Thermodynamics- Vapour Power Cycles Flashcards
What are the impracticalities associated with a Carnot cycle within the saturation dome of a pure substance water?
Limiting the heat transfer processes to two-phase systems severely limits the maximum temperature that can be used in the cycle (must remain under critical point) which limits thermal efficiency (process 1-2). The turbine cannot handle steam with high moisture (low quality) as in process 2-3. Process 4-1 (isentropic compression) involves liquid-vapour mixture and it isn’t practical to design a compressor which handles two phases.
Why can’t a Carnot cycle be used for vapour power cycles starting above the saturation dome?
Requires isentropic compression to extremely high pressures and isothermal heat transfer at variable pressures.
How can the impracticalities of the Carnot cycle be eliminated for a vapour power cycle?
Superheating the steam in the boiler and condensing it completely in a condenser
Describe the Rankine cycle
The ideal cycle for vapour power plants. Doesn’t involve any internal irreversibilities. Has 4 steps of
1-2: Isentropic compression in a pump
2-3: Constant pressure heat addition in a boiler
3-4: Isentropic expansion in a turbine
4-1: Constant pressure heat rejection in a condenser
Describe the T-s graph of the ideal Rankine cycle
Has the normal saturation curve. Starts near bottom left on saturation curve. Moves vertically up to a new pressure on liquid side at state 2. Straight diagonal line to higher T and s point on curve. Horizontal line to other side of curve. Line curves upwards to state 3 on vapour side. Vertical line down to same temperature as state 1 (just inside saturation curve). Horizontal line back to state 1.
Describe what goes on in the ideal vapour power cycle
Water enters pump at state 1 as saturated liquid. Is compressed isentropically to operating pressure of boiler. Water temperature increases during this compression due to a slight increase in its v. Water enters boiler as compressed liquid at state 2 and leaves as superheated vapour at state 3. This enters the turbine where it expands isentropically and produces work by rotation the shaft connected to an electric generator. Pressure and T drop during this process to state 4 (high quality saturated liquid-vapour mixture) when it enters a condenser. Leaves as saturated liquid and enters pump at state 1.
What does the area enclosed on a T-s graph of the Rankine cycle represent?
The net work produced during the cycle
What can be steady-flow energy per unit mass equation for the Rankine cycle be reduced to?
(qin-qout)+(win-wout)=he-hi
This is because kinetic and potential energy changes usually small relative to work and heat transfer terms
Think e and i mean end and initial
Which types of energy change are 0 for each component of a Rankine cycle?
Pump: q=0
Boiler: w=0
Turbine: q=0
Condenser: w=0
What are the conservation of energy relations for each component in a Rankine cycle?
Pump: win=h2-h1 or win=v(P2-P1) Boiler: qin=h3-h2 Turbine: wout=h3-h4 Condenser: qout=h4-h1 All numbers are subscript and the works are for that specific component.
Formula for thermal efficiency of the Rankine cycle
ηth=wnet/qin=1-qout/qin
Uses wnet=qin-qout=work output of turbine-work input of pump
th, net, in and out subscript
How can the thermal efficiency of a Rankine cycle be interpreted using its T-s graph?
Ratio of area enclosed by the cycle on the T-s diagram to the area under the heat-addition process
Name two common sources of irreversibilities in a vapour power cycle
Fluid friction and heat loss to the surroundings
What does fluid friction mean for a vapour power cycle in practice?
Causes pressure drops in boiler, condenser (small) and piping between components. To compensate, water must be pumped to a sufficiently higher pressure than the ideal cycle calls for meaning a larger pump and a larger work input to the pump.
What does heat loss from the steam to the surroundings mean in practice for a vapour power cycle?
To maintain the same level of net work output, more heat needs to be transferred to the steam in the boiler to compensate for the undesired heat losses. Therefore cycle efficiency decreases.
How does the T-s graph of a real vapour power cycle deviate from that of the ideal Rankine cycle if nothing is done to compensate for irreversibilities?
1-2: vertical line becomes diagonally right so state 2 further up
2-3: horizontal line becomes diagonally down and curve upwards has same gradient as before so state 3 further right
3-4: vertical line becomes diagonally right so state 4 not under saturation curve and is higher
4-1: horizontal line becomes diagonally down, bit curvy from state 4 to saturation curve
How does the T-s graph of a real vapour power cycle deviate from that of the ideal Rankine cycle for irreversibilities of pump and turbine alone?
Only 2 differences in processes.
1-2: vertical line becomes diagonally right so state 2 is higher
3-4: vertical line becomes diagonally right from 3 to saturation curve, then curves right once under saturation curve to T at state 1 so state 4 is further right