Prior art
[0001] Lighting systems have evolved in the past years with increasingly efficient solutions,
which first involved the simple evolution of the light source from incandescent filament
to mercury vapors, and then metal halide lamps.
[0002] These last sources have a high efficiency but show drawbacks in terms of minimum
available power, directionality and control. The efficiency of a vapor or metal halide
source grows with the power of the source and this led to light assemblies with large
dimensions and diffusing systems more and more complex, introducing a limit to the
applications of these systems. They are in practice applicable only to large areas
and they are not suitable for street lighting or lighting of a city centre, due to
loss of efficiency caused by distribution and lighting interference with home buildings.
[0003] Concentrated high efficiency and high power sources make necessary to distribute
the light with suitably shaped reflecting surfaces, which require multiple reflection
and penalize the efficiency of the lighting body. Moreover said surfaces require the
use of transmission angles to the output, such that the protection losses become relevant
for modern installations with sparse light posts.
[0004] The so optimized sources are suitable for operation at fixed point in terms both
thermal and of current/tension excitation. The variations which are artificially imposed,
made necessary by the norms, lead to deviation of behaviour that allow poor control
and affect the quality of the emission and life of the source.
[0005] Sources have been studied with high efficiency but low specific power and high directionality
such as LED sources and more recently the quartz metallic micro sources. Their application
allowed to distribute punctually and with defined direction the sources obtaining
a gain in efficiency and an improved quality of the light. A LED road lamp is described
for example in
EP 2 101 106.
[0006] Said sources together with directionality have a sharp controllability which is a
consequence of the physical principles underlying the emission of electrons and their
conversion by means of the converting means (phosphor, etc.) involved. Intensity and
fast response in status change allow to manage dimming by high frequency on-off techniques
allowing a regulation from 0% to 100% of the emission but maintaining quality of the
same.
[0007] These sources are based on new and fast developing technologies, allowing to pass
in two years from products with specific luminosity of 80-90 lumen per watt to commercially
available products of 130 lumen per watt and products under laboratory testing of
190 lumen per watt.
[0008] The accurate disposition of the leds is the first cause of saving, which is not dependent
on the source, that was possible after the market introduction of these new sources.
It has been addressed the need to orient light rays in a more efficient way in order
to fully exploit the increasing efficiency of the sources and to optimize the overall
cost of the lighting body (see
KR 20010069867 and
CA2411219).
[0009] The introduction of these light sources has been so fast that it was not possible
to provide adequate infrastructures and the culture of use and, despite the high performances,
the issue of control has been overlooked.
Summary of the invention
[0010] In this context, the disclosed method and the relative system have the advantage
of optimizing the energy saving, maintaining the light intensity adapted to the purpose,
as it is often required by norms.
[0011] According to the invention, the light emission of a lighting body comprising at least
two light sources is controlled by means of measuring and storing a set of chromatic
emissions, also named chromatic coordinates, made in at least one reference point.
According to different embodiments of the invention, said reference point may belong
or may not belong to the area which is lightened by the lighting body.
[0012] A first aspect of the invention consists in a method for controlling the light emission
of a lighting body having at least two light sources that can be controlled in intensity,
said method comprising the steps of:
- defining at least one reference point in a zone lightened by said lighting body,
- making a measure of the intensity of each component of a set of chromatic emissions
in said reference point, said measure being carried out with a natural or artificial
reference light and in a defined first time instant (t0),
- computing the difference of intensity between said chromatic emissions and computing
the measured absolute intensity, obtaining a set of parameters,
- storing said parameters in a suitable memory location of said lighting body,
- comparing said parameters with a measure of the chromatic emissions made in a generic
second time instant different from said first instant,
- regulating the intensity of the light sources of said lighting body in a way to bring
the intensity of the chromatic emissions to the values measured in said first time
instant or to a predetermined value.
[0013] A second aspect of the invention consists in a method for controlling the light emission
of a lighting body having at least two light sources that can be controlled in intensity,
said method comprising the steps of:
- defining at least a reference point in a zone which is not lightened by said lighting
body;
- making a measure of the intensity of each component of a set of chromatic emissions
in said reference point, said measure being carried out with a natural or artificial
reference light and in a defined first time instant,
- computing the difference of intensity between said chromatic emissions and computing
the measured absolute intensity, obtaining a set of parameters,
- storing said parameters in a suitable memory location of said lighting body,
- storing in said lighting body the intensity that must be given to the source as a
function of said differences,
- interpolating the intensity to be given to the light sources in a generic second time
instant as a function of said differences between said parameters.
[0014] It is an object of the invention also a lighting apparatus suitable to operate according
to the above described method. Preferably said apparatus comprises at least: a control
system adapted to control the light intensity of said at least two sources continuously
and independently; at least one microcontroller that manages said control system;
at least one sensor adapted to measure the intensity of a set of chromatic emissions
in at least one location, for example inside or outside the lightened area; at least
a data memory.
