[0001] The present invention relates to an arc tube for a high pressure discharge lamp.
In particular, though not exclusively, the present invention relates to a high intensity
metal halide discharge lamp.
[0002] Many high intensity discharge lamps, fabricated from fused silica and employing molybdenum
foil pinch seals, operate at very high internal pressures, up to pressures of 3.0MPa.
Accordingly, one important criterion in determining the quality of the arc tubes used
in these lamps is the ultimate bursting strength of the arc tube - the internal pressure
to which the arc tube can be subjected before it explodes. Requirements on lamp performance
dictate that arc tubes should be fabricated with bursting strength as high as possible
consistent with a good geometrical accuracy and freedom from oxidation of metallic
components. Both the design of the arc tube and the detailed values of parameters
of the seal making process, such as times, pressures, gas flow rates etc, are known
to effect the attainable ultimate bursting strength.
[0003] Figures 1(a) and 1(b) are schematic representations of an arc tube for a known single
ended low power metal halide lamp; Figure 1(b) is a cross-sectional view of the arc
tube of Figure 1(a). The discharge chamber 4 of the arc tube is made as near spherical
as possible, although ellipsoidal geometries are also acceptable. A spherical geometry
for the arc tube yields a near isothermal temperature profile for the operating lamp.
This is a highly desirable feature since it ensures stability of lamp performance,
particularly colour and light output, with lamp operating position. Such lamps are
classified as 'universal burning' and are suitable for use in display lighting.
[0004] An example of this type of lamp is the 150W Arcstream 3000 lamp which operates at
internal pressures of about 2.5MPa. Arc tubes for this type of lamp are fabricated
from silica tubing of 11 mm bore with a wall thickness of 1.25 mm. The tubes contain
a mixture of mercury together with the iodides and bromides of tin, sodium and thallium.
Argon is also present at a cold pressure of 24KPa to act as a starting gas. Each arc
tube is pinch sealed into a quartz outer jacket with nitrogen gas in the space between
the arc tube and outer jacket. The assembly so produced is mounted onto a bi-pin ceramic
base.
[0005] It has been found by experience that arctubes made to this design having an ultimate
bursting strength of less than 5.5MPa when tested are more likely to fail violently
by explosion in operation. However lamps manufactured according to existing processes
produced excessive manufacturing scrap when pneumatically pressure tested at pressures
of 5.5MPa. Extensive experimentation to optimise the levels of important parameters
of the manufacturing process using the Taguchi method (a partial factorial method
of systematic experimentation using orthogonal arrays) failed to increase the ultimate
bursting strength (as measured by a hydraulic pressure test) to the required level.
[0006] It is an object of the present invention to at least alleviate the problem outlined
hereinbefore.
[0007] According to the present invention there is provided an arc tube for a high pressure
discharge lamp, the arc tube comprising a discharge chamber containing a fill and
electrical conductors extending into the discharge chamber to form electrodes, the
electrical conductors being sealed in the arc tube by a single pinch seal portion
wherein, at the interface of the discharge chamber and the pinch seal portion, the
discharge chamber has at least in part a non-concave outline.
[0008] The inventors have surprisingly found that arc tubes provided in accordance with
the present invention have a significantly higher bursting strength than prior art
lamps, as shown in Figure 1, in which, at the interface of the discharge chamber and
the pinch seal portion, the discharge chamber has a concave outline. The inventors
believe this is due to changes made in the complex way in which the electrode structures
interrupt the internal geometry of the discharge chamber as compared with prior art
arc tubes. Accordingly, in making the invention, the inventors had needed to appreciate
that despite the prior art, it might be worthwhile investigating the role of pinch
seal geometry on ultimate bursting strength.
[0009] In a preferred embodiment for use in any orientation, the non-concave outline is
a rectilinear outline. Modification of the geometry of the discharge chamber to other
than a spherical geometry had been expected to modify the lamp performance to an unacceptable
extent, in particular, to increase the variation of lamp colour with operating position.
The inventors were surprised to find that the performance of lamps provided in accordance
with this preferred embodiment was acceptable for a universal burning lamp.
[0010] Alternatively, in an embodiment for use in a single orientation, the preferred non-concave
outline is a convex outline. The limitation of use of the arc tube to a single orientation
enables the lamp engineer to modify the fill of the arc tube to provide an optimum
performance for that single orientation.
[0011] Embodiments of the present invention will now be described, by way of example only,
and with reference to the accompanying drawings in which:
Figure 1 is a schematic representation of a prior art arc tube as described hereinbefore;
Figure 2 shows a discharge lamp containing an arc tube provided in accordance with
the present invention;
Figures 3 and 4 are schematic representations of arc tubes provided in accordance
with the present invention.
