THERMODYNAMIC PROCESS OF PERFECT GAS: -
- 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
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
Fig.2 | Adiabatic process |
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.
- THROTTLING PROCESS: - When a perfect gas is expanded through aperture of minute dimension (Slightly open valve)
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