Cyclic processes and their effeciency, Carnot cycle Lecture

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Technology uses cyclic thermodynamic processes to describe the conversion of thermal energy to mechanical energy and vice versa.

During this process a medium undergoes periodically different changes of state, such as compression and expansion, evaporation and condensation, or heating and cooling over a period of time. In a cyclic process, the medium, after having undergone the different changes of state, goes back to its original state and can thus be reused repeatedly.

When a phase change occurs, more energy is converted than during simple heating or cooling. This means that phase change processes involve a higher energy density and require lower  differences in temperature.

Cyclic processes can be used in driving or driven machines. Driving machines convert thermal energy to mechanical energy, such as in steam power plants. Driven machines convert the supplied mechanical energy into thermal energy, like in a compression refrigeration system.


Suitable media are substances that remain in a permanent gaseous state during the cyclic process, such as air or helium, or substances that change their aggregate state during the process (phase change), like water, ammonia, fl uorocarbons, or CO2.

Representation of cyclic processes in state diagrams

A cyclic thermodynamic process can be illustrated clearly by what are known as state diagrams. The most commonly used state diagrams are:

     p-v diagram: pressure p against specifi c volume v, suitable for representing mechanical power. It is often used for reciprocating compressors and internal combustion engines with a purely gaseous working medium. Here, cyclic processes can be observed quite well because there is a fi xed relationship between volume change and time. The enclosed area is a measure for the mechanical work performed, also known as useful work.

     h-s diagram: enthalpy h against entropy s, for representation of steam turbine processes. It is used for water steam and is well suited as a tool for designing steam turbines.

     log p-h diagram: logarithmic representation of the pressure p against the specifi c enthalpy h, particularly well suited for cooling processes in refrigeration engineering, as heat fl uxes

can be read from the diagram directly as horizontal lines. For the vertical pressure scale, a logarithmic division is used, as this is a good way to represent phase limit curves.

T-s diagram: a plot of temperature T against entropy s, used for the representation of the thermodynamic conditions. The direction of the cyclic process indicates the type of system, driving or driven machine. If the cycle goes clockwise, the system is a driving machine, and if it goes counter-clockwise, it is a driven machine. In the clockwise direction, heat is absorbed at a high temperature and released at a low temperature. In the counter-clockwise direction, heat is absorbed at a low temperature and released at a high temperature. If the system is operated in the counter-clockwise direction, it is thus suitable as a heat pump or refrigeration machine. As in the p-v diagram, the enclosed area is a measure of the useful work performed.


Examples of cyclic thermodynamic processes

 

 

Type

Driving or driven machine

Working medium

Aggregate state

Steam power plant

driving

water

liquid/gaseous

Internal combustion engine

driving

air/combustion gas

gaseous

Gas turbine

driving

air/combustion gas

gaseous

Stirling engine

driving

air, helium

gaseous

ORC power plant

(Organic Rankine Cycle)

driving

fl uorocarbons, hydrocarbons

liquid/gaseous

Refrigeration machine

driven

fl uorocarbons, hydrocarbons, ammonia, etc.

liquid/gaseous

Stirling refrigeration system

driven

air, helium

gaseous

The following section presents some technically relevant cyclic processes with their diagrams.


 

Steam power plant

 

Gas turbine power plant

power plant. The working medium is water or water steam.                   stage expansion in a double shaft system.

1 – 2        the water is isobarically heated and evaporated in        1 – 2        polytropic compression of air to a pressure of                a steam boiler at a pressure of 22 bar                20 bar; the air has a temperature of 500°C at the 2 – 3 isobaric superheating of the steam to 300°C                    outlet of the compressor

3   – 4       polytropic expansion of the steam in the steam             2 – 3        isobaric heating of air to the inlet temperature

                  turbine to a pressure of 0,2 bar; mechanical energy                                   of 1000°C of the high-pressure turbine via injection

                  is released in the process                                                                         and combustion of fuel

Point 4 wet steam area: the wet steam content is now                           3 – 4         polytropic expansion in the high-pressure turbine

                 only 90%                                                                                                       that drives the compressor

4   – 5       condensation of the steam Point 5 in the transition to the power turbine the gas

5  

– 1       increase of the pressure to boiler pressure via the                         isobarically cools down slightly         condensate and feed water pump, the cyclic process 5 – 6       second expansion in the power turbine: the exhaust

                 is complete                                                                                                    gas exhausts and is not returned to the process

                                                                                                                                           again, which is why the process is known as an open

                                                                                                                                         gas turbine process; the process heat is released

 

 

Internal combustion engine

 

Refrigeration plant

bustion engine. In the case of the internal combustion engine, all changes of state take place in the same space: the cylinder. The changes of state occur one after the other.

     1 – 2        polytropic gas compression

Point 2 ignition with subsequent fuel combustion

medium is the fl uorohydrocarbon refrigerant R134a.

1   – 2       polytropic compression

2   – 3       isobaric cooling and condensation with 

                heat dissipation

                                                                                                                        3 – 4         isenthalpic expansion to evaporation pressure

idealised division of the combustion process into:

2   – 3       isochoric proportion of the combustion process            4 – 1        isobaric evaporation with heat absorption

3   – 4       isobaric proportion of the combustion process

After being superheated to a certain degree the refrigerant

4   – 5 polytropic (isentropic) expansion, in this phase the vapour is once again sucked in and compressed by the com usefull work results pressor at point 1. The cyclic process ends.

5   – 1       isochoric decompression and exchange of working

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