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Modern Engineering Thermodynamics

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774 CHAPTER 19: Introduction to Coupled Phenomena<br />

EXAMPLE 19.2 (Continued )<br />

Solution<br />

a. From Eq. (19.15), we have that<br />

Thus,<br />

α fe-cu = − dϕ fe<br />

dT<br />

<br />

cu<br />

<br />

I=0<br />

where T is in °C not K. At T = 100.°C, this becomes<br />

α fe-cu = −ð−13:4 + 0:028 T + 0:00039 T 2 Þ × 10 −6 V/K<br />

α fe-cuð100:°CÞ = 6:70 × 10 −6 V/K<br />

b. From Eq. (19.33) we have 11 π fe-cu = Tα fe-cu = ð100: + 273:15 KÞð6:70 × 10 −6 V/KÞ = 2:50 × 10 −3 V<br />

11 Note that, even though most of the temperature to voltage correlations published for thermocouples are written in terms of relative temperature units<br />

(°C or°F), the multiplying temperature factor T in the Peltier and Kelvin coefficient equations is always in absolute units (K or R).<br />

The following example illustrates the thermoelectric effect used in a temperature measurement circuit. Note particularly<br />

the result obtained in part c, where the effect of connecting the thermocouple wires to a remote instrument<br />

using standard copper lead wires is investigated.<br />

EXAMPLE 19.3<br />

The chromel-alumel thermocouple circuit shown below has its cold junction at 0°C and its hot junction at 100.°C. Assuming<br />

that the absolute Seebeck coefficients α ch = 23.0 × 10 −6 V/K and α al = −18.0 × 10 −6 V/K are constant over this temperature<br />

range, determine<br />

a. The open circuit thermoelectric (Seebeck) voltage for the chromel-alumel portion of the circuit.<br />

b. The absolute and relative Peltier coefficients for each chromel-alumel junction.<br />

c. The influence of the copper lead wires on the potentiometer voltage reading for the lead wire junction temperatures<br />

shown in Figure 19.8.<br />

Alumel<br />

20°C<br />

Potentiometer<br />

a f<br />

Copper<br />

b e<br />

25°C 25°C<br />

20°C<br />

Alumel<br />

c<br />

0°C<br />

Chromel<br />

d<br />

100°C<br />

FIGURE 19.8<br />

Example 19.3.<br />

Solution<br />

a. The relative Seebeck coefficient for the chromel-alumel circuit is<br />

α ch-al = α ch − α al = ½23:0 − ð−18:0ÞŠ × 10 −6 V/K = 41:0 × 10 −6 V/K<br />

and for a constant α ch-al , Eq. (19.15) can be integrated to give<br />

−ϕ ch-al = α ch-alðT H − T C Þ = ð41:0 × 10 −6 V/KÞð100: − 0KÞ = 4:1 × 10 −3 V = ϕ al-ch<br />

(note that ϕ al-ch = −ϕ ch-al ).

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