available energy ,irreversibility,exchargy

636 views 10 slides Aug 18, 2018
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available energy ,irreversibility,exchargy


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Available Energy ,Exergy and Irreversibility Prepared by :- sagar paneliya (17MSE011) Thermodynamics & Heat Transfer

The second law of thermodynamics tells us that it is not possible to convert all the heat absorbed by a system into work . Suppose a certain quantity of energy Q as heat can be received from a body at temperature T . The maximum work can be obtained by operating a Carnot engine (reversible engine) using the body at T as the source and the ambient atmosphere at T  as the sink .

Where   s is the entropy of the body supplying the energy as heat.   The Carnot cycle and the available energy is shown in figure.       The area 1-2-3-4 represents the available energy.  

Unavailable energy available energy s s 1 T 1 T Maximum work = {Q s – T (s 1 -s )} Actual work = {Q s - Q r } {dS=dQ/T Q=T ( S )}

IRREVERSIBILITY The actual work is always less than of idealized reversible work and the difference between this two work is called irreversibility. I= W max – W actual For non flow process = when system exchange heat with only environment. I= {Q s – T (s 1 -s )} – (Q s – Q r )} = T (s 1 -s ) + Q r =T ( S) system + T0( S) surround =T {( S) system + ( S) surround } I = T ( S) univ

For steady flow process:- I= W max – W actual H=Q-W B=Q-H (Q=T(S1-S2))

Exergy Useful work Upper limit on the amount of work a device can deliver without violating any thermodynamic law.

A system at a given state can attain a new state through work and heat interactions with its surroundings. Since the exergy value associated with the new state would generally differ from the value at the initial state. The change in exergy of a system during a process would not necessarily equal the net exergy transferred, for exergy would be destroyed if irreversibility were present within the system during the process.

Note that exergy is a property, and the value of a property does not change unless the state changes . If the state of system or the state of the environment do not change, the exergy does not change . Therefore, the exergy change of a system is zero if the state of the system or the environment does not change during the process. For example, the exergy change of steady flow devices such as nozzles, compressors, turbines, pumps, and heat exchangers in a given environment is zero during steady operation . The exergy of a closed system is either positive or zero. It is never negative.

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