0113] Figure 20 illustrates in more detail the vaporisation chamber and therefore the region
of the consumable 150 around the wick 162 and filament 164. The helical filament 164
is wound around a central portion of the porous wick 162. The porous wick extends
across passage 170. E-liquid 160 contained within the tank 152 is conveyed as illustrated
schematically by arrows 401, i.e. from the tank and towards the central portion of
the porous wick 162.
[0114] When the user inhales, air is drawn from through the inlets 176 shown in Figure 19,
along inlet flow channel 178 to vaporisation chamber inlet 172 and into the vaporisation
chamber containing porous wick 162. The porous wick 162 extends substantially transverse
to the airflow direction. The airflow passes around the porous wick, at least a portion
of the airflow substantially following the surface of the porous wick 162. In examples
where the porous wick has a cylindrical cross-sectional profile, the airflow may follow
a curved path around an outer periphery of the porous wick 162.
[0115] At substantially the same time as the airflow passes around the porous wick 162,
the filament 164 is heated so as to vaporise the e-liquid which has been wicked into
the porous wick. The airflow passing around the porous wick 162 picks up this vaporised
e-liquid, and the vapour-containing airflow is drawn in direction 403 further down
passage 170.
[0116] The power source of the main body 120 may be in the form of a battery (e.g. a rechargeable
battery such as a lithium ion battery). The main body 120 may comprise a connector
in the form of e.g. a USB port for recharging this battery. The main body 120 may
also comprise a controller that controls the supply of power from the power source
to the main body electrical contacts (and thus to the filament 164). That is, the
controller may be configured to control a voltage applied across the main body electrical
contacts, and thus the voltage applied across the filament 164. In this way, the filament
164 may only be heated under certain conditions (e.g. during a puff and/or only when
the system is in an active state). In this respect, the main body 120 may include
a puff sensor (not shown) that is configured to detect a puff (i.e. inhalation). The
puff sensor may be operatively connected to the controller so as to be able to provide
a signal, to the controller, which is indicative of a puff state (i.e. puffing or
not puffing). The puff sensor may, for example, be in the form of a pressure sensor
or an acoustic sensor.
[0117] Although not shown, the main body 120 and consumable 150 may comprise a further interface
which may, for example, be in the form of an RFID reader, a barcode or QR code reader.
This interface may be able to identify a characteristic (e.g. a type) of a consumable
150 engaged with the main body 120. In this respect, the consumable 150 may include
any one or more of an RFID chip, a barcode or QR code, or memory within which is an
identifier and which can be interrogated via the interface.
[0118] An apparatus according to an embodiment of the invention may be configured such that
in use, at least part of the air flow drawn by a user through the apparatus from the
air inlet to the outlet bypasses the vaporisation chamber defined by the enclosure.
A second reference arrangement of an apparatus, shown in Figure 21, provides an example
of how such a bypassing air flow may be created. Accordingly, some embodiments of
the invention may include one or a combination of the features of the second reference
arrangement (and variations thereof) where such features are combinable with the present
invention. This second reference arrangement is described below.
[0119] Figure 21 illustrates a schematic longitudinal cross sectional view of a second reference
arrangement of the smoking substitute apparatus forming part of the smoking substitute
system shown in Figures 17 and 18. The arrangement illustrated in Figure 21 differs
from the first reference arrangement illustrated in Figure 19 in that the substitute
smoking apparatus includes two bypass passages 180 in addition to the vaporiser passage
170. The bypass air passages extend between the plurality of device air inlets 176
and two outlets 184. In other variations of the second reference arrangement, the
number of bypass passages 180 and corresponding outlets 184 may be greater or smaller
than in the illustrated example. Furthermore, there may be more or fewer air inlets
and there may be more or fewer outlets.
[0120] In Figure 21 for simplicity, the bypass passage 180 is shown with a substantially
circular cross-sectional profile with a constant diameter along its length. In some
variations of the second reference arrangement, the bypass passage 180 may have other
cross-sectional profiles, such as oval shaped or polygonal shaped profiles. Further,
in some variations of the second reference arrangement, the cross sectional profile
and the diameter (or hydraulic diameter) of the bypass passage 180 may vary along
its longitudinal axis.
[0121] The provision of a bypass passage 180 means that a part of the air drawn through
the smoking substitute apparatus 150a when a user inhales via the mouthpiece 154 is
not drawn through the vaporisation chamber. This has the effect of reducing the flow
rate through the vaporisation chamber in correspondence with the respective flow resistances
presented by the vaporiser passage 170 and the bypass passage 180. This can reduce
the correlation between the flow rate through the smoking substitute apparatus 150a
(i.e. the user's draw rate) and the particle size generated when the e-liquid 160
is vaporised and subsequently forms an aerosol. Therefore, the smoking substitute
apparatus 150a of the second reference arrangement can deliver a more consistent aerosol
to a user.
[0122] Furthermore, the smoking substitute apparatus 150a of the second reference arrangement
is capable of producing an increased particle droplet size, dso, based on typical
inhalation rates undertaken by a user, compared to the first reference arrangement
of Figure 19. Such larger droplet sizes may be beneficial for the delivery of vapour
to a user's lungs. The preferred ratio between the dimensions of the bypass passage
180 and the dimensions of the vaporiser passage 170, and hence flow rate in the respective
passages may be determined from representative user inhalation rates and from the
required air flow rate through the vaporisation chamber to deliver a desired droplet
size. For example, an average total flow rate of 1.3 litres per minute may be split
such that 0.8 litres per minute passes through the bypass air channel 180, and 0.5
litres per minute passes through the vaporiser channel 170, a bypass:vaporiser flow
rate ratio of 1.6:1. Such a flow rate may provide an average droplet size, dso, of
1-3 µm (more preferably 2-3 µm) with a span of not more than 20 (preferably not more
than 10). Alternative flow rate ratios may be provided based on calculations and measurements
of user flow rate, vaporiser flow rate, and average droplet size dso. A bypass:vaporiser
flow rate ratio of between 0.5:1 and 20:1, typically at an average total flow rate
of 1.3 litres per minute may be advantageous depending on the configuration of the
smoking substitute apparatus.
[0123] The bypass passage and vaporiser passage extend from a common device inlet 176. This
has the benefit of ensuring more consistent airflow through the bypass passage 180
and vaporiser passage 170 across the lifetime of the smoking substitute apparatus
150a, since any obstruction that impinges on an air inlet 176 will affect the airflow
through both passages equally. The impact of inlet manufacturing variations can also
be reduced for the same reason. This can therefore improve the user experience for
the smoking substitute apparatus 150a. Furthermore, the provision of a common device
inlet 176 simplifies the construction and external appearance of the device.
[0124] The bypass passage 180 and vaporiser passage 170 separate upstream of the vaporisation
chamber. Therefore, no vapour is drawn through the bypass passage 180. Furthermore,
because the bypass passage leads to outlet 184 that is separate from outlet 174 of
the vaporiser passage, substantially no mixing of the bypass air and vaporiser air
occurs within the smoking substitute apparatus 150a. Such mixing could otherwise lead
to excessive cooling of the vapour and hence a build-up of condensation within the
smoking substitute apparatus 150a. Such condensation could have adverse implications
for delivering vapour to the user, for example by causing the user to draw liquid
droplets rather than vapour when "puffing" on the mouthpiece 154.
