dW = Fds = pAds = pdV W = pdV
dW = Fds = pAds = pdV W = pdV
dW = Fds = pAds = pdV W = pdV
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We defined heat capacity C and specific heat c (heat capacity per mass) as:<br />
Q = C ΔT = c m ΔT<br />
For water, c = 1cal/g o C = 1 Btu/lb o F = 4187 J/kg K<br />
The molar specific heat is the heat capacity per mole.<br />
However, the amount of heat needed to<br />
raise the temperature of 1 mole by<br />
1 kelvin depends on whether we<br />
perform the operation at constant<br />
pressure or at constant volume:<br />
Q = n C P ΔT or Q = n C V ΔT<br />
In both cases, Q= ΔE int +W:<br />
ΔE int is the same, but W is not!<br />
Consider a process at constant volume, raising the<br />
temperature by ΔT . Q = n C V ΔT<br />
Q= ΔE int + W<br />
W = 0 !<br />
Q = ΔE int = (3/2) nR ΔT = n C V ΔT<br />
→ C V = (3/2)R = 12.5 J/molK<br />
→ E int = n C V T<br />
15<br />
16<br />
8