using indicator diagrams Flashcards
otto cycle
the theoretical cycle for a four stroke petrol engine
what condition do theoretical indicator diagrams in both petrol and diesel engines assume
- same gas is taken continuously around the cycle
- pure air
- adiabatic constant of 1.4 (y thing)
- pressure and temperature changes are instantaneous
- heat source is external
- engine is frictionless
processes in the theoretical cycle for four stroke engines
- A
- assumed gas is compressed adiabatically
- no heat transferred
- B
- heat is supplied whilst volume is kept constant
- C
- the gas is allowed to cool adiabatically
- D
- the system is cooled at constant volume
processin the theoretical cycle for a four stroke diesel engine
- A
- gas is adiabatically compressed
- B
- then heat is supplies
- this time pressure is kept constant
- C
- the gas is allowed to cool adiabatically
- D
- then the system is cooled at a constant volume
What are the main differences between theoretical and real-life diagram
- corners of theoretical diagrams are not rounded
- assumed that the same air is used continuously
- real engines, these corners are rounded as the inlet and exhaust valves take time to open and close
- in real, heating doesn’t take place at a constant volume (process b)
- increase in pressure and temperature would have to be instantaneous to do this, or the piston would have to pause
- theoretical model doesnt include small amount of negative work caused by the loop between the exhaust and induction lines because it assumes the same air cycles around the system continuously
- engines have an internal heat source, not external
- temperature rise is not as large as in the theoretical model because the fuel used to heat the gas is never completely burned
- so you can never get the max energy out of it
- theoretical engines acheive higher pressure
- energy is needed to overcome friction caused by moving parts
- net work done always less than a theoeretical engine
- area inside loop is smaller
types of engien efficiency
- mechanical efficiency
- affected by the energy lost through moving parts
- = brake power / indicated power
- thermal efficeiny
- describes how well heat ernergy transferred into work
- = indicated power / input power
- ovarall efficeincy
- = break power / input power
why is all heat not transferred to work
some heat always ends up increasing the temp of th engine
why must engines objey 2nd law?
- if engine temp reaches that of the heat source, then no heat flows and no work is done
- no engine can operate using only 1st law
- have to obey second law
- heat engines operate between a heat source and a heat sink
what would happen if an engine could work from just the first law
- all heat energy supplies could be transferred to useful work
How are engines never efficient
- heat energy transferred to the engine from the heat source is QH
- some of this energy is converted to useful work, W
- however, some of this energy (QC) must be transferred to a heat sink, which has a lower temp (TC) than the heat source
WHat are the reason the real heat engines effieciencies are lower than their theoretical max
- frictional forces inside engine
- fuel does’nt burn entirely
- energy needed to move internal components
How is waste heat reused in CHP plants
- maximise efficiency, as much of the input energy must be trasnferred usefully
- engines are very ineffeicent
- waste heat trasnferred to surroudnigs
- combines heat and power plants try to limit energy waste by using this heat for other purposes
- e.g. heating houses near yb