Temperature Measurements thermocouples, thermistors and resistance thermometers

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Temperature Measurements thermocouples, thermistors and resistance thermometers • exposure and shielding of thermometers • soil temperature measurements • response times and sampling rates

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Temperature Measurements thermocouples, thermistors and resistance thermometers exposure and shielding of thermometers soil temperature measurements response times and sampling rates. Thermo couple measures temperature difference (T1 – T2) between two junctions. Copper. T1. - PowerPoint PPT Presentation

Transcript of Temperature Measurements thermocouples, thermistors and resistance thermometers

Page 1: Temperature Measurements thermocouples, thermistors and resistance thermometers

Temperature Measurements

• thermocouples, thermistors and resistance thermometers

• exposure and shielding of thermometers

• soil temperature measurements

• response times and sampling rates

Page 2: Temperature Measurements thermocouples, thermistors and resistance thermometers

Thermocouple measures temperature difference (T1 – T2) between two junctions

Copper

Copper

Constantan Voltage output

T1

T2

- Easy to construct. Just twist together Copper and Constantan wires, and solder.

- Beautifully suited to measuring temperature differences directly.

- Requires knowledge of temperature at T2 (“reference” temp) to get actual temperature at T1.

Page 3: Temperature Measurements thermocouples, thermistors and resistance thermometers

Can construct “thermopile” of several thermocouples connected in series.

- Increases signal strength. Calibration factor increases according to the number of junction pairs in the “pile”.

- Allows for spatial averaging, if desired.

- For example, measuring soil temperature gradients…

Upper level

Lower level

Voltage to Data Logger

= Cu, = Con

Soil surface

Page 4: Temperature Measurements thermocouples, thermistors and resistance thermometers

Thermocouple measures temperature difference (T1 – T2) between two junctions

Data logger

Copper

Constantan

Copper

Copper

Constantan Voltage output

1. Where is the second junction, when using logger?

2. What temperature difference is being measured?

T1

T2

Page 5: Temperature Measurements thermocouples, thermistors and resistance thermometers

The output signal from a thermocouple is not quite linear.

Voltage change = (a + b T) (Temperature change)

Microvolts per degree= 38.58 + 0.0428T for copper/constantan

Page 6: Temperature Measurements thermocouples, thermistors and resistance thermometers

Thermocouples

1. Estimate the maximum signal (in microvolts) you should expect from a thermocouple that is measuring an air temperature of 40 C.

2. Suppose you ignore the non-linearity of a thermocouple and always use the calibration factor for 0 C. What would the temperature error be at 40 C?

Page 7: Temperature Measurements thermocouples, thermistors and resistance thermometers

Thermocouples

1. Estimate the maximum signal (in microvolts) you should expect from a thermocouple that is measuring an air temperature of 40 C.Correct calibration factor is:38.58 + 0.0428 (40) = 40.29 microvolts/degree C

So signal is (40.29 microvolts/degree C) x 40 C = 1,611 microvolts or 1.611 millivolts

2. Suppose you ignore the non-linearity of a thermocouple and always use the calibration factor for 0 C. What would the temperature error be at 40 C?

Signal to be translated to temperature is 1,611 microvolts. Using calibration factor for 0C… 38.58 microvolts/C:1,611 microvolts /38.58 microvolts/C = 41.76 C. Answer is 1.76 C too high.

Page 8: Temperature Measurements thermocouples, thermistors and resistance thermometers

Electronic Temperature (and RH) probe which uses a thermistor, a semi-conductor material whose

resistance changes with temperature.

Advantages are… stronger signal change with temperature than thermocouple, and no reference needed.

Page 9: Temperature Measurements thermocouples, thermistors and resistance thermometers

Thermistor resistance decreases very non-linearly with increasing temperature.

Suppose we take two resistance readings and average them.

250 Kohms50 KohmsAvg = 150 Kohms

Average resistance gives correct average

temperature?

No!! Must convert to temperature before averaging.

Thermistor-based probes can contain electronics to give a linear voltage output with temperature.

Page 10: Temperature Measurements thermocouples, thermistors and resistance thermometers

Platinum resistance-temperature detector

- Resistance of wire changes with temperature

- Platinum wire is typically used, wound inside a protective casing. - stable and almost linear resistance change with temp

- non-linearity can be accounted for in logger program, yielding very accurate temperature measurements that may be used to calibrate other temperature sensors.

~ 5 cm

Page 11: Temperature Measurements thermocouples, thermistors and resistance thermometers

Exposure of thermometers (Str – P. 41)

Unshielded sensor will warm up during the day until heat loss to the air by convection matches the gain from radiation.

Radiation gain

Convection loss

(Tsensor – Tair) is the radiation error.Radiation error is reduced by:- Small sensor size- More air flow- Blocking the radiation

Page 12: Temperature Measurements thermocouples, thermistors and resistance thermometers

Temperature probe will heat above air temperature if exposed to solar radiation.

So….. what are features of a good thermometer shield?

• shades the sensor

• allows wind (or artificial ventilation)

• doesn’t warm incoming air (high solar reflectivity)

• avoids long wave gain from inside surface of shield to sensor (low emission efficiency of shield, poor conductor so inner temperature of shield not higher than air temperature)

• avoids heat conduction down signal wires

Page 13: Temperature Measurements thermocouples, thermistors and resistance thermometers

Here’s a shield that is often used at weather stations (the Gill shield).- a stack of upside-down plastic saucers .