[0012] Figure 2 shows a high pressure discharge lamp 10 provided in accordance with the
present invention. An arc tube 12 is located in a quartz outer jacket 14 by a pinch
seal 16 (shown in part). The space 18 between the outer jacket 14 and the arc tube
12 is filled with nitrogen gas. The assembly so produced is mounted onto a bi-pin
ceramic base 22.
[0013] The arc tube 12 is fabricated from silica tubing having a bore and a wall thickness
dependant on the wattage of the lamp to be produced which may be from 20W to 2.5kW.
For a 150W lamp, the bore is 11 mm and the wall thickness is 1.25 mm. The arc tube
12 has a discharge chamber 24 in which is present a fill comprising a mixture of 25
mg mercury together with the iodides and bromides of tin, sodium and thallium. Argon
is also present at a cold pressure of 24KPa to act as a starting gas. A pair of electrical
conductors 26, 28 are sealed into one end of the arc tube 12 at a single pinch seal
portion 30 to provide a pair of spaced apart electrodes 32, 34 extending into the
discharge chamber 24. The other end of each of the electrical conductors 26, 28 is
joined to a strip of molybdenum foil 36, 38 in the pinch seal portion 30. The strips
of foil 36, 38 are in turn joined to a pair of electrical leads 40, 42, for connection
to the pins of the ceramic base 22 via the pinch seal 16. The value of the dimensions
indicated in Figure 2 is a = 12.8 mm, b = 14.0 mm and c = 15.5 mm.
[0014] The shape of the discharge chamber 24 in the arc tube 12 is defined, inter alia,
by the shape of the pinch seal portion 30. In the discharge lamp 10, the discharge
chamber 24 is shown as having a rectilinear outline 44 at the interface of the discharge
chamber 24 and the pinch seal portion 30. The arc tube is accordingly hereinafter
termed a 'rectilinear arc tube'. Alternatively, the discharge chamber may have a convex
outline at the interface of the discharge chamber and the pinch seal portion 30 -
hereinafter termed a 'convex arc tube'. The radius of curvature of the convex outline
can be as low as 7.5 mm (for a 150W lamp) to infinity (ie 'rectilinear'). In convex
'arc tubes' used in the experiments described hereinafter, the radius of curvature
of the convex outline was 22.0 mm.
[0015] For ease of comparison, Figures 3 and 4 are schematic representations, similar to
Figure 1, of lamps provided in accordance with the present invention. Figure 3a shows
a rectilinear arc tube 46 corresponding to the arc tube of Figure 2. Figure 4a shows
a convex arc tube 48. Figures 3b and 4b show cross-sections of the arc tubes of Figures
3a and 4a along respectively the lines III - III and IV-IV. The prior art arc tube
of Figure 1 will hereinafter be termed a 'concave arc tube'.
[0016] The inventors have experimentally tested the arc tubes hereinbefore described for
bursting strength and lamp performance. Sixty arc tubes of each type - concave, rectilinear
and convex, were constructed by a process using optimized parameters as determined
by the Taguchi analysis. The arc tubes were pressurized hydraulically to failure and
the bursting pressures noted. The results of this experiment are shown in Table 1
below.
Table 1
|
|
Convex |
Rectilinear |
Concave |
Bursting pressure MPa |
Mean |
7.4 |
7.17 |
5.45 |
Standard deviation |
0.98 |
1.17 |
1.17 |
Maximum |
11.2 |
10.5 |
8.45 |
Minimum |
5.5 |
5.0 |
2.07 |
[0017] As can be seen, there is a considerable difference in bursting pressure and hence
ultimate bursting strength between arc tubes of the traditional concave type and either
the rectilinear or convex types. Statistical analysis of these results show this difference
to be highly significant, i.e. it is extremely unlikely that such a result could be
obtained by chance. The difference between rectilinear and convex arc tubes was found
not to be statistically significant, though it is the inventors' opinion that the
results indicate that the convex arc tubes tested were slightly stronger than the
rectilinear arc tubes tested. Thus, when ultimate bursting strength only is taken
into consideration, the preferred type of arc tube is one of the rectilinear or convex
type, not the concave type.
[0018] As already outlined hereinbefore, lamp performance also needs to be considered when
determining arc tube geometry. Relevant parameters were measured for a large number
of arc tubes of each type. The results are shown in Tables 2 to 4; Table 2 for (prior
art) concave arc tubes; Table 3 for rectilinear arc tubes; Table 4 for convex arc
tubes.