[0125] A further example of a bypass air flow is presented by a third reference arrangement.
Accordingly, in some embodiments, the apparatus may include one or a combination of
features of a third reference arrangement (and variations thereof), shown schematically
in Figure 22, where such features are combinable with the present invention. This
third reference arrangement is described below.
[0126] Figure 22 illustrates a longitudinal cross sectional view of a consumable 250 according
to a further arrangement. In Figure 22, the consumable 250 is shown attached, at a
first end of the consumable 250, to the main body 120 of Figure 17 and Figure 18.
More specifically, the consumable 250 is configured to engage and disengage with the
main body 120 and is interchangeable with the first reference arrangement 150 as shown
in Figures 19 and 20. Furthermore, the consumable 250 is configured to interact with
the main body 120 in the same manner as the first reference arrangement 150 and the
user may operate the consumable 250 in the same manner as the first reference arrangement
150.
[0127] The consumable 250 comprises a housing. The consumable 250 comprises an aerosol generation
chamber 280 in the housing. As shown in Figure 26, the aerosol generation chamber
280 takes the form of an open ended container, or a cup, with a single chamber outlet
282 opened towards the outlet 274 of the consumable 250.
[0128] In the illustrated third reference arrangement, the housing has a plurality of air
inlets 272 defined or opened at the sidewall of the housing. An outlet 274 is defined
or opened at a second end of the consumable 250 that comprises a mouthpiece 254. A
pair of passages 270 each extend between the respective air inlets 272 and the outlet
274 to provide flow passage for an air flow 412 as a user puffs on the mouthpiece
254. The chamber outlet 282 is configured to be in fluid communication with the passages
270. The passages 270 extend from the air inlets 272 towards the first end of the
consumable 250 before routing back to towards the outlet 274 at the second end of
the consumable 250. That is, a portion of each of the passages 270 axially extends
alongside the aerosol generation chamber 280. The path of the air flow path 412 is
illustrated in Figure 22. In variations of the third reference arrangement, the passages
270 may extend from the air inlet 272 directly to the outlet 274 without routing towards
the first end of consumable 250, e.g. the passages 270 may not axially extend alongside
the aerosol generation chamber 280.
[0129] In some other variations of the third reference arrangement, the housing may not
be provided with any air inlet for an air flow to enter the housing. For example,
the chamber outlet may be directly connected to the outlet of the housing by an aerosol
passage and therefore said aerosol passage may only convey aerosol as generated in
the aerosol generation chamber. In these variations, the discharge of aerosol may
be driven at least in part by the pressure increase during vaporisation of aerosol
form.
[0130] Referring back to the third reference arrangement of Figure 22, the chamber outlet
282 is positioned downstream from the heater in the direction of the vapour and/or
aerosol flow 414 and serves as the only gas flow passage to the internal volume of
the aerosol generation chamber 280. In other words, the aerosol generation chamber
280 is sealed against air flow except for having the chamber outlet 282 in communication
with the passages 270, the chamber outlet 282 permitting, in use, aerosol generated
by the heater to be entrained into an air flow along the passage 270. In some other
variations of the third reference arrangement, the sealed aerosol generation chamber
280 may comprise a plurality of chamber outlets 282 each arranged in fluid commutation
with the passages 270. In the illustrated third reference arrangement, the aerosol
generation chamber 280 does not comprise any aperture upstream of the heater that
may serve as an air flow inlet (although in some arrangements a vent may be provided).
In contrast with the consumable 150 as shown in Figures 19 and 20, the passages 270
of the consumable 250 allow the air flow, e.g. an entire amount of air flow, entering
the housing to bypass the aerosol generation chamber 280. Such arrangement allows
aerosol precursor to be vaporised in absence of the air flow. Therefore, the aerosol
generation chamber may be considered to be a "stagnant" chamber. For example, the
volumetric flowrate of vapour and/or aerosol in the aerosol generation chamber is
configured to be less than 0.1 litre per minute. The vaporised aerosol precursor may
cool and therefore condense to form an aerosol in the aerosol generation chamber 280,
which is subsequently expulsed into or entrained with the air flow in passages 270.
In addition, a portion of the vaporised aerosol precursor may remain as a vapour before
leaving the aerosol generation chamber 280, and subsequently forms an aerosol as it
is cooled by the air flow in the passages 270. The flow path of the vapour and/or
aerosol 414 is illustrated in Figure 22.
[0131] In the illustrated third reference arrangement, the chamber outlet 282 is configured
to be in fluid communication with a junction 290 at each of the passages 270 through
a respective vapour channel 292. The junctions 290 merge the vapour channels 292 with
their respective passages 270 such that vapour and/or aerosol formed in the aerosol
generation chamber 280 may expand or entrain into the passages 270 through junction
inlets of said junctions 290. The vapour channels form a buffering volume to minimise
the amount of air flow that may back flow into the aerosol generation chamber 280.
In some other variations of the third reference arrangement (not illustrated), the
chamber outlet 282 may directly open towards the junction 290 at the passage, and
therefore in such variations the vapour channel 292 may be omitted.
[0132] In some variations of the third reference arrangement (not illustrated), the chamber
outlet may be closed by a one way valve. Said one way valve may be configured to allow
a one way flow passage for the vapour and/or aerosol to be discharged from the aerosol
generation chamber, and to reduce or prevent the air flow in the passages from entering
the aerosol generation chamber.
[0133] In the illustrated third reference arrangement, the aerosol generation chamber 280
is configured to have a length of 20mm and a volume of 680mm
3. The aerosol generation chamber is configured to allow vapour to be expulsed through
the chamber outlet at a rate greater than 0.1mg/second. In other variations of the
third reference arrangement the aerosol generation chamber may be configured to have
an internal volume ranging between 68mm
3 to 680mm
3, wherein the length of the aerosol generation chamber may range between 2mm to 20mm.
[0134] As shown in Figure 22, a part of each of the passages 270 axially extends alongside
the aerosol generation chamber 280. For example, the passages 270 are formed between
the aerosol generation chamber 280 and the housing. Such an arrangement reduces heat
transfer from the aerosol generation chamber 280 to the external surfaces of the housing.
[0135] The aerosol generation chamber 280 comprises a heater extending across its width.
The heater comprises a porous wick 262 and a heating filament 264 helically wound
around a portion of the porous wick 162. A tank 252 is provided in the space between
the aerosol generation chamber 280 and the outlet 274, the tank being for storing
a reservoir of aerosol precursor. Therefore in contrast with the reference arrangement
as shown in Figures 19 and 20, the tank 252 in the third reference arrangement does
not substantially surround the aerosol generation chamber nor the passage 270. Instead,
as shown in Figure 22, the tank is substantially positioned above the aerosol generation
chamber 280 and the porous wick 262 when the consumable 250 is placed in an upright
orientation during use. The end portions of the porous wick 262 each extend through
the sidewalls of the aerosol generation chamber 280 and into a respective liquid conduit
266 which is in fluid communication with the tank 252. The wick 262, saturated with
aerosol precursor, may prevent gas flow passage into the liquid conduits 266 and the
tank 252. Such an arrangement may allow the aerosol precursor stored in the tank 252
to convey towards the porous wick 262 through the liquid conduits 266 by gravity.
