Thermocouple

When two metals having different work functions are placed together, a voltage is generated at the junction which is nearly proportional to the temperature. This junction is called a thermocouple.

Working Principle of Thermocouple

  • Thomas Seebeck discovered in 1821 that when two dissimilar metals were in contact, a voltage was generated where the voltage was a function of temperature. The device, consisting of two dissimilar metals joined together, is called a thermocouple and the voltage is called the Seebeck voltage.
  • If both ends of the two conductors are connected [Fig 1 (a)] and a temperature difference is maintained between the two junctions, a thermoelectric current will flow through the closed circuit (generation mode).
Seebeck effect, Principle of working of thermocouple,
Figure 1: Seebeck effect
  • If the circuit is opened [Fig (b)] an emf will appear across the open circuit (sensing mode). It is this emf that is measured in a thermocouple sensor.
  • For example, joining copper and constantan produces a voltage on the order of a few tens of millivolts with the positive potential at the copper side. An increase in temperature causes an increase in voltage.

Conductors a and b are homogeneous. Let junctions 1 and 2 are at temperatures T2 and T1.

\begin{array}{l}
em{f_a} = {\alpha _a}({T_2} - {T_1})\\
em{f_b} = {\alpha _b}({T_2} - {T_1})
\end{array}

Total emf is given by

\begin{array}{l}
em{f_T} = em{f_a} - em{f_b}\\
\therefore em{f_T} = {\alpha _a}({T_2} - {T_1}) - {\alpha _b}({T_2} - {T_1})\\
\therefore em{f_T} = {\alpha _{ab}}({T_2} - {T_1})
\end{array}

  • {\alpha _a} and{\alpha _a}are the absolute Seebeck coefficients given in mV/°C and are properties of the materials A, B.

  • {\alpha _{ab}} = {\alpha _a} - {\alpha _b} is the relative Seebeck coefficient of the material combination A and B, given in mV/°C

  • The relative Seebeck coefficients are normally used.
  • Table 1: Absolute Seebeck coefficients for selected elements (Thermoelectric series)

Material

a [mV/°K]

p-Silicon

100 – 1000

Antimony (Sb)

32

Iron (Fe)

13.4

Gold (Au)

0.1

Copper (Cu)

0

Silver (Ag)

-0.2

Aluminum (Al)

-3.2

Platinum (Pt)

-5.9

Cobalt (Co)

-20.1

Nickel (Ni)

-20.4

Bismuth (Sb)

-72.8

n-Silicon

-100 to -1000

Joining Two Disimilar Metals

  • There are several methods of joining the two dissimilar metals.

  1. Weld the wires together
    • This produces a brittle joint, and if not protected from stresses, this type of thermocouple can fracture and break apart.
    • During the welding process, gases from the welding can diffuse into the metal and cause a change in the characteristic of the thermocouple.
  1. Solder the wires together
    • This has the disadvantage of introducing a third dissimilar metal. Fortunately, if both sides of the thermocouple are at the same temperature, the Seebeck voltage due to thermocouple action between the two metals of the thermocouple and the solder will have equal and opposite voltages and the effect will cancel.
    • Another disadvantage is that in many cases the temperatures to be measured are higher than the melting point of the solder and the thermocouple will come apart.

It would appear to be a simple matter to measure the Seebeck voltage and create an electronic thermometer. To do this, wires could be connected as shown in Figure to make the measurement.

Construction and Working

Construction of thermocouple,
Figure 2: Effects of additional parasitic thermocouple

Assume that the meter uses copper wires as shown.

In this case, where the two copper wires come in contact there is no problem, but where the copper comes in contact with another metal, such as the constantan thermocouple wire, the two dissimilar metals create another thermocouple, which generates its own Seeback voltage.

For this example, copper interconnecting wires were used and the thermocouple was copper and constantan. The composition of the wires is immaterial, as any combination will produce these parasitic thermocouples with the problems of additional Seeback voltages.

It is an unavoidable fact that there will be at least two thermocouple junctions in the system. To contend with this, it is necessary that the temperature of one of the junctions be known and constant.

Therefore, there is a fixed offset voltage in the measuring system. In early times, it is mandatory to place this junction in a mixture of ice and water, thus stabilising the temperature to 0°C as shown in Figure 3.

Thermocouple
Figure 3: Application of a reference junction to Thermocouple

In modern-age electronic reference junction is used and it is called the reference or cold junction because this junction was traditionally placed in the ice bath.

Nowadays, electronic devices are used to measure thermocouple voltages and to convert from the Seeback voltage to temperature, and to compensate for the reference junction.

Errors occurring During the Measurement using Thermocouple

Open Junction

  • There are many sources of an open junction. Usually, the error introduced by an openjunction is of such an extreme magnitude that an open junction is easily spotted.
  • Bysimply measuring the resistance of the thermocouple, the open junction is easilyidentified.

Insulation Degradation

  • The thermocouple is often used at very high temperatures. In some cases, the insulationcan break down and causes a significant leakage resistance which will cause an error inthe measurement of the Seeback voltage.
  • In addition, chemicals in the insulation candefuse into the thermocouple wire and cause decalibration.

Thermal Conduction

  • The thermocouple wire will shunt heat energy away from the source to be measured. Forsmall temperature to be measured, small diameter thermocouple wire could be used.
  • However, the small diameter wire is more susceptible to the effects. If a reasonablecompromise between the degrading effects of small thermocouple wire and the loss ofthermal energy and the resultant temperature error cannot be found, thermocoupleextension wire can be used.
  • This allows the thermocouple to be made of small diameterwire, while the extension wire covers majority of the connecting distance.

Galvanic Action

  • Chemicals coming in contact with the thermocouple wire can cause a galvanic action. Thisresultant voltage can be as much as 100 times the Seebeck voltage, causing extremeerrors.

Decalibration

  • This error is a potentially serious fault, as it can cause slight error that may escapedetection. Decalibration is due to altering the characteristics of the thermocouple wire,thus changing the Seeback voltage.
  • This can be caused due to subjecting the wire toexcessively high temperatures, diffusion of particles from the atmosphere into the wire, orby cold working the wire.

Types of Thermocouple

  • The first material in each type (E, J, K, R, S and T) is positive, the second negative.
  • Table 2: Thermocouples (standard types and others) and some of their properties

Materials

Sensitivity [mV/°C] at 25°C.

Standard Type designation

Temperature range [°C]

Notes

Copper/Constantan

40.9

T

-270 to 600

Cu/60%Cu40%Ni

Iron/Constantan

51.7

J

-270 to 1000

Fe/60%Cu40%Ni

Chromel/Alumel

40.6

K

-270 to 1300

90%Ni10%Cr/55%Cu45%Ni

Chromel/Constantan

60.9

E

-200 to 1000

90%Ni10%Cr/60%Cu40%Ni

Platinum(10%)/Rhodium-Platinum

6.0

S

0 to 1450

Pt/90%Pt10%Rh

Platinum(13%)/Rhodium-Platinum

6.0

R

0 to 1600

Pt/87%Pt13%Rh

Silver/Paladium

10

200 to 600

Constantan/Tungsten

42.1

0 to 800

Silicon/Aluminum

446

-40 to 150

Carbon/Silicon Carbide

170

0 to 2000

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