[0015] The above mentioned set of chromatic coordinates is for example represented by the
triad of emissions red, green and blue (RGB) at reference frequencies.
[0016] Preferably the invention applies to LED equipments. Hence, the above said light sources
are preferably LED diodes. A preferred application is the street lighting or public
lighting, but the invention is also applicable to interior lighting.
[0017] Further aspects of the invention are described in the dependent claims.
[0018] An advantage of the present invention is the possibility to use led of the same type,
differencing lighting behavior of the lamp in various zones thus having a product
which is a standard product but able to provide optimal efficiency also near internal
walls of a shed or the facade of a palace.
[0019] A further advantage of the present invention is to allow non-lightened zones such
as for example a private home window under a street lamp or a green area during night
time.
[0020] A further advantage of the proposed invention is to allow to pass to full power upon
receipt of an alarm signal issued from an exterior agent or optically produced in
the field of the luminosity sensor, restoring or increasing the local luminosity level
e.g. in case of an accident in the lightened zone.
[0021] The invention provides a system for acquisition and regulation of a light source,
for example a headlight or a street lamp, based on chromatic coordinates which are
acquired and stored, in a way to allow a correct regulation and control of the measured
and radiated light. The proposed method and the relative equipment are particularly
adapted to use in management of street lamps, relative to intensity and quality of
the light, as well as management of lighting devices for interiors and exteriors and
for urban architectural lighting. The application is particularly advantageous in
the management of the level of luminosity and energy required and may be addressed
to energy saving as well as to the aim of achieving a given lighting.
Description of a preferred embodiment
[0022] The proposed method is implemented by the physical system represented in Fig. 2.
A light device 50 lightens a lightened zone 190 and does not lighten a zone 191. A
set of chromatic coordinates is measured in at least one point 200 in said zone 190,
for example the values of the triad of radiations red, green and blue, at given reference
frequencies. Said measure is performed at a time t0 and the so measured set of chromatic
coordinates is stored in a suitable memory location of the device 50. The coordinates
measured at said instant t0 are depicted in the graph (t0) of Fig. 2.
[0023] Said triad of radiation red, green and blue (RGB) is part of the light ray sent in
the radiation which is schematized by the arrow line of Fig. 2 to at least one sensor
in the light device adapted to receive and decompose the light, so to allow to measure
the components of the triad.
[0024] As time passes, the lighting conditions and then the emitted radiation change, as
is depicted for example in graph (t1) of Fig. 2, registered by the sensor at time
t1 always in the reference light conditions. The light device thanks to its own means
which are described in the following regulates the level of its emission in order
to restore completely the sum of the intensities taken at time t1 and bring them back
to the same values of time t0 or to a predetermined value which is set in the lighting
device. Said value can be set depending on time or depending on an external input
such as a control center, a user remote control or automatic control system.
[0025] Said lighting device acts in a first case in autonomous way trying to lower the difference
between the value (R+G+B)
t0 and the value (R+G+B)
t1 by increase of the intensity of its emission. Said increase of intensity, as said
before, may be limited to a stored value (R+G+B)
max due to an external agent, see as example the condition depicted at time t2a were
the graph (t2a) represents the situation produced by this control algorithm intervened
at time t1.
[0026] Said lighting device acts in a second case in autonomous way to lower the differences
between the n-th components intensity ratio (R/G, B/G)
t0 and the value (R/G, B/G)
t1 increasing the intensity of its own light emission. This increment of light emission
could be, as mentioned above, cut at a stored level (R+G+B)
max depending on an external agent choice, see as example the condition at time t2b where
the graph (t2b) represents the situation produced by this algorithm at time t1.
[0027] In other words said lighting device in general is able to act autonomously to regulate
the intensity of light radiation according to an algorithm which is predetermined
but modifiable during time so to allow a lighting level in control points adapted
to the purpose defined by the external agent, setting the algorithm and defining limits.
[0028] If it is chosen to use more than a point, the lighting device can operate by summing
the homologous members of the radiation received by sensor (or sensors) from different
points, or exploiting a plurality of intensity control channels and acting on channels
that power light sources specifically directed to said point in order to obtain application
of said algorithms each for a different zone of the lightened area (190).
[0029] What has been described apply also independently or together to the radiation received
by said sensors from any non-lightened area 191 created by an object or by a free
surface. In this specific case there is no possibility for the sensor to check its
direct action and the lighting device according to the selected algorithm has a series
of internally stored intensities corresponding to the values of differences between
the reference and the measured that the lighting device execute in a continuous way.
[0030] Said lighting device is also equipped with a time signal internally generated by
an RTC (real clock timer) or universal timer or generated by an external time signal
received preferably, but without loss of generality, via radio. Said time signal may
be processed by the lighting device to obtain the maximum power output by an internal
memory device linked to the internally generated time scale.
[0031] A functional description of the light device which implements the described method
as represented in Fig. 1 is now given.
[0032] The lighting body has a structure (51) able to host and support the internal components,
composed of metal, plastic and any material adapted to the main purpose and able to
dissipate by convection or conduction the heat produced by the components.
