Temperature Measurements
Download
Report
Transcript Temperature Measurements
الرحيـــــِ ِم
َّ الر ْح َم ِن
َّ ِـــــم هللا
ِ ِب ْس
Temperature Measurements
Principles
Measuring Devices
Applications
Definition of Temperature
• An expression for the kinetic energy of vibrating
atoms and molecules of matter.
• Can be measured by various secondary
phenomena, e.g.,
–
–
–
–
–
change of volume or pressure,
electrical resistance,
electromagnetic force,
electron surface charge, or
emission of electromagnetic radiation.
12 Oct. 2015
BME 353 - Biomedical
Measurements and Instrumentation
2
Direct and Indirect
• Many engineering applications require direct
measurement of temperature.
–
–
–
–
Synthetic fuel research,
solar energy conversion and
new engine development are a few of these disciplines.
All industries place new emphasis on energy efficiency.
Hence, the fundamental measurement of temperature
assumes new importance.
• Temperature also effects measurement of most
physical variables and it must be measured for
compensation purposes as well.
12 Oct. 2015
BME 353 - Biomedical
Measurements and Instrumentation
3
Temperature Scale
• Celsius, divide the difference between the freezing
and boiling points of water into 100°
• Fahrenheit which divide the difference between
the freezing and boiling points of water into 180°
• °C = (5 /9) (°F - 32), and °F = (9 /5) °C + 32.
• The thermodynamic scale begins at absolute zero,
or 0 Kelvin, the point at which all atoms cease
vibrating and no kinetic energy is dissipated.
• 0 K = –273.15° C = –459.67° F.
– The official Kelvin scale does not carry a degree sign.
The units are expressed in “kelvins,” not degrees
Kelvin.
12 Oct. 2015
BME 353 - Biomedical
Measurements and Instrumentation
4
Reference Temperatures
• No temperature divider or adder
• We must rely upon temperatures established by
physical phenomena which are easily observed
and consistent in nature.
• The International Temperature Scale (ITS)
establishes seventeen fixed points and
corresponding temperatures. Examples:
– the triple-point (the temperature and pressure at which
solid, liquid, and gas phases of a given substance are all
present simultaneously in varying amounts) of water =
0.01C,
– triple-point of hydrogen = -259.3467C, and
– freezing point of silver = 961.78C.
12 Oct. 2015
BME 353 - Biomedical
Measurements and Instrumentation
5
Heat Gain and Heat Loss
• Heat gain:
–
–
–
–
Environment
Metabolism
Hot food
Shivering
12 Oct. 2015
• Heat loss:
–
–
–
–
Convection
Conduction
Evaporation
IR radiation
BME 353 - Biomedical
Measurements and Instrumentation
6
Temperature measuring devices
• Temperature can be
measured via a diverse
array of sensors. All of
them infer temperature by
sensing some change in a
physical characteristic.
• In the chemical process
industries, the most
commonly used
temperature sensors are
thermocouples, resistive
devices and infrared
devices.
12 Oct. 2015
• thermocouples,
• resistance temperature
devices
– RTD’s and
– Thermistors
•
•
•
•
•
infrared radiators,
I.C. sensors,
bimetallic devices,
liquid expansion devices,
change-of-state devices.
BME 353 - Biomedical
Measurements and Instrumentation
7
Thermocouples
Metal A
Metal A
Metal B
+
VAB
-
Metal A
Metal B
VAB = Seebeck voltage
• Two strips or wires made
of different metals and
joined at one end.
• Changes in temperature at
that junction induce
changes in the emf
between the other ends.
• As temperature goes up,
this output emf of the
thermocouple rises,
though not necessarily
linearly.
VAB = T, where , the Seebeck coefficient, is the constant of proportionality. For real
world thermocouples, is not constant but varies with temperature.
12 Oct. 2015
BME 353 - Biomedical
Measurements and Instrumentation
8
Peltier effect
• If a voltage is applied, then there will be
temperature change at the junction. This is
called the Peltier effect and can be used for
heating and cooling (refrigeration).
12 Oct. 2015
BME 353 - Biomedical
Measurements and Instrumentation
9
Equation of a thermocouple
• The output voltage “V” of a simple thermocouple (with a
reference temperature T0 = 0C = 32F) is:
1
1
2
V AT BT CT 3
2
3
volts,
where T is the temperature of the measuring junction in C, A, B,
and C are constants that depend upon the thermocouple material.
The sensitivity
V
2
S
A BT CT
T
12 Oct. 2015
volt/C
BME 353 - Biomedical
Measurements and Instrumentation
10
Characteristics of thermocouples
80
E
60
Millivolts
K
J
40
20
T
R
S
0
500 1000 1500 2000
Temperature, C
12 Oct. 2015
Type of Metals
+
E Chromel vs Constantan
J Iron vs Constantan
K Chromel vs Alumel
R Platinum vs Platinum
13% Rhodium
S Platinum vs Platinum
10% Rhodium
T Copper vs Constantan
Constantan is a metal alloy with
%60 copper and %40 nickel
BME 353 - Biomedical
Measurements and Instrumentation
11
12 Oct. 2015
BME 353 - Biomedical
Measurements and Instrumentation
12
Resistance Temperature Devices
– fine platinum wire wrapped
around a mandrel and covered
with a protective coating (also
abbreviated PRTD).
– most stable temp trans.