Cut-away view

Good features?

Possible improvements?

Page 14: Temperature Measurements thermocouples, thermistors and resistance thermometers

Temp/RH probe, or thermocouple, can be used in “stacked saucers” shield.

Page 15: Temperature Measurements thermocouples, thermistors and resistance thermometers

The “Stevenson Screen” thermometer shield

World-wide way of housing manually-read thermometers, and automated T

and RH sensors

Max and min thermometers

T & RH probe

Page 16: Temperature Measurements thermocouples, thermistors and resistance thermometers

Good and poor features of the “Stevenson Screen” thermometer shield?

- needs regular repainting- bulky - too warm on calm, sunny days if no supplementary ventilation

-louvered for air flow- white, & double roof, for solar protection- wood for poor heat conduction- world-wide “standard”

Page 17: Temperature Measurements thermocouples, thermistors and resistance thermometers

Soil temperatures on an ideal sunny day.- temperature range decreases with depth,and max/min temperatures lag with depth. •Sensors must

be waterproof

•Sensor in a metal tube can give some spatial averaging

•Place horizontally to spatially average at one depth

•Place at an angle to average over a layer

Page 18: Temperature Measurements thermocouples, thermistors and resistance thermometers

Signals, sampling and sensors

Imagine we take a sample every second with our data logger, for 10 seconds.

For which of the 5 signals will our sampling yield a good 10-second average?

Sampling rate must be at least twice as fast as the period of the signal you wish to average.

Page 19: Temperature Measurements thermocouples, thermistors and resistance thermometers

How quickly does a sensor respond?

A step change is applied to the sensor at time zero.

Time constant is time required for sensor to reach 63% of the step change.

63% level

Tc = 2 sec Tc = 6 sec

Page 20: Temperature Measurements thermocouples, thermistors and resistance thermometers

1. Sampling rate must be at least 2x as fast as the period of the signal you wish to average.

2. Time constant of sensor should be 4x faster than period of the signal you wish to detect. Sensor’s response speed controls the signal fluctuations it “sees”.

Guidelines for good sampling over time.

Signal period 2x slower Sampling rate Sensor 2x faster

Page 21: Temperature Measurements thermocouples, thermistors and resistance thermometers

1. How could you modify the time constant of a temperature sensor?

2. A very small thermocouple could be used without radiation shielding. Any disadvantages of a very small sensor?

3. You decide to ask your data system to sample once each minute. What time constant should your sensor have, and what is the period of the fastest signal you can resolve?

4. Suppose you need to measure temperature fluctuations as fast as 10 cycles per second. What sensor time constant is required, and how often would you sample?

Page 22: Temperature Measurements thermocouples, thermistors and resistance thermometers
Page 23: Temperature Measurements thermocouples, thermistors and resistance thermometers

Infra-red Thermometer (IRT)

Sensor assumes object obeys the Stefan-Boltzmann law which links radiation emitted to object temperature: Radiation in W/m2 = TIRT 4

where = 5.67 X 10-8 and T is in 0K (0K = 0C + 273.2)

Senses radiation solves S-B equation TIRT signal

Looks at I-R radiation from object.

IRT

Page 24: Temperature Measurements thermocouples, thermistors and resistance thermometers

Infra-red Thermometer (IRT)But real objects are not “perfect” emitters so the S-B equation needs a reduction factor called the emissivity ( , which ranges from 0 1

Radiation in W/m2 = Tobject 4

If an object is not a perfect emitter (that is, < 1), then it is also not a perfect absorber, so it will reflect some incoming radiation from the surroundings. The fraction reflected is 1-

Therefore a real object will send out an emittedI-R stream and a reflected I-R stream.

Emitted I-R

Reflected I-R

I-R from surroundings

Page 25: Temperature Measurements thermocouples, thermistors and resistance thermometers

• IRT sees IR emissions from two sources whenpointed at an object…Emission = Tobject 4

Reflection = (1-) (I-R from surroundings)Total IR seen = Tobject 4 + (1-) (I-R surroundings)

Infra-red Thermometer (IRT)

But the IRT changes IR radiation seen into a temperature using the “perfect” S-B law, so… TIRT 4 = Tobject 4 + (1- ) (I-R surroundings)

This means TIRT does not equal Tobject unless = 1. Errors are usually small, since > 0.95 for most objects. Shiny metals are a notable exception. Their typical < 0.5, so T-measurement with an IRT can be seriously degraded by reflected I-R from surroundings.

Page 26: Temperature Measurements thermocouples, thermistors and resistance thermometers

Practice with the IRT equation.

1. Suppose an IRT pointed at the sand on a beach shows the surface temperature is 41.2 C. The sand has an emissivity of 0.97. The sky is emitting 412 W/m2. What is the error between the true sand temperature and the value from the IRT? (~ 0.6 C error)

2. A piece of aluminum foil ( = 0.15) was careless left on the grass near the beach. The foil temperature is 34.2 C. What is the error between the foil temperature and the value from the IRT? (~ 13 C error)

Page 27: Temperature Measurements thermocouples, thermistors and resistance thermometers
Page 28: Temperature Measurements thermocouples, thermistors and resistance thermometers

Maximum and minimum thermometers – design tricks

Page 29: Temperature Measurements thermocouples, thermistors and resistance thermometers

2. Link in parallel- same signal size as 1 couple (resistors 20x longest t/c).

Using thermocouples for spatial sampling.