TABLE 2
CONCAVE ARC TUBES |
|
x |
y |
CCT |
Lm/W |
Vt |
W |
Cap Down (CD) |
.4361 |
.4078 |
3042 |
86.1 |
97.2 |
150.6 |
Horizontal (H) |
.4483 |
.4174 |
2922 |
85.6 |
95.4 |
150.6 |
Shift CD to H |
.0122 |
.0096 |
-120 |
|
|
|
Cap up (CU) |
.4459 |
.4148 |
2938 |
90.2 |
99.7 |
153.9 |
Shift CD to CU |
.0098 |
.0070 |
-104 |
|
|
|
TABLE 3
RECTILINEAR ARC TUBES |
|
x |
y |
CCT |
Lm/W |
Vt |
W |
Cap Down (CD) |
.4433 |
.4067 |
2916 |
82.2 |
94.6 |
149.3 |
Horizontal (H) |
.4531 |
.4162 |
2840 |
81.8 |
93.0 |
148.9 |
Shift CD to H |
.0098 |
.0095 |
-76 |
|
|
|
Cap Up (CU) |
.4563 |
.4153 |
2785 |
85.1 |
95.3 |
150.2 |
Shift CD to CU |
.0130 |
.0086 |
-131 |
|
|
|
TABLE 4
CONVEX ARC TUBES |
|
x |
y |
CCT |
Lm/W |
Vt |
W |
Cap Down (CD) |
.4334 |
.4086 |
3097 |
81.0 |
91.4 |
145.8 |
Horizontal (H) |
.4551 |
.4180 |
2825 |
82.2 |
91.5 |
147.1 |
Shift CD to H |
.0217 |
.0094 |
-272 |
|
|
|
Cap Up (CU) |
.4572 |
.4162 |
2781 |
85.0 |
93.3 |
149.3 |
Shift CD to CU |
.0238 |
.0076 |
-316 |
|
|
|
[0019] Explanation of Terms used in Tables:
x, y colour co-ordinates - a measure of the colour of the light emitted by the arc
tube.
CCT correlated colour temperature - a measure of the colour of the light emitted by
the arc tube.
Lm/W efficacy of lamp in lumens per Watt.
V
t voltage drop across arc tube in volts.
W Lamp Power in Watts.
Cap down Results for operating orientation in which base of lamp is vertically below
arc tube.
Horizontal Results for operating orientation in which base of lamp is on same level
as arc tube.
Cap Up Results for operating orientation in which base of lamp is vertically above
arc tube.
[0020] The results surprisingly show that colour stability with operating orientation for
rectilinear arc tubes is very similar to that of concave arc tubes. As already outlined,
it had expected that concave arc tubes would have the best colour stability with operating
orientation. Accordingly for lamps to be used for universal burning, the preferred
arc tube is the rectilinear type.
[0021] As expected, lamps with convex arc tubes show double the shift in X colour co-ordinates
and colour temperature as compared with lamps with concave or rectilinear arc tubes.
However, convex arc tubes can be used in lamps intended for use in a single orientation.
[0022] Modifications to the embodiments described hereinbefore will be apparent to those
skilled in the art. In particular, the internal pressure within the arc tube is primarily
controlled by the amount of mercury dosed into the arc tube and so the gains in ultimate
bursting strength illustrated by the specific embodiments described can be expected
for any metal halide dose. Similar gains are also expected for lamps of ratings other
than 150W. The present invention is expected to be equally applicable to lamps utilising
bare arc tubes and to arc tubes sealed into glass or quartz envelopes with or without
a gas fill between the arc tube and outer jacket.
1. An arc tube for a high pressure discharge lamp, the arc tube comprising a discharge
chamber containing a fill and electrical conductors extending into the discharge chamber
to form electrodes, the electrical conductors being sealed in the arc tube by a single
pinch seal portion wherein, at the interface of the discharge chamber and the pinch
seal portion, the discharge chamber has at least in part a non-concave outline.
2. An arc tube according to Claim 1 wherein, at the interface of the discharge chamber
and the pinch seal portion, the discharge chamber has a non-concave outline.
3. An arc tube according to Claims 1 or 2 for use in any orientation wherein said
non-concave outline is a rectilinear outline.
4. An arc tube according to Claims 1 or 2 for use in a single orientation wherein
said non-concave outline is a convex outline.
5. An arc tube according to any one of the preceding Claims wherein the fill comprises
mercury, an inert gas and at least one metal halide.
6. A high pressure discharge lamp comprising an arc tube according to any one of the
preceding claims.