Temperature measuring device utilizing birefringence in photoelectric element

A temperature measuring device intended to use the photoelastic effect of a transparent element. The present invention employs as the temperature sensing element a thermal expansion photoelastic cell comprising a photoelastic element and a stress generating element which are closely contacted with each other for yielding stress of anisotropy in the photoelastic element, which changes in response to changing ambient temperature, as the stress generating element is quite remarkably different in thermal expansion coefficient from the photoelastic element. An element is further provided to detect phase difference between two orthogonal light components passed through the photoelastic element which are one polarized component in a stress direction and the other component polarized in a direction perpendicular to the above stress direction when linearly polarized light is passed through the photoelastic element of the thermal expansion photoelastic cell. The detected phase difference is converted into a temperature, which is then displayed on a display device.

FIELD OF THE INVENTION 
The present invention relates to an optical temperature measuring device 
and more particularly, a temperature measuring device capable of measuring 
temperature by using photoelastic effect. 
PRIOR ART 
Various temperature measuring devices have been well known. The most 
popular one uses a thermocouple as its sensor. The temperature measuring 
device using a thermocouple is used in those cases where temperature at a 
remote place must be measured. The thermocouple is low in cost and easy to 
handle, and moreover can make high accuracy temperature measurements. It 
is, however, interfered by electromagnetic wave because 
thermoelectro-motive force generated between two different metals is very 
small. Therefore, the temperature measuring device which uses the 
thermocouple cannot be used in high electric or magnetic fields, for 
example. 
The conventional temperature measuring device which can be used in high 
electric or magnetic fields measure temperature by using a change of an 
energy gap of a semiconductor. If the energy gap changes, the edge of the 
absorption spectrum changes. This change can be detected as the change of 
transmission of LE light which has peak spectrum near the edge of the 
absorption spectrum. This temperature measuring device uses light as 
signals transmission media. This temperature measuring device can be used 
in high electric or magnetic fields. However, the temperature measuring 
device is extremely low in sensitivity because the change of the energy 
gap of the semiconductor depending on temperature is small. It is 
therefore impossible for this temperature measuring device to measure a 
slight change of temperature. 
As described above, the conventional optical temperature measuring devices 
could not measure temperature with high accuracy because they were low in 
temperature sensitivity. 
SUMMARY OF THE INVENTION 
The object of the present invention is therefore to provide an optical 
temperature measuring device which is simple in construction and capable 
of measuring temperature with high accuracy even in high electric or 
magnetic field. 
A temperature measuring device according to the present invention comprises 
a thermal expansion photoelastic cell including a photoelastic element and 
a stress generating means which are closely contacted with each other for 
yielding anisotropic stress in a photoelastic element in response to 
ambient temperature because the stress generating means is quite different 
in thermal expansion coefficient from the photoelastic element; a means 
for making linearly polarized light which is entered into the photoelastic 
element of the thermal expansion photoelastic cell; a means for detecting 
phase difference between two polarized light components passed through the 
photoelastic element, which are, for example, one component polarized in a 
stress direction or largest stress direction, and the other one polarized 
in a direction perpendicular to the above stress direction thereof; and a 
means for converting the detected phase difference into a temperature and 
displaying the converted temperature. 
When the temperature measuring device is arranged as described above, 
stress in the photoelastic element changes according to changing ambient 
temperature. Stress thus generated in the photoelastic element also 
changes accordingly. This stress has anisotropy. When anisotropic stress 
is yielded in the photoelastic element, the photoelastic element has 
birefringence (or anisotropy of refraction) depending upon the stress. The 
degree of this birefringence in the photoelastic element can be detected 
phase difference between two orthogonal polarized components passed 
through the photoelastic element, which are one component polarized in a 
stress direction or largest stress direction thereof and the other 
component polarized in a direction perpendicular to the stress direction 
thereof. The system for detecting this phase difference may be wellknown. 
When materials of the photoelastic element and the stress generating means 
are selected in such a way that large thermal stress is yielded in the 
photoelastic element in response to changing ambient temperature, 
temperature detecting sensitivity can be easily enhanced. This enables the 
temperature measuring device of the present invention to measure 
temperature over a range of from -20.degree. C. to 70.degree. C. with 
higher accuracy, as compared with the conventional temperature measuring 
device using change of energy gap of the semiconductor depending upon 
ambient temperature.

