1. What is the purpose of turbine?
A turbine converts energy in a flowing fluid into useful mechanical shaft power. In a gas-turbine engine, the compressor raises the air pressure, the combustor adds fuel and produces hot gas at approximately constant pressure, and the turbine extracts part of that gas energy as the flow expands through the turbine stages. The resulting shaft power drives the compressor and accessories. The remaining gas then continues to the exhaust nozzle, where its remaining energy can contribute to jet velocity and thrust.
In plain English, the turbine takes energy from the hot gas leaving the combustor and turns that energy into shaft rotation. In the engine flow path, ambient air enters the inlet, the compressor raises its pressure and temperature, fuel is added and burned in the combustor, and the resulting hot gas passes through the turbine. The turbine blades extract energy from that gas and turn the rotor. Through the common shaft, this mechanical power drives the compressor and engine accessories. The gas then continues downstream toward the exhaust nozzle.
For a simple thermodynamic model, define a control volume around the turbine and use a sign convention in which shaft work leaving the turbine is positive. Under steady-state operation, if the turbine is approximately adiabatic and changes in kinetic and potential energy are negligible, the first-law energy balance reduces to:
Ẇ_t ≈ ṁ(h_in − h_out)
where Ẇ_t is turbine shaft power in watts (W), ṁ is mass flow rate in kilograms per second (kg/s), and h_in and h_out are the inlet and outlet specific enthalpies in joules per kilogram (J/kg). A turbine that produces positive shaft work therefore has h_in > h_out. The gas loses stagnation enthalpy as work is extracted, and in a normal gas-turbine expansion its pressure and temperature also decrease.
This simplified relation matches the physical purpose of the turbine: convert part of the hot-gas energy into rotational mechanical work. In a gas-turbine engine, that work is primarily required to keep the compressor operating. The turbine is therefore essential to sustaining the engine cycle; it is not simply another component that directly produces nozzle thrust.
The simplified model has limits. A real turbine is not perfectly adiabatic or reversible, and actual performance is affected by aerodynamic losses, turbine cooling flow, leakage, pressure losses, and mechanical losses. If those effects are important, the full steady-flow energy balance and measured or calculated component efficiencies should be used instead of the simplified equation.
A useful design tradeoff is how much energy the turbine extracts. It must extract enough work to satisfy the compressor and accessory power demand. However, extracting more energy lowers the energy remaining in the gas downstream, which can reduce the energy available to the exhaust nozzle. The required turbine work therefore has to be consistent with the overall engine-cycle objective.
- Are we discussing a gas-turbine or jet-engine turbine specifically, or turbines in general?
- Would you like only the conceptual purpose, or should I also explain the control-volume energy balance?
- Should I discuss how the turbine's work is matched to the compressor and exhaust-nozzle requirements?
I would explain the engine from left to right. Air enters the compressor, which raises its pressure and temperature. Fuel is then burned with the compressed air in the combustor, approximately at constant pressure. The resulting hot gas expands through the turbine, where part of its energy is converted into rotational shaft work. That shaft power drives the compressor and accessories. For a steady, approximately adiabatic turbine with negligible kinetic- and potential-energy changes, the relationship is Ẇ_t ≈ ṁ(h_in − h_out). I would then check that h_in is greater than h_out, that the turbine power is consistent with the required compressor and accessory load, and that the remaining gas energy is physically reasonable for the downstream nozzle. Real turbines require additional consideration of efficiency, cooling flow, leakage, and aerodynamic losses.
- Define a control volume around the turbine and identify the inlet, outlet, and rotating shaft.
- State the operating condition as steady state unless transient behavior is specifically requested.
- Use the sign convention that shaft work leaving the turbine is positive.
- Start with the steady-flow first-law energy balance.
- For the simplified model, assume the turbine is approximately adiabatic and neglect changes in kinetic and potential energy.
- Reduce the balance to Ẇ_t ≈ ṁ(h_in − h_out).
- Interpret the result physically: the fluid loses enthalpy and the turbine produces shaft work.
- Connect that shaft work to the gas-turbine system: it drives the compressor and accessories.
- Check physical feasibility by confirming h_in > h_out for positive turbine work and that the extracted work is consistent with the required shaft load.
- If higher accuracy is required, include cooling flow, heat transfer, kinetic-energy changes, leakage, mechanical losses, and turbine efficiency.
The important engineering tradeoff is how much energy the turbine removes from the hot gas. More extraction can provide more shaft power for the compressor or other loads, but it leaves less energy available downstream for the exhaust nozzle. Real turbines also lose performance through aerodynamic losses, cooling requirements, leakage, and mechanical losses, so the ideal enthalpy-drop relation is a useful first model rather than a complete prediction of hardware performance.
Interviewers ask this to check whether you understand the energy flow through a gas-turbine engine, can distinguish the turbine from the compressor, combustor, and nozzle, and can connect the turbine's physical purpose to a correct control-volume energy balance.
Common mistakes include confusing the turbine with the compressor, saying that the turbine's primary purpose is to produce exhaust thrust directly, forgetting that the turbine and compressor are mechanically linked by a shaft, using the enthalpy relation without stating steady and approximately adiabatic assumptions, or using the wrong sign so that a turbine producing power appears to increase the fluid enthalpy.
Explain the energy path in one sequence: compressor raises air pressure, combustor adds heat through fuel combustion, turbine extracts part of the hot-gas energy as shaft work, and the shaft drives the compressor. Then add Ẇ_t ≈ ṁ(h_in − h_out) with its assumptions. That gives both the intuitive purpose and the thermodynamic reasoning.

