Patent Application
20130099663
The present invention relates to a plasma light source.
In European Patent No EP1307899, granted in our name there is claimed a light source comprising a waveguide configured to be connected to an energy source and for receiving electromagnetic energy, and a bulb coupled to the waveguide and containing a gas-fill that emits light when receiving the electromagnetic energy from the waveguide, characterised in that:
In our European Patent No 2,188,829 there is described and claimed a light source to be powered by microwave energy, the source having:
We refer to this as our Light Emitting Resonator or LER patent. Its main claim as immediately above is based, as regards its prior art portion, on the disclosure of our EP1307899, first above.
In our European Patent Application No 08875663.0, published under No WO 2010055275, there is described and claimed a light source comprising:
We refer to this as our Clam Shell application, in that the lucent wave guide forms a clam shell around the bulb.
As used in our LER patent, our Clam Shell application and this specification:
We have recently disclosed LER improvements in Patent Applications filed on Jun. 30, 2011, under Nigel Brooks references Nos 3133 and 3134. The improvements relate to the incorporation of a lucent tubes within a bore in the solid body, the tube being integral with the body and having the void formed in it. In order to put beyond doubt that the present improvement applies to the improvements of these two applications, we define as follows:
The LER patent, the Clam Shell Applications and the above LER improvement applications have in common that they are in respect of:
A microwave plasma light source having:
the arrangement being such that on introduction of microwaves of a determined frequency a plasma is established in the void and light is emitted via the Faraday cage.
In this specification, we refer to such a light source as a Lucent Waveguide Microwave Plasma Light Source or LWMPLS.
With the objective of improving our LWMPLS, we have determined that by comparison with conventional plasma lamps using electroded bulbs we can achieve higher wattage per unit length of plasma.
To set this in perspective, the light output and lives of conventional electroded plasma, i.e. HID (High Intensity Discharge), bulbs is very dependent on both the minimum and maximum wall temperature. The minimum wall temperature sets the vapour pressure of the additives, the higher the additive pressure generally the higher the light output. The maximum wall temperature sets a limit on the life of the bulb. Below 725° C. bulbs can have a long life; above 850° C. the life deteriorates rapidly.
The wall loading of a bulb is its input power divided by internal bulb surface area, usually expressed in Watts per cm2. Wall loading is used as crude metric to encompass both temperatures. Many proposals have been made to minimise the difference between these two temperatures. For long life of electroded bulbs, greater than 15,000 hrs life, 20 Watts per cm2 is regarded as an upper limit while 50 Watts per cm2 bulb lives are reckoned to be less than 2,000 hrs.
The efficiency with which microwave energy is converted into light—in terms of lumens per watt—increases in our LWMPLSs with their operating wattage, all other things being equal. This results from maximum temperature in the plasma increasing and is linked to conductivity or skin depth of the plasma which decreases as the power per unit length is increased.
We have been surprised by how marked this effect is and accordingly, we now believe that we can specify improved LWMPLS and LER performance, in terms of them or at least their plasma voids being short for their operational power.
According to the invention there is provided a Lucent Waveguide Microwave Plasma Light Source having a void length L and a rated power P, wherein:
We prefer to operate at 125 W per cm or higher and for higher powers at least 140 W per cm.
Measuring plasma loading in terms of the actual length of the plasma in the void, which may be able to be observed through the lucent waveguide, is awkward. We prefer to measure the overall length of the void and subtract its radius from each end on the basis that the plasma is strongest in the central parallel portion of a domed end void and does not extend to the extreme end of flatter ended voids. While, it is possible to measure the actual microwave power, or at least the power transferred to a magnetron powering a LWMPLS, we prefer to measure power in terms of the rated power of the light source, i.e. the overall power consumption of the light source.
In some of our LWMPLSs, the plasma void is directly in the lucent crucible, as in our LER, and in others the plasma void is in a lucent bulb within a lucent waveguide as in our Clamshell Application. This invention and the definition of our LWMPLSs is not restricted to these two arrangements. Other arrangements are the subject of certain of our pending and un-published patent applications.
Again in certain of our LWMPLSs, we are able to operate at much lower internal surface areas of their voids for their operational power.
In particular, we prefer to operate at a wall loading of between 100 W per cm2 and 300 W per cm2. For higher powers, we would normally expect to operate at least at 125 W per cm2 and preferably in the range between 150 W per cm2 and 250 W per cm2.
We measure wall loading in terms of the internal surface area of the part of the void for which we measure plasma loading, with the power being the rated power.
We ascribe the fact that we can operate at such higher wall loading than traditionally to the conductive and radiant heat transfer occurring from our lucent crucibles and waveguides.
To help understanding of the invention, a specific embodiment thereof will now be described by way of example and with reference to the accompanying drawings, in which:
Referring to the drawings, a lucent crucible 1 for an LER LWMPLS has a central void 2 having microwave excitable material 3 within it. The void is 4 mm in diameter and 21 mm long. The crucible is of fused quartz and is 21 mm long between end flats 4 and is circular cylindrical with a 49 mm outside diameter. The identicalness of the length of the void and the length between the end flats of the crucible results from this being constructed from a piece of quartz, having a bore and closed at the ends of the bore. The length of the crucible—but not the void—is somewhat arbitrary for present purposes, because in the preferred TM010 mode, resonance is independent of the crucible length. This LER is designed to operate at 280 watts at 2.45 GHz.
Also shown are a bore 5 for an antenna 6 to introduce microwaves into the crucible and a Faraday cage 7 for retaining microwave resonance within the crucible. It is backed by an aluminium carrier 8 to which it is held by the cage.
With the LER operating at 280 Watts in TM010 mode, corresponding to a plasma loading of 133 W per cm and a wall loading of 106 W per cm2, we measure a wall temperature of 700° C. Such a device has an efficacy of up to 110 lumens per Watt.
To measure the plasma loading, we divide the rated power of the LER by the length of the plasma. In our experience the plasma 11 stops just short of the full length 12 of the void, as shown in
We measure the overall length of the void and subtract its radius 15 from each end on the basis that the plasma is strongest in the central parallel portion of a domed end void and does not extend to the extreme ends of flatter ended voids.
In order to achieve efficacies>110 lumens per Watt we have found it necessary to increase the loading per unit length of plasma to be greater than 150 W per cm. In order that the lamp has a reasonable lifetime, simultaneously, we have found it necessary to restrict the maximum wall loading to be less than 300 W per cm2 and preferably less than 250 W per cm2.
Examples of higher plasma loadings for crucibles operating in the TM010 mode are:
Thus for high efficiency LERs with reasonably long life the operating conditions may be set out as follows:
While these conditions apply to resonators operating in any mode, cylindrical LERs operating in the TM010 and TM110 modes have advantages in ease of manufacturability and cost compared to resonators operating in other modes. This is because these two modes have the property that the resonant frequency is independent of the length of the cavity. This makes it particularly easy to vary the power input per unit length of plasma by varying the length of the LER and using butt sealed tubes at each end of the resonator the cost is kept to a minimum.
| Number | Date | Country | Kind |
|---|---|---|---|
| 1011303.3 | Jul 2010 | GB | national |
| Filing Document | Filing Date | Country | Kind | 371c Date |
|---|---|---|---|---|
| PCT/GB11/01015 | 7/5/2011 | WO | 00 | 1/10/2013 |
