THERMODYNAMIC PROCESS OF PERFECT GAS: -

  1. CONSTANT VOLUME PROCESS / ISOCHORIC PROCESS: - [n = ∞ ]

    Follows Law – Gay-Lussac Law

P ∝ T (When V = Constant)

    Heat Transferred Q1-2 = (U2 – U1) = mCv (T2 –T1)

    Work Done dW = 0

    Entropy Change dS = Cvln (T2 / T1)

 

    2. CONSTANT PRESSURE PROCESS / ISOBARIC PROCESS: - [n = 0]

    Follows Law – Charles’ Law

V ∝ T (When P = Constant)

    Heat Transferred Q1-2 = mCp (T2 –T1)

    Work Done dW = P (V2 – V1)

                              = mR (T2 –T1)

    Internal energy dE = dQ – dW

                              =mCp (T2 –T1) – mR (T2 –T1)

                              = mCp (T2 –T1) – m (Cp – Cv) (T2 –T1)

                              = m Cv (T2 – T1)

    Entropy Change dS = Cvln (T2 / T1)


3. CONSTANT TEMPERATURE PROCESS / ISOTHERMAL PROCESS: -[n = 1]

    Follows Law – Boyel’s Law

        P ∝ 1 / V (When T = Constant)

        PV = CONSTANT.

    Internal energy (dE) = 0

Isothermal Process
Fig.1 | Isothermal Process

                dQ = dE + dW

                = dW      [dE = 0]

                = P. dV

P1V1 = PV

P = P 1V1 / V 

= (P1V1 / V). dV
= P1V1 ln(V2/V1)

 

            Heat Transferred dQ = dW = P1V1 ln(V2/V1) OR P1V1 ln(P2 / P1)

            Entropy Change dS = R ln(V2/V1)


    4. ADIABATIC PROCESS OR ISENTROPIC PROCESS: - [n =γ ]

            Follows Law

PVγ = CONSTANT.

            Heat Transferred dQ = 0

            Internal energy (dE) = - dW

                            dW = P. dV

                                  = (P1V1γ / Vγ).dV

Adiabatic Process
Fig.2 | Adiabatic process




Entropy Changes dS = 0


        5. POLYTROPIC PROCESS: - [n =γ ]

                Follows Law

PVn = CONSTANT.

                 Heat Transferred Q1-2 = Cn (T2 – T1)

                                             = Cv (γ – n/ γ – 1) (T2 - T1)

                                             = (γ – n/ γ – 1) X Work Done

 

                Work Done (W1-2) = (P1V1 – P2V2) / n-1

                Internal energy (dE) = mCv (T2 - T1

                Entropy Change dS =  











  • FREE EXPANSION PROCESS: - When a fluid is allowed to expand suddenly in to a vacuum chamber through an orifice of  large dimension.
 Q1-2 = 0 ;      W1-2 = 0 ;    & dU = 0 

  • THROTTLING PROCESS: - When a perfect gas is expanded through aperture of minute dimension (Slightly open valve)
Enthalpy remains constant.

 Q1-2 = 0 ;      W1-2 = 0 ;    & dU = 0