Rankine Reheat Cycle
Split expansion into two turbine stages with heat addition between them
Difficulty
Advanced
Read time
6 min
Review status
Needs review
Concept sketch
Rankine Reheat Cycle
Illustrative model, not experimental data
Overview
A reheat Rankine cycle sends steam back for heating between high- and low-pressure turbine stages. Reheat can reduce moisture at the final turbine exit and changes both the work output and the heat-input budget.
How to read it
- Identify both turbine stages and the intermediate reheat pressure.
- Read heat addition at both boiler and reheater.
- Compare exit quality and efficiency separately.
When to use it
- Understanding why a steam plant includes a reheater.
- Checking the energy balance of a two-stage expansion.
Add two states to the basic loop
Keep states 1 and 2 at the pump inlet and outlet, and 3 at the high-pressure turbine inlet. Expansion ends at 4, reheating raises temperature to 5 at an intermediate pressure, and the low-pressure turbine exhaust is state 6.
Count both heat inputs
The boiler and reheater both draw energy from the heat source. Omitting reheater heat inflates the apparent efficiency.
Count both expansions and the pump
Add the work of both turbine stages and subtract the pump input. Use isentropic expansions only for the ideal model; real turbine efficiencies change the exit states.
Separate moisture benefits from efficiency claims
Reheating normally makes the final exhaust drier at a comparable final pressure. Its effect on efficiency depends on the chosen reheat pressure and temperatures; adding a reheater is not an unconditional efficiency guarantee. Check wet-region quality using appropriate water properties.
Worked example
Use illustrative enthalpies h₁ = 200, h₂ = 210, h₃ = 3400, h₄ = 2900, h₅ = 3500, h₆ = 2400 kJ/kg. Evaluate the energy balance without inferring steam states from these values.
1.Sum boiler and reheater heat input.
2.Sum turbine work and subtract pump work.
3.Check efficiency and heat rejection.
The illustrative balance gives 42.0% efficiency, with 3790 − 2200 = 1590 kJ/kg of net work.