The liquid conduits 266 are configured to have a hydraulic diameter that allow a controlled
amount of aerosol precursor to flow from the tank 252 towards the porous wick 262.
More specifically, the size of liquid conduits 266 are selected based on the rate
of aerosol precursor consumption during vaporisation. For example, the liquid conduits
266 are sized to allow a sufficient amount of aerosol precursor to flow towards and
replenish the wick, yet not so large as to cause excessive aerosol precursor to leak
into the aerosol generation chamber. The liquid conduits 266 are configured to have
a hydraulic diameter ranging from 0.01mm to 10mm or 0.01 mm to 5mm. Preferably, the
liquid conduits 266 are configured to have a hydraulic diameter in the range of 0.1mm
to 1mm.
[0136] The heating filament is electrically connected to electrical contacts 256 at the
base of the aerosol generation chamber 280, sealed to prevent air ingress or fluid
leakage. As shown in Figure 22, when the first end of the consumable 250 is received
into the main body 120, the electrical contacts 256 establish electrical communication
with corresponding electrical contacts of the main body 120, and thereby allow the
heater to be energised.
[0137] The vaporised aerosol precursor, or aerosol in the condensed form, may discharge
from the aerosol generation chamber 280 based on pressure difference between the aerosol
generation chamber 280 and the passages 270. Such pressure difference may arise form
i) an increased pressure in the aerosol generation chamber 280 during vaporisation
of aerosol form, and/or ii) a reduced pressure in the passage during a puff.
[0138] For example, when the heater is energised and forms a vapour, it expands in to the
stagnant cavity of the aerosol generation chamber 280 and thereby causes an increase
in internal pressure therein. The vaporised aerosol precursor may immediately begin
to cool and may form aerosol droplets. Such increase in internal pressure causes convection
inside the aerosol generation chamber which aids expulsing aerosol through the chamber
outlet 282 and into the passages 270.
[0139] In the illustrated third reference arrangement, the heater is positioned within the
stagnant cavity of the aerosol generation chamber 280, e.g. the heater is spaced from
the chamber outlet 282. Such arrangement may reduce or prevent the amount of air flow
entering the aerosol generation chamber, and therefore it may minimise the amount
of turbulence in the vicinity of the heater. Furthermore, such arrangement may increase
the residence time of vapour in the stagnant aerosol generation chamber 280, and thereby
may result in the formation of larger aerosol droplets. In some other variations of
the third reference arrangement, the heater may be positioned adjacent to the chamber
outlet and therefore that the path of vapour 414 from the heater to the chamber outlet
282 is shortened. This may allow vapour to be drawn into or entrained with the air
flow in a more efficient manner.
[0140] The junction inlet at each of the junctions 290 opens in a direction orthogonal or
non-parallel to the air flow. That is, the junction inlet each opens at a sidewall
of the respective passages 270. This allows the vapour and/or aerosol from the aerosol
generation chamber 280 to entrain into the air flow at an angle, and thus improving
localised mixing of the different streams, as well as encouraging aerosol formation.
The aerosol may be fully formed in the air flow and be drawn out through the outlet
at the mouthpiece.
[0141] With the absence of, or much reduced, air flow in the aerosol generation chamber,
the aerosol as generated by the illustrated third reference arrangement has a median
droplet size dso of at least 1µm. More preferably, the aerosol as generated by the
illustrated third reference arrangement has a median droplet size dso of ranged between
2µm to 3µm.
[0142] Figure 23 shows a schematic cross sectional view through the aerosol generation chamber
(also disclosed herein as the vaporisation chamber) of the smoking substitute apparatus
110C. The smoking substitute apparatus 110C comprises a first air inlet 120C, a second
air inlet 122C and an outlet (not shown). The outlet is at an opposing side to the
first and second air inlets. The smoking substitute apparatus also comprises an occlusion
member 140C. The occlusion member 140C is arranged to either cover the second air
inlet 122C, as shown in Figure 23, which illustrates a first configuration of the
occlusion member, or leave the second air inlet uncovered, as shown in Figure 24,
which illustrates a second configuration of the occlusion member (the occlusion member
being omitted from this view). The smoking substitute apparatus further comprises
a first air inlet passage 124C extending from the first air inlet 120C, and a second
air inlet passage 126C extending from the second air inlet 122C. The first air inlet
passage 124C and the second air inlet passage 126C extend to at least partially bypass
aerosol generator chamber 130C which comprises an aerosol generator 132C. The aerosol
generator comprises a wick 162C and a heater 164C in the form of a metal coil wrapped
around the wick.
[0143] As will be understood from the preceding discussion, the embodiment shown in Figure
23 is a type of stagnant chamber device, in which the air inlet does not directly
jet air onto the aerosol generator. This is found to be advantageous in the context
of the generation of relatively large aerosol particles.
[0144] In use, when the occlusion member is in a first configuration, as shown in Figure
23, air enters the second air inlet 120C and flows along an air flow path A only,
from the second air inlet 120C, through the second air inlet passage 124C and just
downstream of the aerosol generator chamber 130C. The air is guided along a first
part of the aerosol generator chamber by a guide 150C, which also serves as an electrical
contact to the heater, so that the incoming air is not directed at the aerosol generator.
As the air passes the end of the guide 150C, vapour and/or aerosol particles, generated
by the aerosol generator, are entrained in the air, to form an aerosol. The aerosol
moves towards the outlet, to be inhaled by the user.
[0145] In use, when the occlusion member is in a second configuration, as shown in Figure
24, air enters both the first air inlet 120C and the second air inlet 122C and flows
along air flow paths A and B. The air flows through the first air inlet passage 124C
and the second air inlet passage 126C. Downstream of the first air inlet passage 124C
and the second air inlet passage 126C, the air is separated from the aerosol generator
by guides 150C, 152C so that the air does not come into direct contact with the aerosol
generator 132C. Once the air flow paths A and B pass the guides 150C, the air flow
is directed to move substantially axially through the apparatus towards the outlet
(not shown). Aerosol particles are entrained in the air flow. The guide 152C for the
air flow path B is shown as being shorter than guide 150C for air flow path A. However,
this is in view of the guides' additional function as electrical contacts for heater
164. Each is sufficiently long to reduce the risk of air flow being directed at the
aerosol generator.
[0146] Figure 25 shows a schematic partial perspective view of the base of the smoking substitute
apparatus of Figure 23 when the occlusion member 140C is in the first configuration
(also known as a 'closed position'), in which the second air inlet is covered.
[0147] Figure 26 shows a schematic partial perspective view of the base of the smoking substitute
apparatus of Figure 23 when the occlusion member 140Cis in the second configuration
(also known as an 'open position'), in which the second air inlet 122C is uncovered.