• Film RTD
– a platinum or metal-glass slurry
film is deposited or screened
onto a small flat ceramic
substrate, etched with a lasertrimming system, and sealed
– device size itself is small, which
means it can respond quickly to
step changes in temperature.
• Film RTD’s are less stable
12 Oct. 2015
• Thermistors
– NTC
– PTC
• most sensitive temperature
transducer
V or T
• RTD’s R = R0[1 + (T – T0)]
• platinum, nickel, or ni alloys
Thermistor
RTD
Thermocouple
Temperature, C
BME 353 - Biomedical
Measurements and Instrumentation
13
Equation of a thermistor
Steinhart-Hart equation:
a simpler equation:
1
A B(ln R) C (ln R) 3
T
T
1
C
(ln R) A
R R0e
12 Oct. 2015
(
T0 T
TT0
BME 353 - Biomedical
Measurements and Instrumentation
)
14
The Self-Heating Problem
100
0 slope
Voltage, V
10
- slope
1.0
+ slope
0.1
0.10
1.0
10.0
100.0
Current, mA
12 Oct. 2015
BME 353 - Biomedical
Measurements and Instrumentation
15
Integrated Circuit (I.C.) Sensors
+
+
1 A/K
To DVM
Current sensor
12 Oct. 2015
10 mV/K
1 M
To DVM
Voltage sensor
BME 353 - Biomedical
Measurements and Instrumentation
16
RTD
T
Self powered
Simple
Rugged
Inexpensive
Wide variety of
physical forms
Wide temperature
range
Non-linear
Low voltage
Reference required
Least stable
Least sensitive
12 Oct. 2015
Resistance
Voltage
Disadvantages
Advantages
Temperature
I.C. Sensor
R
R
Resistance
V
Thermistor
Temperature
Most stable
Most accurate
More linear than
thermocouple
T
Temperature
High output
Fast
Two-wire ohmic
measurement
Expensive
Non-linear
Slow
Limited
temperature range
Current source
Fragile
required
Small resistance
Current source
change
required
Four-wireBME 353 - Biomedical
Self-heating
Measurements and Instrumentation
measurement
T
Voltage or current
Thermocouple
V or I
Temperature
Most linear
Highest output
Inexpensive
T < 250C
Power supply
required
Self-heating
Limited
configurations
17
T
Bimetallic Devices
Metal A
Metal B
12 Oct. 2015
BME 353 - Biomedical
Measurements and Instrumentation
18
Fluid-Expansion Devices
• Types:
Safety bulb
50
– the mercury type: an environmental
hazard, so there are regulations governing
the shipment of devices that contain it.
– the organic-liquid type.
– gas instead of liquid type
• No electric power, do not pose
explosion hazards, and are stable even
after repeated cycling.
• On the other hand,
– they do not generate data that are easily
recorded or transmitted, and
– they cannot make spot or point
12 Oct.measurements.
2015
BME 353 - Biomedical
Measurements and Instrumentation
Capillary tube
Stem
0
Temperature
sensing bulb
19
Chemical (Change-of-State) Sensors
• Change-of-state temperature sensors
– labels, pellets, crayons,lacquers or liquid crystals whose appearance
changes when a certain temperature is reached.
– They are used, for instance, with steam traps – when a trap exceeds
a certain temperature, a white dot on a sensor label attached to the
trap will turn black.
– Response time typically takes minutes, so these devices often do not
respond to transient temperature changes, and accuracy is lower
than other types of sensors.
– the change in state is irreversible, except in the case of liquid-crystal
displays.
– Even so, change-of-state sensors can be handy when one needs
confirmation that the temperature of a piece of equipment or a
material has not exceeded a certain level, for instance for technical
or legal reasons, during product shipment
12 Oct. 2015
BME 353 - Biomedical
Measurements and Instrumentation
20
Radiation Detectors (IR Sensors)
12 Oct. 2015
BME 353 - Biomedical
Measurements and Instrumentation
21
100%
0.00312
0.003
80
60
0.002
40
0.001
20
T = 300 K
5
10
15
20
25
% Total power
Spectral radient emittance, W-cm-2·mm-1
m= 9.66 m
Spectral radiant emittance versus wavelength for a blackbody at 300 K on the
left vertical axis; percentage of total energy on the right vertical axis.
12 Oct. 2015
BME 353 - Biomedical
Measurements and Instrumentation
22
Fused silica
100
Sapphire
Arsenic trisulfide
Thallium
bromide
iodine
50
10
0
1
10
100
Wavelength, m
Spectral transmission for a number of optical materials.
12 Oct. 2015
BME 353 - Biomedical
Measurements and Instrumentation
23
All thermal detectors
100
Indium antimonide (InSb)
(photovoltaic)
60
Lead sulfide (PbS)
20
0
1
2
3
4
5
6
7
8
Wavelength, m
Spectral sensitivity of photon and thermal detectors.
12 Oct. 2015
BME 353 - Biomedical
Measurements and Instrumentation
24
Shutter
Ear
IR
Ambient sensor
Micro
processor
Ta
Tb
MUX
A/D
Amp.
Sensor
Waveguide
Window
Shutter
switch
Digital
display
The infrared thermometer opens a shutter to expose the sensor
to radiation from the tympanic membrane.
12 Oct. 2015
BME 353 - Biomedical
Measurements and Instrumentation
25
Details of the fiber/sensor arrangement for the GaAs
semiconductor temperature probe.
12 Oct. 2015
BME 353 - Biomedical
Measurements and Instrumentation
26