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THERMODYNAMIC PROCESSES
By Mohammed Afzal 11A
Introduction:
Conducting Insulating
Types of System:
(Diathermic)
1)
Types of System:
2)
Types of System:
3)
Depends on amount of matter.
Eg;- Mass,Vol,Moles,Heat
Capacity,Energy,Enthalpy,Entropy,Gibb’s
Free Energy,Internal energy
Does not depend on matter.
Eg:- Density,Refractive index, specific heat
capacity,pressure,temp,viscosity,concentra
tion
Molarity,Molality,mole
fraction,normality,molar entropy,molar
enthalpy,internal energy.
Extensive: Intensive:
Depends on initial and final state of a
system.
Does not depend on path of flow.
Eg:-
Pressure(P),Temp(T),Volume(V),moles(n),
Enthalpy(H),Entropy(S),Internal
Energy(U),Gibbs Free Energy(G)
Depends on path of flow.
Eg:-Heat(Q),Work(W)
State Functions: Path Functions:
Cyclic Process:
P
V
ΔP=0
ΔT=0
ΔE=0
ΔV=0
ΔS=0
ΔQ≠0
ΔW≠0
Gram SHC : c = Q/mΔT Molar SHC : C = Q/nΔT
Cisothermal -> ∞ Cadiabatic = 0 (For gases) c = 4.2 J/g °C (Water)
cv = Q/mΔT (At constant vol) Cv = Q/nΔT (At constant vol)
cP = Q/mΔT (At constant pressure) CP = Q/nΔT (At constant pressure)
Cv=Mcv CP=McP CP - CV = R CV = (f/2)R CP = (f/2 + 1)R γ=CP/CV
Specific Heat Capacity:
f(degree of
freedom)
Cv = (f/2)R CP = CV + R γ=CP/CV
3(Monoatomic) 3R/2 5R/2 5/3 = 1.66
5(Diatomic) 5R/2 7R/2 7/5 = 1.4
6(Polyatomic) 7R/2 4R 4/3 = 1.33
γ= 1 + 2/f
PV Graph for all processes:
P
V
Isobaric
Isochoric Isobaric:ΔP=0
Isochoric:ΔV=0
Isothermal:ΔT=0
Adiabatic:ΔQ=0
Occurs in infinitely small steps -> Infinite
time to finish.
Slow
Each step in equilibrium.
Not practical.
W = - ∫ Pext dV
Occurs at once -> finite time.
Fast
Equilibrium initially and finally only.
Practical situation.
W = - 𝝨pΔV
Reversible Process: Irreversible Process:
Heat given to the system -> +ve
Heat given by the system -> -ve
Work done on a system -> +ve
Work done by a system -> -ve
Conventions:
W=PV relation:
Pext = F/A ⟹ F = Pext x A
W = F Δx = Pext A Δ x ⟹ W = - Pext ΔV
Why -ve? By convention
P
V
dV
P
∫ dW = ∫ P dV
W = - ∫ Pext dV = Area under P-V
Graph
Expansion: W = -ve
Compression: W = +ve
Cyclic Process:
P
V
Wnet = Area of shape(ie square
in this case) enclosed
-ve for clockwise (as in this
case)
+ve for anti-clockwise
Isobaric(Δp=0): W= -Pext ΔV
Isochoric(ΔV=0): W = 0
Vacuum(Free Expansion):Pext = 0 ⟹ W = 0
Isobaric and Isochoric processes:
W = - ∫ Pext dV = - ∫ nRT dV/V = - nRT ln (V2/V1)
= - 2.303 nRT log10 (V2/V1)
= - 2.303 nRT log10 (P2/P1)
= - 2.303 P1V1 log10 (V2/V1) = - 2.303 P2V2 log10 (V2/V1)
= - 2.303 P1V1 log10 (P2/P1) = - 2.303 P2V2 log10 (V2/V1)
Isothermal process
Adiabatic Process

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Thermodynamics class 11 physics

  • 6. Depends on amount of matter. Eg;- Mass,Vol,Moles,Heat Capacity,Energy,Enthalpy,Entropy,Gibb’s Free Energy,Internal energy Does not depend on matter. Eg:- Density,Refractive index, specific heat capacity,pressure,temp,viscosity,concentra tion Molarity,Molality,mole fraction,normality,molar entropy,molar enthalpy,internal energy. Extensive: Intensive:
  • 7. Depends on initial and final state of a system. Does not depend on path of flow. Eg:- Pressure(P),Temp(T),Volume(V),moles(n), Enthalpy(H),Entropy(S),Internal Energy(U),Gibbs Free Energy(G) Depends on path of flow. Eg:-Heat(Q),Work(W) State Functions: Path Functions:
  • 9. Gram SHC : c = Q/mΔT Molar SHC : C = Q/nΔT Cisothermal -> ∞ Cadiabatic = 0 (For gases) c = 4.2 J/g °C (Water) cv = Q/mΔT (At constant vol) Cv = Q/nΔT (At constant vol) cP = Q/mΔT (At constant pressure) CP = Q/nΔT (At constant pressure) Cv=Mcv CP=McP CP - CV = R CV = (f/2)R CP = (f/2 + 1)R γ=CP/CV Specific Heat Capacity:
  • 10. f(degree of freedom) Cv = (f/2)R CP = CV + R γ=CP/CV 3(Monoatomic) 3R/2 5R/2 5/3 = 1.66 5(Diatomic) 5R/2 7R/2 7/5 = 1.4 6(Polyatomic) 7R/2 4R 4/3 = 1.33 γ= 1 + 2/f
  • 11. PV Graph for all processes: P V Isobaric Isochoric Isobaric:ΔP=0 Isochoric:ΔV=0 Isothermal:ΔT=0 Adiabatic:ΔQ=0
  • 12. Occurs in infinitely small steps -> Infinite time to finish. Slow Each step in equilibrium. Not practical. W = - ∫ Pext dV Occurs at once -> finite time. Fast Equilibrium initially and finally only. Practical situation. W = - 𝝨pΔV Reversible Process: Irreversible Process:
  • 13.
  • 14. Heat given to the system -> +ve Heat given by the system -> -ve Work done on a system -> +ve Work done by a system -> -ve Conventions:
  • 15. W=PV relation: Pext = F/A ⟹ F = Pext x A W = F Δx = Pext A Δ x ⟹ W = - Pext ΔV Why -ve? By convention
  • 16. P V dV P ∫ dW = ∫ P dV W = - ∫ Pext dV = Area under P-V Graph Expansion: W = -ve Compression: W = +ve
  • 17. Cyclic Process: P V Wnet = Area of shape(ie square in this case) enclosed -ve for clockwise (as in this case) +ve for anti-clockwise
  • 18. Isobaric(Δp=0): W= -Pext ΔV Isochoric(ΔV=0): W = 0 Vacuum(Free Expansion):Pext = 0 ⟹ W = 0 Isobaric and Isochoric processes:
  • 19. W = - ∫ Pext dV = - ∫ nRT dV/V = - nRT ln (V2/V1) = - 2.303 nRT log10 (V2/V1) = - 2.303 nRT log10 (P2/P1) = - 2.303 P1V1 log10 (V2/V1) = - 2.303 P2V2 log10 (V2/V1) = - 2.303 P1V1 log10 (P2/P1) = - 2.303 P2V2 log10 (V2/V1) Isothermal process