Field of the Invention
[0001] The present invention relates generally to electrodeless high intensity discharge
(HID) lamps. More particularly, the present invention relates to an improved HID lamp
and excitation coil configuration for maximizing light output.
Background of the Invention
[0002] In a high intensity discharge (HID) lamp, a medium to high pressure ionizable gas,
such as mercury or sodium vapor, emits visible radiation upon excitation caused by
passage of current through the gas. One class of HID lamps comprises inductively-coupled
electrodeless lamps which generate an arc discharge by generating a solenoidal electric
field in a high-pressure gaseous lamp fill. In particular, the lamp fill, or discharge
plasma, is excited by radio frequency (RF) current in an excitation coil surrounding
an arc tube. The arc tube and excitation coil assembly acts essentially as a transformer
which couples RF energy to the plasma. That is, the excitation coil acts as a primary
coil, and the plasma functions as a single-turn secondary. RF current in the excitation
coil produces a time-varying magnetic field, in turn creating an electric field in
the plasma which closes completely upon itself, i.e., a solenoidal electric field.
Current flows as a result of this electric field, resulting in a toroidal arc discharge
in the arc tube.
[0003] A practical excitation coil configuration avoids as much light blockage by the coil
as possible in order to maximize light output. An exemplary coil configuration is
described in commonly assigned U.S. Pat. No. 5,039,903 of G.A. Farrall, issued August
13, 1991 and incorporated by reference herein. However, even though the excitation
coil configuration of the Farrall patent is effective in avoiding much light blockage
from the lamp, it is desirable to provide a new lamp and coil configuration which
increases light output even further.
Summary of the Invention
[0004] The present invention is set forth in Claims 1 and 2.
[0005] The centroid of the excitation coil of an electrodeless HID lamp is offset from the
centroid of the arc tube a predetermined distance along a common central axis in order
to maximize total light output. In a preferred embodiment, i.e., for a lamp configured
to direct light downward, the centroid of the excitation coil is situated above the
centroid of a spheroidal arc tube; and the upper hemisphere of the arc tube is coated
with a reflective coating in order to further maximize light output.
Brief Description of the Drawings
[0006] The features and advantages of the present invention will become apparent from the
following detailed description of the invention when read with the accompanying drawing
figures in which:
Figure 1 illustrates an electrodeless HID lamp and excitation coil configuration according
to the present invention;
Figure 2 illustrates an electrodeless HID lamp and excitation coil configuration according
to an alternative embodiment of the present invention; and
Figure 3 illustrates an electrodeless HID lamp and excitation coil configuration according
to another alternative embodiment of the present invention
Detailed Description of the Invention
[0007] Figure 1 illustrates an electrodeless HID lamp and excitation coil configuration
in accordance with the present invention. As shown, HID lamp 10 includes an arc tube
14 preferably formed of a high temperature glass, such as fused quartz, or an optically
transparent or translucent ceramic, such as polycrystalline alumina. Typically, as
shown, a light-transmissive envelope 15 surrounds arc tube 14. An excitation coil
16 is disposed about arc tube 14, i.e., outside envelope 15, and is coupled to a radio
frequency (RF) ballast 18 for exciting a toroidal arc discharge 20 therein. By way
of example, arc tube 14 is shown as having a substantially ellipsoid shape. However,
arc tubes of other shapes may be desirable, depending upon the application. For example,
arc tube 14 may be spherical or may have the shape of a short cylinder, or "pillbox",
having rounded edges, if desired.
[0008] Arc tube 14 contains a fill in which an arc discharge having a substantially toroidal
shape is excited during lamp operation. A suitable fill is described in U.S. Patent
No. 4,810,938 of P.D. Johnson, J.T. Dakin and J.M. Anderson, issued on March 7, 1989,
and assigned to the instant assignee. The fill of the Johnson et al. patent comprises
a sodium halide, a cerium halide and xenon combined in weight proportions to generate
visible radiation exhibiting high efficacy and good color rendering capability at
white color temperatures. For example; such a fill according to the Johnson et al.
patent may comprise sodium iodide and cerium chloride, in equal weight proportions,
in combination with xenon at a partial pressure of about 500 torr. Another suitable
fill is described in commonly assigned U.S. Pat. No. 4,972,120 of H.L. Witting, issued
November 20, 1990, which patent is incorporated by reference herein. The fill of the
Witting patent comprises a combination of a lanthanum halide, a sodium halide, a cerium
halide and xenon or krypton as a buffer gas. For example, a fill according to the
Witting patent may comprise a combination of lanthanum iodide, sodium iodide, cerium
iodide, and 250 torr partial pressure of xenon.
[0009] As illustrated in Figure 1, RF power is applied to the HID lamp by RF ballast 18
via excitation coil 16 coupled thereto. Excitation coil 16 is illustrated as comprising
a two-turn coil having a configuration such as that described in U.S. Pat. No. 5,039,903
of G.A. Farrall, cited hereinabove. Such a coil configuration results in very high
efficiency and causes minimal light blockage from the lamp. The overall shape of the
excitation coil of the Farrall patent is generally that of a surface formed by rotating
a bilaterally symmetrical trapezoid about a coil center line situated in the same
plane as the trapezoid, but which line does not intersect the trapezoid. However,
other suitable coil configurations may be used, such as that described in commonly
assigned U.S. Patent no. 4,812,702 of J.M. Anderson, issued March 14, 1989, which
patent is incorporated by reference herein. In particular, the Anderson patent describes
a coil having six turns which are arranged to have a substantially V-shaped cross
section on each side of a coil center line. Another suitable excitation coil may be
of solenoidal shape, for example. Still another suitable excitation coil may be of
a spiral type which conforms to, but is spaced apart from, at least a portion of the
arc tube.
