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Modern Engineering Thermodynamics

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258 CHAPTER 8: Second Law Closed System Applications<br />

EXAMPLE 8.6 (Continued )<br />

Here, the unknowns are (a) _Q , (b) _U , (c) _S P , and (d) an expression for _S P as a function of time. The system is the lightbulb<br />

itself, and apparently, we do not need to know any specific system properties to solve this problem.<br />

The answers for parts a and b can be found in Example 5.2 as<br />

a). _Q = −100: W:<br />

b). _U = 100: W:<br />

The answer to part c can be obtained by the indirect method of the SRB. From Eq. (8.2), we have<br />

_S P = _S − d Z <br />

dQ<br />

dt Σ T b act<br />

Since we are given that the surface temperature of the bulb is isothermal,<br />

Z <br />

d dQ<br />

= 1 Z<br />

d Q<br />

dQ =<br />

_ dt Σ T b T b dt Σ T b<br />

and<br />

Q _S P = _S − _ T b<br />

In part a, we have steady state operation so _S = 0, then the answer to part c is<br />

Q _S P = − _ =<br />

100: W<br />

= 0:261 W/K<br />

T b ð110: + 273:15 KÞ The solution to part d is obtained by recognizing that. in part b. The bulb is insulated, so _Q = 0, then<br />

_S P = _S<br />

The surface and internal temperatures of the bulb are not constant here. If we recognize that most of the mass of the bulb is<br />

made up of incompressible material (glass and tungsten wire), then we can write<br />

s − s ref = c ln ðT/T ref Þ = c ln ðTÞ− c ln ðT ref Þ<br />

where s ref and T ref are values chosen at some arbitrary reference state. Then,<br />

_S = m_s = mc <br />

dT<br />

= mc _T <br />

T dt T<br />

Similarly, we can write<br />

mu− ð u ref<br />

Þ = cT− ð T ref Þ<br />

so that<br />

<br />

_U = m _u = mc dT <br />

= mc _T <br />

dt<br />

Therefore,<br />

_S =<br />

U _ T = _S P<br />

The temperature in this equation is the mean temperature of the bulb and can be evaluated from the answer to part b,<br />

where we find that _U = 100: W:<br />

Therefore,<br />

_T = dT<br />

dt<br />

= _ U<br />

mc = constant<br />

and integration of this equation gives<br />

U<br />

T =<br />

_ mc t + T 0<br />

where T 0 is the bulb temperature immediately before the insulation is applied. Therefore, the answer to part d is<br />

_S P =<br />

_U<br />

=<br />

_Ut<br />

mc + T 0<br />

mc<br />

t + mcT 0<br />

_U<br />

Since _U = 100:W: and m, c, and T 0 are all constant measurable quantities, it is clear from this result that _S p slowly decays to<br />

zero as time t goes to infinity. However, the bulb temperature increases linearly with time, so the bulb overheats and burns<br />

out quickly.

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