APPLICATION OF 1 LAW OF THERMODYNAMICS TO ISOPROCESSES |
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Process |
Constant m=const M=const |
Graph |
Change in internal energy |
Record 1st law thermodynamics |
Physical meaning |
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Isothermal expansion |
T=const pV=const |
|
U=const ΔU=0 |
Q=A' |
An isothermal process cannot occur without heat transfer. All the amount of heat transferred to the system is expended on the performance of mechanical work by this system. |
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Isothermal compression |
T=const pV=const |
|
U=const ΔU=0 |
A=-Q |
An isothermal process cannot occur without heat transfer. All work of external forces is emitted in the form of heat. |
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Isochoric the heating |
V=const |
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p↑ T↑ U↑ ΔU>0 |
A=0 Q= ΔU |
All the amount of heat transferred to the system is spent on increasing its internal energy. |
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Isochoric cooling |
V=const |
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p↓ T↓ U↓ ΔU<0 |
A=0 Q= ΔU<0 |
The system reduces its internal energy, giving off heat to surrounding bodies. |
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Isobaric expansion (heating) |
p=const |
|
V↑ T↑ U↑ ΔU>0 |
Q=ΔU+A' ΔU=Q-А'>0 |
The amount of heat transferred to the system exceeds the perfect mechanical work. Part of the heat is spent on the work, and some - to increase the internal. energy. |
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Isobaric compression (cooling) |
p=const |
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V↓ T↓ U↓ ΔU<0 |
ΔU=Q+A<0 Q<0 |
The amount of heat given by the system exceeds the work of external forces. Part of the heat the system gives by reducing the internal. energy. |
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