[0148] In the first configuration, shown in Figure 25, the occlusion member 140C lies flat
across a base 270C of the smoking substitute apparatus to cover the second air inlet
(hidden from view and therefore not shown). In the second configuration, shown in
Figure 26, the occlusion member 140C is curved in shape and provides access for air
to enter the second air inlet 122C. The occlusion member 140C in Figures 25 and 26
is in the shape of a plate.
[0149] Figure 27 is a perspective side view of a smoking substitute system according to
an embodiment of the invention when the smoking substitute apparatus 110C is in a
first engagement arrangement with the main body 310C. The smoking substitute system
presents two air inlets (only one shown at 320C) and a mouthpiece 360C for a user
to inhale the aerosol. The smoking substitute apparatus 110C comprises bar 330C configured
to slide into a corresponding slot formed in the main body 310C, permitting easy location
and a positive engagement between the smoking substitute apparatus and the main body.
[0150] A first engagement arrangement is selected by the user when the exterior casings
of smoking substitute apparatus 110C and the main body 310C are fully engaged, as
shown in Figure 27. In the first configuration, the occlusion member is in a first
configuration, shown in Figures 23 and 25. In this engagement position, the second
air inlet 122C is covered and so air is not permitted to travel along air flow path
B.
[0151] A second engagement arrangement is selected by the user when the exterior casings
of the smoking substitute apparatus 110C and the main body 310C are partially separated,
as shown in Figure 28. In this engagement arrangement, the occlusion member is in
a second configuration, shown in Figures 24 and 26, and the second air inlet 122C
is uncovered and so air is permitted to travel along air flow path A and air flow
path B. In order to get the smoking substitute apparatus and main body into the second
engagement arrangement from the first engagement arrangement, a user pulls the exterior
casing of the smoking substitute apparatus 110C away from the main body 310C. When
the smoking apparatus 110C and the main body 310C are partially separated, a gap 350C
forms between the casing of the smoking apparatus and the casing of the main body,
and the occlusion member, which comprises a resilient material, is released, such
that it uncovers the second air inlet, as shown in Figures 24 and 26.
[0152] Figure 29 shows an enlarged schematic perspective cross sectional view taken parallel
to the principal axis of the wick and parallel to the principal axis of the apparatus,
showing interior features of the smoking substitute apparatus and the main body when
the occlusion member is in the second configuration. The dashed line in Figure 29
denotes a separation line between the substitute smoking apparatus and the main body.
When the substitute smoking apparatus and main body are engaged, the occlusion member
140C can be moved from a first configuration to a second configuration, and vice versa,
by the action of a user pushing or pulling the smoking substitute apparatus towards
or away from the main body. Pins 420C connect the battery (not shown) in the main
body, with the aerosol generator in the smoking substitute apparatus, to provide power
to the aerosol generator.
[0153] In Figure 30, the occlusion member 140C is in the first configuration, and is lying
flat against the base 270C of the smoking substitute apparatus. The occlusion member
is forced into the first configuration by a fixed protrusion 430C in the interior
casing of the main body. When the user pushes the smoking substitute apparatus towards
the main body, the occlusion member becomes compressed against the protrusion 430C
in the main body, which causes the occlusion member to flatten and cover the second
air inlet.
[0154] In Figure 29, the occlusion member 140C is curved in shape, and allows air to enter
the second air inlet. When the user pulls the exterior casing of smoking substitute
apparatus 110C away from the exterior casing of the main body at least a minimum configuration
distance, the protrusion 430C in the interior casing of the main body no longer compresses
the occlusion member 140C. Because the occlusion member 140C is made of a resilient
material, it returns to its original shape, which is a curved shape, after being compressed.
The occlusion member is now in the second configuration.
[0155] There now follows a disclosure of certain experimental work undertaken to determine
the effects of certain conditions in the smoking substitute apparatus on the particle
size of the generated aerosol.
[0156] The experimental results reported here are relevant to the embodiments disclosed
above in view of their demonstration of the control over particle size based on control
of the conditions at the wick. In particular, the embodiments disclosed above have
an effect on the air flow conditions and/or temperature in the vaporisation chamber,
in view of the effect of the occlusion member on occluding one of the air inlets and/or
the provision of bypass airflow.
1. Introduction
[0157] Aerosol droplet size is a considered to be an important characteristic for smoking
substitution devices. Droplets in the range of 2-5 µm are preferred in order to achieve
improved nicotine delivery efficiency and to minimise the hazard of second-hand smoking.
However, at the time of writing (September 2019), commercial EVP devices typically
deliver aerosols with droplet size averaged around 0.5 µm, and to the knowledge of
the inventors not a single commercially available device can deliver an aerosol with
an average particle size exceeding 1 µm.
[0158] The present inventors speculate, without themselves wishing to be bound by theory,
that there has to date been a lack of understanding in the mechanisms of e-liquid
evaporation, nucleation and droplet growth in the context of aerosol generation in
smoking substitute devices. The present inventors have therefore studied these issues
in order to provide insight into mechanisms for the generation of aerosols with larger
particles. The present inventors have carried out experimental and modelling work
alongside theoretical investigations, leading to significant achievements as now reported.
[0159] This disclosure considers the roles of air velocity, air turbulence and vapour cooling
rate in affecting aerosol particle size.
2. Experiments
[0160] In this work, a Malvern PANalytical Spraytec laser diffraction system was employed
for the particle size measurement. In order to limit the number of variables, the
same coil and wick (1.5 ohms Ni-Cr coil, 1.8 mm Y07 cotton wick), the same e-liquid
(1.6% freebase nicotine, 65:35 propylene glycol (PG)/vegetable glycerine (VG) ratio,
no added flavour) and the same input power (10W) were used in all experiments. Y07
represents the grade of cotton wick, meaning that the cotton has a linear density
of 0.7 grams per meter.
[0161] Particle sizes were measured in accordance with ISO 13320:2009(E), which is an international
standard on laser diffraction methods for particle size analysis. This is particularly
well suited to aerosols, because there is an assumption in this standard that the
particles are spherical (which is a good assumption for liquid-based aerosols). The
standard is stated to be suitable for particle sizes in the range 0.1 micron to 3
mm.
[0162] The results presented here concentrate on the volume-based median particle size Dv50.
This is to be taken to be the same as the parameter dso used above.
2.1. Rectangular tube testing
[0163] The work reported here based on the inventors' insight that aerosol particle size
might be related to: 1) air velocity; 2) flow rate; and 3) Reynolds number. In a given
EVP device, these three parameters are interlinked to each other, making it difficult
to draw conclusions on the roles of each individual factor. In order to decouple these
factors, experiments were carried out using a set of rectangular tubes having different
dimensions. These were manufactured by 3D printing. The rectangular tubes were 3D
printed in an MJP 2500 3D printer. Figure 1 illustrates the set of rectangular tubes.
Each tube has the same depth and length but different width. Each tube has an integral
end plate in order to provide a seal against air flow outside the tube. Each tube
also has holes formed in opposing side walls in order to accommodate a wick.
[0164] Figure 2 shows a schematic perspective longitudinal cross sectional view of an example
rectangular tube 1170 with a wick 1162 and heater coil 1164 installed. The location
of the wick is about half way along the length of the tube. This is intended to allow
the flow of air along the tube to settle before reaching the wick.
