Exergy in Thermal Engineering

Exergy — also called availability or available energy — is the maximum useful work obtainable from a system as it comes into equilibrium with a specified reference environment through reversible processes. Unlike energy, which is conserved, exergy is destroyed by irreversibilities and is zero at equilibrium with the environment.

Definition and concept

Energy vs exergy

Reference environment

Types of exergy

Key formulas

Closed system (physical exergy)

e_ph = (u - u0) + p0(v - v0) - T0(s - s0)
    

Where u, v, s are specific internal energy, volume, and entropy at system state; subscript 0 denotes environment state.

Flow exergy (steady-flow devices)

ψ = (h - h0) - T0(s - s0) + (V² - V0²)/2 + g(z - z0)
    

h = specific enthalpy, V = velocity, z = elevation.

Exergy of heat transfer at boundary temperature Tb

Ex_Q = Q * (1 - T0/Tb)
    

Exergy of work

Ex_W = W   (for mechanical work fully convertible to work)
    

Gouy–Stodola theorem

Exergy destruction is proportional to entropy generation:

Ex_dest = T0 * S_gen
  

This links Second Law irreversibility directly to lost work potential.

Worked examples

Example 1: Physical exergy of steam

Given: Steam at 2 MPa, 400°C; environment T0 = 25°C, p0 = 100 kPa.

From steam tables: h = 3230.1 kJ/kg, s = 6.769 kJ/(kg·K); h0 = 104.83 kJ/kg, s0 = 0.3672 kJ/(kg·K).

Flow exergy: ψ = (3230.1 − 104.83) − 298.15 × (6.769 − 0.3672) ≈ 3125.27 − 1916.6 ≈ 1208.7 kJ/kg.

Example 2: Exergy of heat transfer

Given: Q = 500 kJ at Tb = 500 K, T0 = 300 K.

ExQ = 500 × (1 − 300/500) = 500 × 0.4 = 200 kJ.

Applications

Exergy destruction and losses

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