[0033] Said lighting body holds a plurality (at least two) of light sources 100 which are
independently controlled by a control system 120 through connecting branches 110 obtained
in the structure or discretely made as wires according to per se known technique.
The arrangement of the leds in three-dimensional inclination in the space is advantageous
for the purpose of uniformity and efficiency of the emitted light radiation, and is
per se known art, in fact the product available on the market are uniforming their
disposition.
[0034] Said system for powering and regulating the sources 120 is controlled by on board
micro controller of the light device that executes the algorithms and the strategies
described in the method, and operates the accessory functions of measure and active
check of consumption, control of the system by means of check of temperature and magnetic
fields induced by operation.
[0035] A micro controller 130 receives the data of the chromatic set from at least one sensor
140 which may receive them (210) from different locations, indicated for example with
numerals 200 and 150, or from a single location. The microcontroller computes the
signal from said chromatic sensors 140 and save them in a stable and safe position
such as eeprom 160 or more eeproms in a suitable format to be used by the algorithms
as chromatic coordinates. Those memory locations or eeprom stores also the data necessary
for autonomous operation of the lighting body such as the tables of correspondence
between the measured intensity and the light radiation to emit, ratio between the
intensities of the set and power output, the maximum limit of light radiation to emit
as a function of the time scale.
[0036] The micro controller may generate autonomously a time scale but it is preferred to
use a dedicated and more precise RTC system (170) which feeds the clock to the micro
controller.
[0037] According to another of the preferred aspects of the invention, the sunlight is measured
at regular intervals, e.g. at 15'-45' intervals, obtaining a curve of sunlight intensity;
the maximum of said curve is identified with a parabola or other interpolation; said
maximum is given the meaning of midday and, as a consequence, the midnight is also
indentified. This process is carried out for every day of the year, with a possibility
of self-adaptation of the lighting body to the actual sunlight conditions, and with
a considerable energy saving compared to a conventional lighting system that is activated
at predetermined times.
[0038] Modifications to data, function parameters are made for example by means of a communication
device 180 integrated in the microcontroller or external as in the figure.
1. Method for controlling the light emission of a lighting body (50) having at least
two light sources that can be controlled in intensity, said method comprising the
steps of:
a) defining at least one reference point (200) in a zone (190) which is lightened
by said lighting body,
b) making a measure of the intensity of each component of a set of chromatic emissions
in said reference point, said measure being carried out with a natural or artificial
reference light and in a defined first time instant (t0),
c) computing the difference of intensity between said chromatic emissions and computing
the measured absolute intensity, obtaining a set of parameters,
d) storing said parameters in a suitable memory location of said lighting body,
e) comparing said parameters with a measure of the chromatic emissions made in a generic
second time instant (t1) different from said first instant,
f) regulating the intensity of the light sources of said lighting body in a way to
bring the intensity of the chromatic emissions to the values measured in said first
time instant or to a predetermined value.
2. Method according to claim 1 characterized in that the step of regulating the intensity of the light sources is effected using the mutual
ratios between the differences of intensities of the chromatic emissions of said set
of emissions.
3. Method for controlling the light emission of a lighting body (50) having at least
two light sources that can be controlled in intensity, said method comprising the
steps of:
a) defining at least a reference point (200) in a zone (191) which is not lightened
by said lighting body,
b) making a measure of the intensity of each component of a set of chromatic emissions
in said reference point, said measure being carried out with a natural or artificial
reference light and in a defined first time instant (t0),
c) computing the difference of intensity between said chromatic emissions and computing
the measured absolute intensity, obtaining a set of parameters,
d) storing said parameters in a suitable memory location of the lamp,
e) storing in said lighting body the intensity that must be given to the source depending
on said differences,
f) interpolating the intensity to be given to the light sources in a generic second
time instant (t1) as a function of said differences between said parameters.
4. A method according to claim 3 characterized in that said step of regulating the intensity of the light sources is made using the mutual
ratios between the differences.
5. A method according to claim 1 or 2 comprising the further steps of measuring the intensity
table as a function of time and regulating the intensity as a function of time instant
derived upon interpolation of said table.
6. A method according to claims 3 and 4 comprising the further steps of measuring the
intensity table as a function of time and regulating the intensity as a function of
time instant derived upon interpolation of said table.
7. Lighting apparatus comprising at least two light sources (100) that can be controlled
in intensity, and characterized in that it is suitable to operate with a method according to any of claims 1 to 6.
8. Apparatus according to claim 7, comprising at least: a control system (120) adapted
to control the light intensity of said at least two sources (100) continuously and
independently; at least one microcontroller (130); at least one sensor (140) adapted
to measure the intensity of a set of chromatic emissions in at least one location
(150, 200); at least a data memory (160).
9. Apparatus according to claim 8, further comprising a clock generator (170) defining
the time scale of said microcontroller (130).
10. Apparatus according to claim 8 or 9, said light sources being LED diodes.