[0165] Figure 3 shows a schematic transverse cross sectional view an example rectangular
tube 1170 with a wick 1162 and heater coil 1164 installed. In this example, the internal
width of the tube is 12 mm The rectangular tubes were manufactured to have same internal
depth of 6 mm in order to accommodate the standardized coil and wick, however the
tube internal width varied from 4.5 mm to 50 mm. In this disclosure, the "tube size"
is referred to as the internal width of rectangular tubes.
[0166] The rectangular tubes with different dimensions were used to generate aerosols that
were tested for particle size in a Malvern PANalytical Spraytec laser diffraction
system. An external digital power supply was dialled to 2.6A constant current to supply
10W power to the heater coil in all experiments. Between two runs, the wick was saturated
manually by applying one drop of e-liquid on each side of the wick.
[0167] Three groups of experiments were carried out in this study:
- 1. 1.3 Ipm (litres per minute, L min-1 or LPM) constant flow rate on different size tubes
- 2. 2.0 Ipm constant flow rate on different size tubes
- 3. 1 m/s constant air velocity on 3 tubes: i) 5mm tube at 1.4 Ipm flow rate; ii) 8mm
tube at 2.8 Ipm flow rate; and iii) 20mm tube at 8.6 Ipm flow rate.
[0168] Table 1 shows a list of experiments in this study. The values in "calculated air
velocity" column were obtained by simply dividing the flow rate by the intersection
area at the centre plane of wick. Reynolds numbers (Re) were calculated through the
following equation:

where:
ρ is the density of air (1.225 kg/m
3);
v is the calculated air velocity in table 1;
µ is the viscosity of air (1.48 × 10
-5 m
2/s);
L is the characteristic length calculated by:

where: P is the perimeter of the flow path's intersection, and A is the area of the
flow path's intersection.
Table 1. List of experiments in the rectangular tube study
| |
Tube size [mm] |
Flow rate [Ipm] |
Reynolds number |
Calculated air velocity [m/s] |
| 1.3 Ipm constant flow rate |
4.5 |
1.3 |
153 |
1.17 |
| 6 |
1.3 |
142 |
0.71 |
| 7 |
1.3 |
136 |
0.56 |
| 8 |
1.3 |
130 |
0.47 |
| 10 |
1.3 |
120 |
0.35 |
| 12 |
1.3 |
111 |
0.28 |
| 20 |
1.3 |
86 |
0.15 |
| 50 |
1.3 |
47 |
0.06 |
| 2.0 lpm constant flow rate |
4.5 |
2.0 |
236 |
1.81 |
| 5 |
2.0 |
230 |
1.48 |
| 6 |
2.0 |
219 |
1.09 |
| 8 |
2.0 |
200 |
0.72 |
| 12 |
2.0 |
171 |
0.42 |
| 20 |
2.0 |
132 |
0.23 |
| 50 |
2.0 |
72 |
0.09 |
| 1.0 m/s constant air velocity |
5.0 |
1.4 |
155 |
1.00 |
| 8 |
2.8 |
279 |
1.00 |
| 20 |
8.6 |
566 |
1.00 |
[0169] Five repetition runs were carried out for each tube size and flow rate combination.
Between adjacent runs there were at least 5 minutes wait time for the Spraytec system
to be purged. In each run, real time particle size distributions were measured in
the Spraytec laser diffraction system at a sampling rate of 2500 per second, the volume
distribution median (Dv50) was averaged over a puff duration of 4 seconds. Measurement
results were averaged and the standard deviations were calculated to indicate errors
as shown in section 4 below.
2.2. Turbulence tube testing
[0170] The Reynolds numbers in Table 1 are all well below 1000, therefore, it is considered
fair to assume all the experiments in section 2.1 would be under conditions of laminar
flow. Further experiments were carried out and reported in this section to investigate
the role of turbulence.
[0171] Turbulence intensity was introduced as a quantitative parameter to assess the level
of turbulence. The definition and simulation of turbulence intensity is discussed
below (see section 3.2).
[0172] Different device designs were considered in order to introduce turbulence. In the
experiments reported here, jetting panels were added in the existing 12mm rectangular
tubes upstream of the wick. This approach enables direct comparison between different
devices as they all have highly similar geometry, with turbulence intensity being
the only variable.
[0173] Figures 4A-4D show air flow streamlines in the four devices used in this turbulence
study. Figure 4A is a standard 12mm rectangular tube with wick and coil installed
as explained in the previous section, with no jetting panel. Figure 4B has a jetting
panel located 10mm below (upstream from) the wick. Figure 4C has the same jetting
panel 5mm below the wick. Figure 4D has the same jetting panel 2.5mm below the wick.
As can be seen from Figures 4B-4D, the jetting panel has an arrangement of apertures
shaped and directed in order to promote jetting from the downstream face of the panel
and therefore to promote turbulent flow. Accordingly, the jetting panel can introduce
turbulence downstream, and the panel causes higher level of turbulence near the wick
when it is positioned closer to the wick. As shown in Figures 4A-4D, the four geometries
gave turbulence intensities of 0.55%, 0.77%, 1.06% and 1.34%, respectively, with Figure
4A being the least turbulent, and Figure 4D being the most turbulent.
[0174] For each of Figures 4A-4D, there are shown three modelling images. The image on the
left shows the original image (colour in the original), the central image shows a
greyscale version of the image and the right hand image shows a black and white version
of the image. As will be appreciated, each version of the image highlights slightly
different features of the flow. Together, they give a reasonable picture of the flow
conditions at the wick.
[0175] These four devices were operated to generate aerosols following the procedure explained
above (section 2.1) using a flow rate of 1.3 Ipm and the generated aerosols were tested
for particle size in the Spraytec laser diffraction system.
2.3. High temperature testing
[0176] This experiment aimed to investigate the influence of inflow air temperature on aerosol
particle size, in order to investigate the effect of vapour cooling rate on aerosol
generation.
[0177] The experimental set up is shown in Figure 5. The testing used a Carbolite Gero EHA
12300B tube furnace 3210 with a quartz tube 3220 to heat up the air. Hot air in the
tube furnace was then led into a transparent housing 3158 that contains the EVP device
3150 to be tested. A thermocouple meter 3410 was used to assess the temperature of
the air pulled into the EVP device. Once the EVP device was activated, the aerosol
was pulled into the Spraytec laser diffraction system 3310 via a silicone connector
3320 for particle size measurement.
[0178] Three smoking substitute apparatuses (referred to as "pods") were tested in the study:
pod 1 is the commercially available "myblu optimised" pod (Figure 6); pod 2 is a pod
featuring an extended inflow path upstream of the wick (Figure 7); and pod 3 is pod
with the wick located in a stagnant vaporisation chamber and the inlet air bypassing
the vaporisation chamber but entraining the vapour from an outlet of the vaporisation
chamber (Figures 8A and 8B).
[0179] Pod 1, shown in longitudinal cross sectional view (in the width plane) in Figure
6, has a main housing that defines a tank 160x holding an e-liquid aerosol precursor.