BEST MODE FOR EMBODYING THE INVENTION 
The present invention will be described in detail with reference to the 
accompanying drawings. 
FIG. 1 shows the arrangement of an example of the temperature measuring 
device according to the present invention. 
Numeral 10 represents a sensor system located at the temperature measuring 
point and this sensor system 10 includes thermal expansion photoelastic 
cell 12. 
As shown in FIG. 2, thermal expansion photoelastic cell 12 comprises 
photoelastic element 14 made of a silica glass plate having length (l) of 
10 mm, width (w) of 7 mm and thickness (t) of 4 mm, for example, filler 
members 18 and 20 embedded symmetrical and parallel relative to center 
line 16 in photoelastic element 14, and rectangular sleeve 21 closely 
fitted onto photoelastic element 14. Filler members 18 and 20 are made of 
epoxy resin and each of them fills a through-hole formed in photoelastic 
element 14 and having a diameter of 1.5 mm, for example. The thermal 
expansion coefficient of epoxy resin of filler members 18 and 20 is about 
150 times as large as that of silica glass of photoelastic element 14. 
When the ambient temperature rises at the area where thermal expansion 
photoelastic cell 12 is located, both of photoelastic element 14 and 
filler members 18, 20 are thermally expanded. However, photoelastic 
element 14 is quite remarkably different in thermal expansion coefficient 
from filler members 18 and 20. Photoelastic element 14 is forced in 
rectangular sleeve 21. Therefore, stress at that portion of photoelastic 
element 14 which is between filler members 18 and 20 becomes larger in a 
direction of axis (x) than in another direction of axis (y) in Cartesiain 
coordinates shown in FIG. 2. In other words, filler members 18 and 20 work 
as stress generating means 22 yielding stress anisotropy in photoelastic 
element 14 according to ambient temperature because filler members 18 and 
20 are quite remarkably different in thermal expansion from photoelastic 
element 14. 
Polarizer 26 is located facing one end face 24 of photoelastic element 14 
when viewed in the length direction of photoelastic element 14. The 
polarizing plane of this polarizer 26 is tilted at the angle 45 degrees 
relative to axis (x) of Cartesiain coordinates shown in FIG. 2. Lens 28 
whose optical axis is in line with axis (z) of the Cartesiain coordinates 
is located outside polarizer 26. One end of optical fiber 30 is located 
outside lens 28 while the other end thereof remote from the temperature 
measuring point is optically connected to light source 34 (for example an 
LED) through lens 32. 
1/4 wave plate 38, analyzer 40 and lens 42 are located on the same optical 
axis, facing other end face 36 of photoelastic effect element 14. 1/4 wave 
plate 38 holds one of its main axes parallel to axis (x) of Cartesiain 
coordinates shown in FIG. 2. The polarizing plane of analyzer 40 is 
perpendicular to that of polarizer 26. One end of optical fiber 44 is 
located outside lens 42 while the other end thereof remote from the 
temperature measuring point is optically connected to photodetector 46 
which is, for example, a photodiode. Outputs of photodetector 46 are 
amplified by amplifier 48 and then applied to signal processor means 50, 
which calculates the ambient temperature at the area where sensor system 
10 is located as will be described later. The ambient temperature thus 
calculated is displayed on display means 52. Sensor system 10 is roughly 
shown in FIG. 1, but it is actually arranged that the above-mentioned 
components are located as described above and fixed on a substrate by a 
bonding agent, keeping only the outer faces of thermal expansion 
photoelastic cell 12 exposed but the other components shielded by cover. 
As already described above, photoelastic element 14 which works as thermal 
expansion photoelastic cell 12 is quite remarkably different in thermal 
expansion coefficient from filler members 18 and 20 embedded in 
photoelastic element 14. When the ambient temperature rises, therefore, 
stress at that portion of photoelastic element 14 which is between filler 
members 18 and 20 becomes larger in the direction of axis (x) than in the 
direction of axis (y). This stress corresponds to the ambient temperature. 
When this anisotropy of stress is caused in photoelastic element 14 made 
of silica glass, element 14 comes to have birefringence or anisotropy of 
refractive index. 
