process

5
Thermodynamic Processes • States of a thermodynamic system can be changed by interacting with its surrounding through work and heat. When this change occurs in a system, it is said that the system is undergoing a process. • A thermodynamic cycle is a sequence of different processes that begins and ends at the same thermodynamic state. • Some sample processes: Isothermal process: temperature is constant T=C Isobaric process: pressure is constant, P=C Isentropic process: entropy is

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Page 1: Process

Thermodynamic Processes

• States of a thermodynamic system can be changed by interacting with its surrounding through work and heat. When this change occurs in a system, it is said that the system is undergoing a process.

• A thermodynamic cycle is a sequence of different processes that begins and ends at the same thermodynamic state.

• Some sample processes: Isothermal process: temperature is constant T=C Isobaric process: pressure is constant, P=C Isentropic process: entropy is constant, s=C Constant-volume process, v=C Adiabatic process: no heat transfer, Q=0

Page 2: Process

Process-1• Use ideal gas assumption (closed system):

2

1

2 1

1 2

Isothermal process: T=constantEnergy balance U=Q-W, for ideal gas U= H=0since both are functions of temperature only

Q=W, W= P

ln ln

Isobaric process:

mRT dVdV dV mRTV V

V PmRT mRTV P

2

2 11

2 1 2 1 2 1

2 2 1 1 2 1

P=constant

U=Q-W, W= PdV=P dV=P(V )

( ) ( ) ( )( ) ( )

V

Q U P V V U U P V VU PV U PV H H H

Page 3: Process

Process-2

v

v

Constant volume process: V=constant

Q-W= U, W= 0, no work done

Q= U=m u=m c

Adiabatic process: Q=0Q-W= U, -W= U- W=dU (infinitesimal increment of work and energy)

dU+PdV=0, mc 0

v

PdV

dT

mRTdT dVV

c

v

2 2 2 1 1

1 1 1 2 2

1

0, , integrate and assume

c =constant

ln ln ,

v

vv

R kc

cRT dT dVdT dVV R T V

c T V T V VR T V T V V

Page 4: Process

Process-3

2 1

1 2

1 1 2

2 2 1

2 1 2 2

1 2 1 1

2 2 2 1

1 1 1

( 1)

1

1 1

, from ideal gas relation

PV=RT, , substitute

, multiply from both sides

,k

k

k

k k

T VT V

V T PV T P

T T P TT T P T

T P P VT P P

and

2

1 1 2 2kAlso and tan

For an ideal gas undergoing adiabatic process

k

k

k

V

PV PV pV cons t

Page 5: Process

Process-4

Polytropic Process: its P-V relation can be expressed asPVn = constant, where n is a constant for a specific process

Isothermal, T=constant, if the gas is an ideal gas then PV=RT=constant, n=1 Isobaric, P=constant, n=0 (for all substances) Constant-volume, V=constant, V=constant(P)(1/n), n= (for all substances) Adiabatic process, n=k for an ideal gas

1 1 2 2

2 2

1 11 1

21 11 1 2 2 1 1

1 1 2 11

( )

( )( ) ( )1 1

n n n

n n

nn n n n

PV PV PV

W PdV PV V dV

PV PV PVPV V dV V Vn n