Mouthpiece 154x is formed at the upper part of the pod. Electrical contacts 156x are
formed at the lower end of the pod. Wick 162x is held in a vaporisation chamber. The
air flow direction is shown using arrows.
[0180] Pod 2, shown in longitudinal cross sectional view (in the width plane) in Figure
7, has a main housing that defines a tank 160y holding an e-liquid aerosol precursor.
Mouthpiece 154y is formed at the upper part of the pod. Electrical contacts 156y are
formed at the lower end of the pod. Wick 162y is held in a vaporisation chamber. The
air flow direction is shown using arrows. Pod 2 has an extended inflow path (plenum
chamber 157y) with a flow conditioning element 159y, configured to promote reduced
turbulence at the wick 162y.
[0181] Figure 8A shows a schematic longitudinal cross sectional view of pod 3. Figure 8B
shows a schematic longitudinal cross sectional view of the same pod 3 in a direction
orthogonal to the view taken in Figure 8A. Pod 3 has a main housing that defines a
tank 160z holding an e-liquid aerosol precursor. Mouthpiece 154z is formed at the
upper part of the pod. Electrical contacts 156z are formed at the lower end of the
pod. Wick 162z is held in a vaporisation chamber. The air flow direction is shown
using arrows. Pod 3 uses a stagnant vaporiser chamber, with the air inlets bypassing
the wick and picking up the vapour/aerosol downstream of the wick.
[0182] All three pods were filled with the same e-liquid (1.6% freebase nicotine, 65:35
PG/VG ratio, no added flavour). Three experiments were carried out for each pod: 1)
standard measurement in ambient temperature; 2) only the inlet air was heated to 50
°C; and 3) both the inlet air and the pods were heated to 50 °C. Five repetition runs
were carried out for each experiment and the Dv50 results were taken and averaged.
3. Modelling work
[0183] In this study, modelling work was performed using COMSOL Multiphysics 5.4, engaged
physics include: 1) laminar single-phase flow; 2) turbulent single-phase flow; 3)
laminar two-phase flow; 4) heat transfer in fluids; and (5) particle tracing. Data
analysis and data visualisation were mostly completed in MATLAB R2019a.
3.1. Velocity modelling
[0184] Air velocity in the vicinity of the wick is believed to play an important role in
affecting particle size. In section 2.1, the air velocity was calculated by dividing
the flow rate by the intersection area, which is referred to as "calculated velocity"
in this work. This involves a very crude simplification that assumes velocity distribution
to be homogeneous across the intersection area.
[0185] In order to increase reliability of the work, computational fluid dynamics (CFD)
modelling was performed to obtain more accurate velocity values:
- 1) The average velocity in the vicinity of the wick (defined as a volume from the
wick surface to 1mm away from the wick surface)
- 2) The maximum velocity in the vicinity of the wick (defined as a volume from the
wick surface to 1mm away from the wick surface)
Table 2. Average and maximum velocity in the vicinity of wick surface obtained from
CFD modelling
| |
Tube size [mm] |
Flow rate [lpm] |
Calculated velocity* [m/s] |
Average velocity** [m/s] |
Maximum Velocity** [m/s] |
| 1.3 Ipm constant flow rate |
4.5 |
1.3 |
1.17 |
0.99 |
1.80 |
| 6 |
1.3 |
0.71 |
0.66 |
1.22 |
| 7 |
1.3 |
0.56 |
0.54 |
1.01 |
| 8 |
1.3 |
0.47 |
0.46 |
0.86 |
| 10 |
1.3 |
0.35 |
0.35 |
0.66 |
| 12 |
1.3 |
0.28 |
0.27 |
0.54 |
| 20 |
1.3 |
0.15 |
0.15 |
0.32 |
| 50 |
1.3 |
0.06 |
0.05 |
0.12 |
| 2.0 Ipm constant flow rate |
4.5 |
2.0 |
1.81 |
1.52 |
2.73 |
| 5 |
2.0 |
1.48 |
1.31 |
2.39 |
| 6 |
2.0 |
1.09 |
1.02 |
1.87 |
| 8 |
2.0 |
0.72 |
0.71 |
1.31 |
| 12 |
2.0 |
0.42 |
0.44 |
0.83 |
| 20 |
2.0 |
0.23 |
0.24 |
0.49 |
| 50 |
2.0 |
0.09 |
0.08 |
0.19 |
| * Calculated by dividing flow rate with intersection area |
| ** Obtained from CFD modelling |
[0186] The CFD model uses a laminar single-phase flow setup. For each experiment, the outlet
was configured to a corresponding flowrate, the inlet was configured to be pressure-controlled,
the wall conditions were set as "no slip". A 1 mm wide ring-shaped domain (wick vicinity)
was created around the wick surface, and domain probes were implemented to assess
the average and maximum magnitudes of velocity in this ring-shaped wick vicinity domain.
[0187] The CFD model outputs the average velocity and maximum velocity in the vicinity of
the wick for each set of experiments carried out in section 2.1. The outcomes are
reported in Table 2.
3.2. Turbulence modelling
[0188] Turbulence intensity (
I) is a quantitative value that represents the level of turbulence in a fluid flow
system. It is defined as the ratio between the root-mean-square of velocity fluctuations,
u', and the Reynolds-averaged mean flow velocity,

where
ux,
uy and
uz are the x-, y- and z-components of the velocity vector,
ux,
uy, and
uz represent the average velocities along three directions.
[0189] Higher turbulence intensity values represent higher levels of turbulence. As a rule
of thumb, turbulence intensity below 1% represents a low-turbulence case, turbulence
intensity between 1% and 5% represents a medium-turbulence case, and turbulence intensity
above 5% represents a high-turbulence case.
[0190] In this study, turbulence intensity was obtained from CFD simulation using turbulent
single-phase setup in COMSOL Multiphysics. For each of the four experiments explained
in section 2.2, the outlet was set to 1.3 Ipm, the inlet was set to be pressure-controlled,
and all wall conditions were set to be "no slip".
[0191] Turbulence intensity was assessed within the volume up to 1 mm away from the wick
surface (defined as the wick vicinity domain). For the four experiments explained
in section 2.2, the turbulence intensities are 0.55%, 0.77%, 1.06% and 1.34%, respectively,
as also shown in Figures 4A-4D.
3.3. Cooling rate modelling
[0192] The cooling rate modelling involves three coupling models in COMSOL Multiphysics:
1) laminar two-phase flow; 2) heat transfer in fluids, and 3) particle tracing. The
model is setup in three steps:
- 1) Set up two phase flow model
Laminar mixture flow physics was selected in this study. The outlet was configured
in the same way as in section 3.1. However, this model includes two fluid phases released
from two separate inlets: the first one is the vapour released from wick surface,
at an initial velocity of 2.84 cm/s (calculated based on 5 mg total particulate mass
over 3 seconds puff duration) with initial velocity direction normal to the wick surface;
the second inlet is air influx from the base of tube, the rate of which is pressure-controlled.