When light of a certain intensity is sent from light source 34, it enters 
into optical fiber 30 through lens 32 and optical fiber 30 guides it to 
sensor system 10 located at the temperature measuring section. The light 
coming out of optical fiber 30 is converted by lens 28 into parallel 
beams, which enter into polarizer 26. Polarizer 26 emits linearly 
polarized light which includes polarized components tilted at the angle 45 
degrees relative to the direction in which the stress of photoelastic 
element 14 becomes the largest. This light passes through photoelastic 
element 14 and comes out of the other end face of the element 14. Phase 
difference .phi. between the two orthogonal components of the light 
passing through photoelastic element 14 which are polarized component in 
the direction of axis (x) and polarized one in the direction of axis (y) 
is yielded by the birefringence of photoelastic element 14 which 
corresponds to the ambient temperature. This phase difference .phi. is 
represented by 
EQU .phi.=2.pi.l(nx-ny)/.lambda. (1) 
where the refractive index of the light polarized in the direction of axis 
(x) is nx, the refractive index of light polarized in the direction of 
axis (y) is ny, the wavelength of light is .lambda., and the length of 
photoelastic element 14 in the direction in which light passes through 
element 14 is l. 
Since nx and ny change according to the ambient temperature, phase 
difference .phi. changes according to the ambient temperature, too. 
The light which has passed through photoelastic element 14 then passes 
through analyzer 40, whose polarizing plane is arranged perpendicular to 
that of polarizer 26, and comes to photodetector 46 through lens 42 and 
optical fiber 44. Intensity (I) of the light can be expressed as follows: 
EQU I.infin.I.sub.O (1-cos2.phi.)2 (2) 
wherein I.sub.O represents the intensity of light emitted through polarizer 
26. When the relation of phase difference .phi. relative to the ambient 
temperature is previously known, the ambient temperature can be obtained 
from the measured light intensity I. In the case of this embodiment of the 
present invention, 1/4 wave plate 38 is interposed to make (I) 
proportional to .phi.. Therefore, the light intensity is expressed as 
EQU I.infin.I.sub.O (1+sin2.phi.)/2 (3) 
At that range where phase difference .phi. is small, I is proportional to 
.phi.. 
Outputs of photodetector 46 are amplified by amplifier 48 and then applied 
to signal processor means 50. Signal processor means 50 calculates the 
ambient temperature using a previously obtained input/temperature 
calibration table and this calculated temperature value is displayed on 
display means 52. Ambient temperature (T) can be thus monitored 
immediately. 
Sensor system 10 for measuring temperature are composed of only optical 
ones in this case. Even when sensor system 10 is located in a high 
electric or magnetic field, therefore, it can measure temperature without 
being interfered with by the high electric or magnetic field. In addition, 
detection sensitivity can be easily enhanced only by selecting the 
material of stress generating means 22. Because stress generating means 22 
can yield anisotropic stress in photoelastic element 14 corresponding to 
the ambient temperature when the material of means 22 is quite remarkably 
different in thermal expansion from photoelastic element 14. 
FIG. 3 shows a variation of the thermal expansion photoelastic cell. 
Thermal expansion photoelastic cell 60 comprises photoelastic element 62 
which is made of silica glass and shaped like a rectangular pole, two 
members 64 and 66 each which are made of epoxy resin and shaped like a 
rectangular pole, and rectangular sleeve-like frame 68 made of a material 
of which thermal expansion coefficient is smaller than that of silica 
glass of photoelastic element 62, wherein two members 64 and 66 which 
sandwich photoelastic element 62 between them are closely fitted into 
frame 68. 
With thermal expansion photoelastic cell 60 arranged as described above, 
anisotropic stress is generated in photoelastic effect element 62 
responsive to ambient temperature because of the difference of thermal 
expansion coefficient between photoelastic element 62 and members 64, 66. 
The thermal expansion coefficient of epoxy resin is larger than that of 
silica glass. Larger stress in the direction of axis (x) can be generated 
than that in the direction of axis (y) in this case in photoelastic 
element 62, corresponding to changing ambient temperature. Frame 68 and 
members 64, 66 work as stress generating means 70 in this case. Thermal 
expansion photoelastic cell 60 can be used instead of thermal expansion 
photoelastic cell 12 shown in FIG. 1. 
