Title | GAS Power Cycles - Lecture notes 2 |
---|---|
Author | Mthobisi Calvin |
Course | Thermodynamics 3 |
Institution | Vaal University of Technology |
Pages | 11 |
File Size | 762.2 KB |
File Type | |
Total Downloads | 115 |
Total Views | 140 |
gas power cycle...
APPLIED THERMODYNAMICS II (EHATH3A/EHTTA3C GAS POWER CYCLES 1. Air-Standard Analysis • Air-Standard Analysis Air-standard analysis makes the following assumptions: • The working fluid is air, and is an ideal gas • Compression and expansion processes are adiabatic and reversible, so they are isentropic • Combustion will be treated as a heat transfer process from an external source • Exhaust transfers heat and does no work
• Cold-Air Standard The cold-air standard additionally assumes that the specific heats are constant. We use the specific heats at 27 ºC. The assumptions of the air-standard and cold-air standard analyses introduce some error, but allow simplified analysis of gas cycles. 2. Reciprocating Engine Terminology • Reciprocating Engine Terminology The position where the piston provides the minimum volume is top dead centre (TDC). The position where the piston provides the maximum volume is bottom dead centre (BDC). The bore is the inside diameter of the cylinder. The stroke is the distance of travel of the piston from BDC to TDC
• Reciprocating Engine Terminology The displacement is the volume equal to the stroke times the cross-sectional area:
The clearance volume is the volume between the cylinder head and the top of the piston when the piston is at top dead centre. The compression ratio is the ratio of the maximum volume (piston at BDC) to the minimum volume (piston at TDC). The intake valve lets air or an air-fuel mixture into the cylinder. The exhaust valve lets combustion products exit the cylinder • Reciprocating Engine Terminology A spark plug ignites the fuel-air mixture in spark ignition. The high temperature during compression ignites the fuel-air mixture in compression ignition. The mean effective pressure (MEP) is the ratio of the net work done during the cycle to the displacement
3. The Brayton Cycle The gas turbine is used in most aircrafts as well as some power plants.
It is a continuous flow engine: there is a constant flow of air into the engine and combustion products out of the engine.
The open-cycle gas turbine The top heat exchanger accounts for the energy input that would occur during combustion of the fuel. The lower heat exchanger emits the heat associated with the products of combustion and does no work.
The closed-cycle gas turbine
• The Efficiency of the Brayton Cycle The pressure ratio is
𝑃�2 is at the exit of the compressor, 𝑃�1 is at the entrance. The efficiency is:
• The Brayton Cycle with Regenerative Heating In the regenerative Brayton cycle, the exhaust gases are used to heat the air before it enters the combustion chamber using a regenerator.
• The Efficiency of the Regenerative Brayton Cycle The efficiency is:
The efficiency of the regenerative cycle will actually decrease as the pressure ratio increases
• The Brayton Cycle with Regeneration, Intercooling, and Reheat An intercooler reduces compressor work by cooling the air between compressor stages. A reheater increases turbine power output by heating the air in between turbine stages
• The Brayton Cycle with Regeneration, Intercooling, and Reheat Intercooling and reheat are only effective when combined with a regenerator. • The Turbojet Engine Perhaps the primary use of the gas turbine that operates on the Brayton cycle has been in the aircraft propulsion.
• The Turbojet Engine Operation of an turbojet engine.
4. The Combined Brayton-Rankine Cycle • Cogeneration Cycles The combined-cycle power plant is an example of cogeneration. The exhaust gases from the gas turbine are used to generate steam in boiler
•
Cogeneration Cycles The efficiency of an actual combined-cycle power plant may exceed 60%. This efficiency is possible because the secondary Rankine cycle recovers much of the rejected heat from the turbine.
• Gas Properties Properties of Air
Properties of Combustion Gas
R = 0.287 kJ/kg·K
R = 0.287 kJ/kg·K
CP = 1.003 kJ/kg·K k = 1.4
CP = 1.003 kJ/kg·K k = 1.4...