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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

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