- 2) Set up two-way coupling with heat transfer physics
The inflow and outflow settings in heat transfer physics was configured in the same
way as in the two-phase flow model. The air inflow was set to 25 °C, and the vapour
inflow was set to 209 °C (boiling temperature of the e-liquid formulation). In the
end, the heat transfer physics is configured to be two-way coupled with the laminar
mixture flow physics. The above model reaches steady state after approximately 0.2
second with a step size of 0.001 second.
- 3) Set up particle tracing
A wave of 2000 particles were release from wick surface at t = 0.3 second after the
two-phase flow and heat transfer model has stabilised. The particle tracing physics
has one-way coupling with the previous model, which means the fluid flow exerts dragging
force on the particles, whereas the particles do not exert counterforce on the fluid
flow. Therefore, the particles function as moving probes to output vapour temperature
at each timestep.
[0193] The model outputs average vapour temperature at each time steps. A MATLAB script
was then created to find the time step when the vapour cools to a target temperature
(50°C or 75°C), based on which the vapour cooling rates were obtained (Table 3).
Table 3. Average vapour cooling rate obtained from Multiphysics modelling
| |
Tube size [mm] |
Flow rate [lpm] |
Cooling rate to 50°C [°C/ms] |
Cooling rate to 75°C [°C/ms] |
| 1.3 lpm constant flow rate |
4.5 |
1.3 |
11.4 |
44.7 |
| 6 |
1.3 |
5.48 |
14.9 |
| 7 |
1.3 |
3.46 |
7.88 |
| 8 |
1.3 |
2.24 |
5.15 |
| 10 |
1.3 |
1.31 |
2.85 |
| 12 |
1.3 |
0.841 |
1.81 |
| 20 |
1.3 |
0* |
0.536 |
| 50 |
1.3 |
0 |
0 |
| 2.0 Ipm constant flow rate |
4.5 |
2.0 |
19.9 |
670 |
| 5 |
2.0 |
13.3 |
67 |
| 6 |
2.0 |
8.83 |
26.8 |
| 8 |
2.0 |
3.61 |
8.93 |
| 12 |
2.0 |
1.45 |
3.19 |
| 20 |
2.0 |
0.395 |
0.761 |
| 50 |
2.0 |
0 |
0 |
| * Zero cooling rate when the average vapour temperature is still above target temperature
after 0.5 second |
4. Results and discussions
[0194] Particle size measurement results for the rectangular tube testing are shown in Table
4. For every tube size and flow rate combination, five repetition runs were carried
out in the Spraytec laser diffraction system. The Dv50 values from five repetition
runs were averaged, and the standard deviations were calculated to indicate errors,
as shown in Table 4.
[0195] In this section, the roles of different factors affecting aerosol particle size will
be discussed based on experimental and modelling results.
Table 4. Particle size measurement results for the rectangular tube testing
| |
Tube size [mm] |
Flow rate [lpm] |
Dv50 average [µm] |
Dv50 standard deviation [µm] |
| 1.3 Ipm constant flow rate |
4.5 |
1.3 |
0.971 |
0.125 |
| 6 |
1.3 |
1.697 |
0.341 |
| 7 |
1.3 |
2.570 |
0.237 |
| 8 |
1.3 |
2.705 |
0.207 |
| 10 |
1.3 |
2.783 |
0.184 |
| 12 |
1.3 |
3.051 |
0.325 |
| 20 |
1.3 |
3.116 |
0.354 |
| 50 |
1.3 |
3.161 |
0.157 |
| 2.0 Ipm constant flow rate |
4.5 |
2.0 |
0.568 |
0.039 |
| 5 |
2.0 |
0.967 |
0.315 |
| 6 |
2.0 |
1.541 |
0.272 |
| 8 |
2.0 |
1.646 |
0.363 |
| 12 |
2.0 |
3.062 |
0.153 |
| 20 |
2.0 |
3.566 |
0.260 |
| 50 |
2.0 |
3.082 |
0.440 |
| 1.0 m/s constant air velocity |
5.0 |
1.4 |
1.302 |
0.187 |
| 8 |
2.8 |
1.303 |
0.468 |
| 20 |
8.6 |
1.463 |
0.413 |
4.1. Decouple the factors affecting particle size
[0196] The particle size (Dv50) experimental results are plotted against calculated air
velocity in Figure 9. The graph shows a strong correlation between particle size and
air velocity.
[0197] Different size tubes were tested at two flow rates: 1.3 Ipm and 2.0 Ipm. Both groups
of data show the same trend that slower air velocity leads to larger particle size.
The conclusion was made more convincing by the fact that these two groups of data
overlap well in Figure 9: for example, the 6mm tube delivered an average Dv50 of 1.697
µm when tested at 1.3 Ipm flow rate, and the 8mm tube delivered a highly similar average
Dv50 of 1.646 µm when tested at 2.0 Ipm flow rate, as they have similar air velocity
of 0.71 and 0.72 m/s, respectively.
[0198] In addition, Figure 10 shows the results of three experiments with highly different
setup arrangements: 1) 5mm tube measured at 1.4 Ipm flow rate with Reynolds number
of 155; 2) 8mm tube measured at 2.8 Ipm flow rate with Reynolds number of 279; and
3) 20mm tube measured at 8.6 Ipm flow rate with Reynolds number of 566. It is relevant
that these setup arrangements have one similarity: the air velocities are all calculated
to be 1 m/s. Figure 10 shows that, although these three sets of experiments have different
tube sizes, flow rates and Reynolds numbers, they all delivered similar particle sizes,
as the air velocity was kept constant. These three data points were also plotted out
in Figure 9 (1 m/s data with star marks) and they tie in nicely into particle size-air
velocity trendline.
[0199] The above results lead to a strong conclusion that air velocity is an important factor
affecting the particle size of EVP devices. Relatively large particles are generated
when the air travels with slower velocity around the wick. It can also be concluded
that flow rate, tube size and Reynolds number are not necessarily independently relevant
to particle size, providing the air velocity is controlled in the vicinity of the
wick.
4.2. Further consideration of velocity
[0200] In Figure 9 the "calculated velocity" was obtained by dividing the flow rate by the
intersection area, which is a crude simplification that assumes a uniform velocity
field. In order to increase reliability of the work, CFD modelling has been performed
to assess the average and maximum velocities in the vicinity of the wick. In this
study, the "vicinity" was defined as a volume from the wick surface up to 1 mm away
from the wick surface.
[0201] The particle size measurement data were plotted against the average velocity (Figure
11) and maximum velocity (Figure 12) in the vicinity of the wick, as obtained from
CFD modelling.
[0202] The data in these two graphs indicates that in order to obtain an aerosol with Dv50
larger than 1 µm, the average velocity should be less than or equal to 1.2 m/s in
the vicinity of the wick and the maximum velocity should be less than or equal to
2.0 m/s in the vicinity of the wick.
[0203] Furthermore, in order to obtain an aerosol with Dv50 of 2 µm or larger, the average
velocity should be less than or equal to 0.6 m/s in the vicinity of the wick and the
maximum velocity should be less than or equal to 1.2 m/s in the vicinity of the wick.
[0204] It is considered that typical commercial EVP devices deliver aerosols with Dv50 around
0.5 µm, and there is no commercially available device that can deliver aerosol with
Dv50 exceeding 1 µm. It is considered that typical commercial EVP devices have average
velocity of 1.5-2.0 m/s in the vicinity of the wick.
