Poisson equation Cards for beginning

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  • 04.05.2020
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APPLICATION OF 1 LAW OF THERMODYNAMICS TO ISOPROCESSES

Process

Constant

m=const

M=const

Graph

Change in

internal

energy

Record

1st law

thermodynamics

 

Physical

meaning

 

Isothermal

expansion

T=const

pV=const

Изотермическое  расширение

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.

 

Isothermal

compression

T=const

pV=const

Изотермическое  сжатие

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.

 

Isochoric

the heating

 

V=const

http://www.eduspb.com/public/img/formula/image006_13.gif

Изохорное  нагревание   

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.

 

Isochoric

cooling

 

V=const

http://www.eduspb.com/public/img/formula/image006_13.gif

Изохорное  нагревание 

p

T

U

ΔU<0

A=0

Q= ΔU<0

The system reduces its internal energy, giving off heat to surrounding bodies.

 

Isobaric

expansion (heating)

p=const

Изобарное  расширение (нагревание)

 

Изобарное  расширение (нагревание)

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.

 

Isobaric

compression (cooling)

p=const

Изобарное  сжатие (охлаждение)

Изобарное  сжатие (охлаждение)

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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