FIG. 4 shows a further variation of the thermal expansion photoelastic 
cell. Thermal expansion photoelastic cell 80 comprises photoelastic 
element 82 made of Pyrex glass or polycarbonate shaped a rectangular pole, 
outer member 84 which is made of Invar alloy and is contact at 4 side 
faces with photoelastic element 82, and through-holes 86 and 88 which is 
symmetrical and parallel to axis (z) in photoelastic element 82. 
The thermal expansion coefficient of Pyrex glass or polycarbonate is larger 
than that of Invar alloy. In addition, through-holes 86 and 88 are made on 
axis (x) in this case. With this thermal expansion photoelastic cell 80, 
therefore, stress in the direction of axis (y) in photoelastic element 82 
can be generated larger than that in the direction of axis (x), 
corresponding to changing ambient temperature. Outer member 84 and 
through-holes 86, 88 work as stress generating means 90 in this case. 
FIG. 5 shows a still further variation of the thermal expansion 
photoelastic cell. This thermal expansion photoelastic cell 100 is a 
variation of thermal expansion photoelastic cell 80 shown in FIG. 4. In 
the case of this variation, therefore, through-holes in photoelastic 
element 82 are filled with inner members 102 and 104 which are made of a 
material with a larger thermal expansion coefficient than that of the 
material of photoelastic element 82. 
With thermal expansion photoelastic cell 100, therefore, stress in the 
direction of axis (x) in photoelastic effect element 82 can be generated 
become larger than that in the direction of axis (y) responding to 
changing ambient temperature, so that temperature detecting sensitivity 
can be enhanced. Outer and inner members 84, 102 and 104 work as stress 
generating means 106 in this case. FIG. 6 shows the relation of ambient 
temperature and the output of amplifier 48 when thermal expansion 
photoelastic cell 100 is used instead of thermal expansion photoelastic 
cell 12 shown in FIG. 1. As apparent from FIG. 6, the output of amplifier 
48 changes almost linearly when ambient temperature changes. 
FIG. 7 shows a light incident end face of thermal expansion photoelastic 
cell 110 which is a still further variation according to the present 
invention. Thermal expansion photoelastic cell 110 comprises photoelastic 
element 112 made of Pyrex glass or polycarbonate, outer member 114 which 
is made of Invar alloy and is contact at 4 side faces with photoelastic 
element 112, and inner members 116, 118 which are made of a material with 
a thermal expansion coefficient larger than that of the material of 
photoelastic element 112, and which are located on both sides of element 
112 in the direction of axis (x). 
When thermal expansion photoelastic cell 110 is arranged as described 
above, stress in the direction of axis (x) is far larger than stress in 
the direction of axis (y), in photoelastic element 112 in response to 
changing ambient temperature. Temperature detecting sensitivity can be 
thus enhanced. Outer and inner members 114, 116 and 118 work as stress 
generating means 120 in this case. 
FIG. 8 shows a light incident end face of thermal expansion photoelastic 
cell 130 which is a still further variation according to the present 
invention. Thermal expansion photoelastic cell 130 comprises photoelastic 
element 132 which is made of Pyrex glass or polycarbonate and is shaped as 
a rectangular pole, and outer member 134 which is made of Invar alloy and 
is contact at 2 side faces with photoelastic element 132 and leaves spaces 
between two sides of element 132 in the direction of axis (y). 
When thermal expansion photoelastic cell 130 is arranged like this, stress 
in the direction of axis (x) can be far larger than stress in the 
direction of axis (y), of those stresses which are generated in 
photoelastic element 132 in response to changing ambient temperature. 
Temperature detecting sensitivity can be thus enhanced. Outer member 134 
and spaces 136, 138 which is left between both sides of element 132 in the 
direction of axis (y) and outer member 134 work as stress generating means 
140 in this case. 
