Thermodynamic - Work Done is Path Dependend
Thermodynamic - Work Done
- Definition:
In Thermodynamics, Work Done Refers To The Energy Transfer
That Occurs When A Force Acts On A System, Causing It To
Undergo A Displacement. It Is A Form Of Energy Transfer That
Can Change The State And Properties Of A Thermodynamic
System.
- The Sign Of Work Done Is Important In Thermodynamics. If
Work Is Done On The System (Energy Being Transferred Into
The System), It Is
Considered Positive.
- If Work Is Done By The System (Energy Being Transferred Out
Of The System), It Is Considered Negative.
- Units Of Work:
Work Is Typically Expressed In Units Of Energy, Such As Joules
(J) In The International System Of Units (SI). Other Common
Units Include Foot-Pounds (Ft-Lb) And Calorie (Cal).
- Types Of Work Done: In Thermodynamics,Some Common Types
Include Expansion Work, Compression Work, Electrical Work,
And Shaft Work. Each Type Of Work Has Its Own Specific
Formula And Considerations.
- Applications:
Understanding Work Done In Thermodynamics Is Crucial In
Various Real-Life Applications, Such As The Design Of Engines,
Power Plants, Refrigeration Systems, And Energy Conversion
Devices.
Thermodynamic - Work
Done Is Path Dependend
- One Crucial Aspect Of Work In Thermodynamics Is That It Is
Path Dependent.
- This Means That The Amount Of Work Done Depends On The
Specific Path Taken During The Process.
- Different Paths Can Lead To Different Amounts Of Work, Even If
The Initial And Final States Of The System Are The Same.
- Prove That Work Done Is Path Dependend
Ans :
- Work Done Along Path
A-D-C
- Work Done Formula
δw=Pdv
- W1 = P1(V2-V1)+ 0....(1)
(In Eq.(1) 0 Means Volume Constant)
- Work Done Alongpath A-B-C
- W2 = 0 + P2(V2-V1)
W2 = P2(V2-V1)....(2)
- Work Done Along A → C
W3 = 1/2
(V2-V1)(P1-P2) + P2(V2-V1)
= 1/2 P1(V2-V1)-
1/2 P2(V2-V1) + P2(V2-V1)
= 1/2 P1(V2-V1) +
1/2 P2(V2-V1)
- W3 = 1/2 (P1+P2) (V2-V1)....(3)
- From Equation (1),(2),(3)
W1≠W2≠W3
- It Means Work Done Depend On Path
#Thermodynamics
#WorkDone
#PathDependence
#EnergyTransfer
#ThermalProcesses
#ThermodynamicWork
#WorkPath
#PathDependentWork
#IrreversibleProcesses
#CarnotCycle
#EntropyChange
#FirstLawofThermodynamics
#SecondLawofThermodynamics
#ReversibleProcesses
#ThermodynamicEquilibrium