4.3. The role of turbulence
[0205] The role of turbulence has been investigated in terms of turbulence intensity, which
is a quantitative characteristic that indicates the level of turbulence. In this work,
four tubes of different turbulence intensities were used to general aerosols which
were measured in the Spraytec laser diffraction system. The particle size (Dv50) experimental
results are plotted against turbulence intensity in Figure 13.
[0206] The graph suggests a correlation between particle size and turbulence intensity,
that lower turbulence intensity is beneficial for obtaining larger particle size.
It is noted that when turbulence intensity is above 1% (medium-turbulence case), there
are relatively large measurement fluctuations. In Figure 13, the tube with a jetting
panel 10mm below the wick has the largest error bar, because air jets become unpredictable
near the wick after traveling through a long distance.
[0207] The results clearly indicate that laminar air flow is favourable for the generation
of aerosols with larger particles, and that the generation of large particle sizes
is jeopardised by introducing turbulence. In Figure 13, the 12mm standard rectangular
tube (without jetting panel) delivers above 3 µm particle size (Dv50). The particle
size values reduced by at least a half when jetting panels were added to introduce
turbulence.
4.4. Vapour cooling rate
[0208] Figure 14 shows the high temperature testing results. Larger particle sizes were
observed from all 3 pods when the temperature of inlet air increased from room temperature
(23°C) to 50 °C. When the pods were heated as well, two of the three pods saw even
larger particle size measurement results, while pod 2 was unable to be measured due
to significant amount of leakage.
[0209] Without wishing to be bound by theory, the results are in line with the inventors'
insight that control over the vapour cooling rate provides an important degree of
control over the particle size of the aerosol. As reported above, the use of a slow
air velocity can have the result of the formation of an aerosol with large Dv50. It
is considered that this is due to slower air velocity allowing a slower cooling rate
of the vapour. Another conclusion related to laminar flow can also be explained by
a cooling rate theory: laminar flow allows slow and gradual mixing between cold air
and hot vapour, which means the vapour can cool down in slower rate when the airflow
is laminar, resulting in larger particle size.
[0210] The results in Figure 14 further validate this cooling rate theory: when the inlet
air has higher temperature, the temperature difference between hot vapour and cold
air becomes smaller, which allows the vapour to cool down at a slower rate, resulting
in larger particle size; when the pods were heated as well, this mechanism was exaggerated
even more, leading to an even slower cooling rate and an even larger particle size.
4.5. Further consideration of vapour cooling rate
[0211] In section 3.3, the vapour cooling rates for each tube size and flow rate combination
were obtained via multiphysics simulation. In Figure 15 and Figure 16, the particle
size measurement results were plotted against vapour cooling rate to 50°C and 75°C,
respectively.
[0212] The data in these graphs indicates that in order to obtain an aerosol with Dv50 larger
than 1 µm, the apparatus should be operable to require more than 16 ms for the vapour
to cool to 50°C, or an equivalent (simplified to an assumed linear) cooling rate being
slower than 10 °C/ms. From an alternative viewpoint, in order to obtain an aerosol
with Dv50 larger than 1 µm, the apparatus should be operable to require more than
4.5 ms for the vapour to cool to 75°C, or an equivalent (simplified to an assumed
linear) cooling rate slower than 30 °C/ms.
[0213] Furthermore, in order to obtain an aerosol with Dv50 of 2 µm or larger, the apparatus
should be operable to require more than 32 ms for the vapour to cool to 50°C, or an
equivalent (simplified to an assumed linear) cooling rate being slower than 5 °C/ms.
From an alternative viewpoint, in order to obtain an aerosol with Dv50 of 2 µm or
larger, the apparatus should be operable to require more than 13 ms for the vapour
to cool to 75°C, or an equivalent (simplified to an assumed linear) cooling rate slower
than 10 °C/ms.
5. Conclusions of particle size experimental work
[0214] In this work, particle size (Dv50) of aerosols generated in a set of rectangular
tubes was studied in order to decouple different factors (flow rate, air velocity,
Reynolds number, tube size) affecting aerosol particle size. It is considered that
air velocity is an important factor affecting particle size - slower air velocity
leads to larger particle size. When air velocity was kept constant, the other factors
(flow rate, Reynolds number, tube size) has low influence on particle size.
[0215] The role of turbulence was also investigated. It is considered that laminar air flow
favours generation of large particles, and introducing turbulence deteriorates (reduces)
the particle size.
[0216] Modelling methods were used to simulate the average air velocity, the maximum air
velocity, and the turbulence intensity in the vicinity of the wick. A COMSOL model
with three coupled physics has also been developed to obtain the vapour cooling rate.
[0217] All experimental and modelling results support a cooling rate theory that slower
vapour cooling rate is a significant factor in ensuring larger particle size. Slower
air velocity, laminar air flow and higher inlet air temperature lead to larger particle
size, because they all allow vapour to cool down at slower rates.
[0218] The features disclosed in the foregoing description, or in the following claims,
or in the accompanying drawings, expressed in their specific forms or in terms of
a means for performing the disclosed function, or a method or process for obtaining
the disclosed results, as appropriate, may, separately, or in any combination of such
features, be utilised for realising the invention in diverse forms thereof.
[0219] While the invention has been described in conjunction with the exemplary embodiments
described above, many equivalent modifications and variations will be apparent to
those skilled in the art when given this disclosure. Accordingly, the exemplary embodiments
of the invention set forth above are considered to be illustrative and not limiting.
Various changes to the described embodiments may be made without departing from the
spirit and scope of the invention.
[0220] For the avoidance of any doubt, any theoretical explanations provided herein are
provided for the purposes of improving the understanding of a reader. The inventors
do not wish to be bound by any of these theoretical explanations.
[0221] Any section headings used herein are for organizational purposes only and are not
to be construed as limiting the subject matter described.
[0222] Throughout this specification, including the claims which follow, unless the context
requires otherwise, the words "have", "comprise", and "include", and variations such
as "having", "comprises", "comprising", and "including" will be understood to imply
the inclusion of a stated integer or step or group of integers or steps but not the
exclusion of any other integer or step or group of integers or steps.
[0223] It must be noted that, as used in the specification and the appended claims, the
singular forms "a," "an," and "the" include plural referents unless the context clearly
dictates otherwise. Ranges may be expressed herein as from "about" one particular
value, and/or to "about" another particular value. When such a range is expressed,
another embodiment includes from the one particular value and/or to the other particular
value. Similarly, when values are expressed as approximations, by the use of the antecedent
"about," it will be understood that the particular value forms another embodiment.
The term "about" in relation to a numerical value is optional and means, for example,
+/- 10%.
[0224] The words "preferred" and "preferably" are used herein refer to embodiments of the
invention that may provide certain benefits under some circumstances. It is to be
appreciated, however, that other embodiments may also be preferred under the same
or different circumstances. The recitation of one or more preferred embodiments therefore
does not mean or imply that other embodiments are not useful, and is not intended
to exclude other embodiments from the scope of the disclosure, or from the scope of
the claims.