FIG. 9 shows a light incident end face of thermal expansion photoelastic 
cell 150 which is a still further variation according to the present 
invention. Thermal expansion photoelastic cell 150 comprises photoelastic 
element 152 which is made of Pyrex glass or polycarbonate and is shaped a 
rectangular pole, outer member 154 which is made of Invar alloy closely 
contact with photoelastic element 152 leaving both end faces of element 
152 uncovered and forming spaces between both sides of element 152 in the 
direction of axis (y) and outer member 154, and circular through-holes 
156, 158 which is made symmetrical to axis (y) and parallel to axis (z) in 
photoelastic effect element 152. 
When thermal expansion photoelastic cell 150 is arranged like this, stress 
in the direction of axis (x) can be made far larger than stress in the 
direction of axis (y), in photoelastic element 152 in response to changing 
ambient temperature, thereby enabling temperature detecting sensitivity to 
be remarkably enhanced. In this arrangement, element 152 extended in the 
direction of axis (z) and through-holes 156, 158 work as stress generating 
means 164. Through-holes 156 and 158 may be filled with members made of a 
material with a thermal expansion coefficient larger than that of the 
material of photoelastic element 152. 
FIG. 10 shows a light incident end face of thermal expansion photoelastic 
cell 170 which is a still further variation according to the present 
invention. In this case of this thermal expansion photoelastic cell 170, 
photoelastic element 172 is made of Pyrex glass or polycarbonate and 
shaped like a rectangular pole. Outer member 174 is made of Invar alloy 
and encloses photoelastic element 172 of which both end faces of element 
172 is uncovered. A space is left between one side of element 172 in the 
direction of axis (x) and outer member 174. This assembly of photoelastic 
element 172 and outer member 174 is closely fitted into cylindrical member 
176. Auxiliary member 178 is fitted into the space between one side of 
element 172 in the direction of axis (x) and outer member 174 and screw 
180 loads bias force to auxiliary member 178 from outside cylindrical 
member 176 in the direction of axis (x). Circular through-holes are made 
symmetrical to axis (y) and parallel to axis (z) in photoelastic effect 
element 172. They are filled with inner members 182 and 184 which are made 
of a material with a thermal expansion coefficient larger than that of the 
material of photoelastic element 172. 
When thermal expansion photoelastic cell 170 is arranged like this, 
cylindrical member 176, outer member 174 and inner members 182, 184 work 
as stress generating means 186. Therefore, stress in the direction of axis 
(x) can be made larger than stress in the direction of axis (y) in 
photoelastic element 172 in response to changing ambient temperature. When 
screw 180 is adjusted to apply initial bias stress to photoelastic element 
172 in the direction of axis (x), the compressive stress can be kept by 
the initial bias stress, even if outer member 174 shrinks in a case where 
the thermal expansion coefficient of inner members 182 and 184 is smaller 
than that of outer member 174. 
FIG. 11 shows a light incident end face of thermal expansion photoelastic 
cell 190 which is a still further variation according to the present 
invention. In the case of this thermal expansion photoelastic cell 170, 
column 192 is made of glass and rectangular pole-like spaces 194 and 196 
are made symmetrical to axis (x) and parallel to axis (z) in column 192. 
That portion 198 of column 192 which is between spaces 194 and 196 is 
doped with Ge or B to have a thermal expansion coefficient different from 
that of the other portion thereof and to work as the photoelastic element. 
Therefore, the other portion of column 192 and portions 194, 196 thereof 
work as stress generating means 200. 
The thermal expansion photoelastic cell can be further modified as follows: 
In the case of thermal expansion photoelastic cell 130 shown in FIG. 8, 
inner members made of a material with a thermal expansion coefficient 
larger than that of the material of photoelastic element 132 may be fitted 
into spaces between both sides of photoelastic element 132 in the 
direction of axis (x) and outer member 134. 
The stress generating means of the above-described thermal expansion 
photoelastic cell are all intended to apply a compression force to the 
photoelastic element. In the case of thermal expansion photoelastic cell 
80 shown in FIG. 4, however, a pull stress can be applied to photoelastic 
element 82 when outer member 84 which is made of brass with a large 
thermal expansion coefficient is bonded to photoelastic element 82 made of 
Pyrex glass. The stress generating means may work to apply pull stress to 
the photoelastic element in this manner. Industrial Applicability: 
As apparent from the above, the temperature measuring device according to 
the present invention can be useful in those cases where temperature must 
be measured with high accuracy in high electric or magnetic fields.