For the constant-volume path, all the energy input goes into increasing the internal energy of the gas because no work is done. P Isotherms T+ AT т V Along the constant-pressure path, part of the energy transferred in by heat is transferred out by work. Figure 20.4 Energy is trans- ferred by heat to an ideal gas in two ways.

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(i) How does the internal energy of an ideal gas change as it follows path if as shown? (a) Eint increases. (b) Eint decreases. (c) Eint stays the same. (d) There is not enough information to determine how Eint changes. (ii) From the same choices, how does the internal energy of an ideal gas change as it follows path ff ' along the isotherm labeled T + ΔT as shown?

For the constant-volume
path, all the energy input
goes into increasing the
internal energy of the gas
because no work is done.
P
Isotherms
T+ AT
т
V
Along the constant-pressure
path, part of the energy
transferred in by heat is
transferred out by work.
Figure 20.4 Energy is trans-
ferred by heat to an ideal gas in
two ways.
Transcribed Image Text:For the constant-volume path, all the energy input goes into increasing the internal energy of the gas because no work is done. P Isotherms T+ AT т V Along the constant-pressure path, part of the energy transferred in by heat is transferred out by work. Figure 20.4 Energy is trans- ferred by heat to an ideal gas in two ways.
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