[0010] In operation, RF current in coil 16 results in a time-varying magnetic field which
produces within arc tube 14 an electric field that completely closes upon itself.
Current flows through the fill within arc tube 14 as a result of this solenoidal electric
field, producing toroidal arc discharge 20 therein. Suitable operating frequencies
for RF ballast 18 are in the range from 0.1 to 300 megahertz (MHz), exemplary operating
frequencies being 6.78 MHz and 13.56 MHz.
[0011] In accordance with the present invention, the centroid
a of the excitation coil of the electrodeless HID lamp is offset from the centroid
b of the arc tube a predetermined distance
d along a common central axis Y-Y. As shown, in a preferred embodiment, the centroid
a of the excitation coil is situated above the centroid
b of a spheroidal arc tube. Furthermore, a reflective coating 30 is preferably disposed
on the outer surface of the upper hemisphere of arc tube 14 in order to further maximize
light output. As described in European patent application, Serial No. 92310081.2 )docket
no. LD-10,184), such a reflective coating is disposed on a portion of the arc tube
nearest the excitation coil so that light that would otherwise be blocked thereby
is usefully directed out of the arc tube. Such a reflective coating preerably covers
between approximately 30% and 70% of the arc tube. Moreover, such a reflective coating
is comprised of one or more electrically insulating materials, preferably one or more
refractory insulating materials, such as alumina, silica, zirconia, titania, magnesia
and tantala.
[0012] The lamp and excitation coil configuration of the present invention results in an
increased total light output as well as a higher forward lumen ratio, i.e., ratio
of forward light output by the lower hemisphere of the arc tube to total light output
from the lamp. By way of example, for an HID lamp and excitation coil configured as
shown in Figure 1 with an arc tube having an outer diameter of approximately 26 mm
and a height of approximately 19 mm, the total light output and the forward lumen
ratio increased for a displacement
d in the range from approximately 3 to 6 millimeters, resulting from a reduction in
the direct light incident on the surface of the excitation coil. However, further
displacement of the coil resulted in a decrease in light output due to the reduced
coupling efficiency between the arc tube and the excitation coil. Hence, for the lamp
shown in the Figure 1, there is an optimum range of displacement of the coil with
respect to the arc tube.
[0013] In one alternative embodiment, as illustrated in Figure 2, excitation coil 16 is
offset from the arc tube by a distance d' such that the excitation coil does not cover
any of the uncoated portion of the arc tube. In this way, substantially no light is
absorbed by the excitation coil.
[0014] In still other alternative embodiments, a coated or uncoated arc tube may be employed
in conjunction with suitable reflectors and/or refractors. For example, as illustrated
in Figure 3, an electrodeless HID lamp and excitation coil configured according to
the present invention are employed as the light source for a luminaire 40. As shown,
luminaire 40 includes a cup-shaped enclosure 42 having an open end 44 through which
light is transmitted. A bowl-shaped refractor 46 is mounted over open end 44. As described
in European patent application no. 92310081.2 (docket no. LD-10,184), cited hereinabove,
such a refractor may have a prismatic outer surface for directing light from the lamp
to desired locations beneath the luminaire. In Figure 3, luminaire 40 is also illustrated
as including a reflective partition 48 for reflecting spill light.
[0015] Although the centroid of the excitation coil has been illustrated as being situated
above the centroid of the arc tube, it is to be understood that the centroid of the
excitation coil may be situated below the centroid of the arc tube, depending upon
the particular application and the particular reflector/refractor configurations employed.
Furthermore, other arc tube shapes may be used, if desired, with the centroid of the
excitation coil being offset from the centroid of the arc tube in order to maximize
light output in accordance with the present invention.
[0016] While the preferred embodiments of the present invention have been shown and described
herein, it will be obvious that such embodiments are provided by way of example only.
Numerous variations, changes and substitutions will occur to those of skill in the
art without departing from the invention herein. Accordingly, it is intended that
the invention be limited only by the scope of the appended claims.
1. An improved electrodeless high intensity discharge lamp of the type comprising an
excitation coil situated about an arc tube for exciting an arc discharge in an ionizable
fill contained in said arc tube, wherein the improvement comprises:
offsetting the centroid of said excitation coil from the centroid of said arc tube
a predetermined distance along a common central axis in order to maximize light output
from said lamp.
2. An electrodeless high intensity discharge lamp, comprising:
an arc tube for containing an ionizable fill; and
an excitation coil disposed about said arc tube for coupling to a radio frequency
power supply for exciting an arc discharge in said fill, the centroid of said excitation
coil being offset a predetermined distance along a common central axis from the centroid
of said arc tube in order to maximize light output from said lamp.
3. The lamp of claim 2, further comprising an outer envelope surrounding said arc tube,
said outer envelope being disposed between said arc tube and said excitation coil.
4. The lamp of claim 1 or 2, further comprising a reflective coating disposed on a portion
of said arc tube.
5. The lamp of claim 4 wherein said distance is determined such that said excitation
coil is situated about the coated portion of said arc tube.
6. The lamp of claim 4 wherein the centroid of said excitation coil is situated above
the centroid of said arc tube, said reflective coating being disposed on the upper
portion of said arc tube.
7. The lamp of claim 6 wherein said excitation coil is situated about the upper, coated
portion of said arc tube.
8. The lamp of claim 4 wherein said reflective coating covers approximately 30% to 70%
of said arc tube.
9. The lamp of claim 4 wherein said reflective coating is comprised of a a material selected
from the group consisting of alumina, silica, zirconia, titania, magnesia, tantala,
and combinations thereof.
10. The lamp of claim 4, further comprising light redirecting means for receiving light
reflected from said reflective coating and redirecting said light to control the distribution
of light output from said lamp.