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OCTOBER 19-20, 2012 - YMCA University of Science & Technology

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Proceedings <strong>of</strong> the National Conference on<br />

Trends and Advances in Mechanical Engineering,<br />

<strong>YMCA</strong> <strong>University</strong> <strong>of</strong> <strong>Science</strong> & <strong>Technology</strong>, Faridabad, Haryana, Oct <strong>19</strong>-<strong>20</strong>, <strong>20</strong>12<br />

2.OPTIMIZATION ANALYSIS :<br />

2.1 Optimization for Endoreversible Heat Pump system<br />

Taking the finite thermal capacity <strong>of</strong> reservoir makes the cycle realistic, conceptual heat pump cycle. The<br />

schematic model and T-S diagram <strong>of</strong> an endoreversible heat pump system, coupled to a variable temperature heat<br />

reservoir are shown in Fig 1. The system operates steadily between two variable reservoirs, i.e. between heat<br />

source <strong>of</strong> temperature range (T L1 -T L2 ) and heat sink <strong>of</strong> temperature range (T H2 -T H1 ). The working fluid in the<br />

heat pump, exchanges heat with the reservoirs, has two constant temperature limits T y and T x . Assuming that the<br />

heat exchangers are counter flow, and the heat conductance (heat transfer co-efficient and area product) <strong>of</strong> hot<br />

and cold side heat exchangers are U H A H and U L A L , respectively.<br />

From the heat transfer theory, the steady rate <strong>of</strong> heat flow (Q L ) from heat source to the working fluid <strong>of</strong> heat<br />

pump and the rate (Q H ) at which the heat is rejected from the working fluid <strong>of</strong> heat pump to the heat sink in the<br />

heat exchangers, during the two isothermal processes are, respectively, given by:<br />

Q H<br />

T H<br />

1/U H A H<br />

T X<br />

T H2<br />

T H1<br />

3<br />

2<br />

T X<br />

Q H<br />

Heat Pump<br />

Q L<br />

Q L<br />

T Y<br />

T L<br />

W<br />

T X<br />

T L1<br />

TL2<br />

T Y 4<br />

1/U L A L<br />

1<br />

Fig 1 Endo-reversible Carnot heat pump model and its T-S diagram<br />

Q L = U L A L (LMTD) L = m L C pL (T L1 – T L2 ) (1)<br />

Q H = U H A H (LMTD) H = m H C pH (T H2 – T H1 ) (2)<br />

Where U L and U H are the overall heat transfer coefficients on evaporator and condenser side; and A L , A H are the<br />

heat transfer area <strong>of</strong> the heat exchangers on evaporator and condenser side, respectively.<br />

LMTD is the logarithmic mean temperature difference and is defined as<br />

(LMTD) L = {(T L1 - T Y ) – (T L2 - T Y )} / ln {(T L1 - T Y ) / (T L2 - T Y )} (3)<br />

(LMTD) H = {(T X – T H1 ) – (T X – T H2 )} / ln {(T X – T H1 ) / (T X – T H2 )} (4)<br />

Using above equations, the following expressions are obtained<br />

T L2 = T Y + (T L1 - T Y ) exp (-U L A L / m L C pL ) (5)<br />

T H2 = T X - (T X – T H1 ) exp (-U H A H / m H C pH ) (6)<br />

Further, Eq. (1) - (6) gives<br />

Q L = C L ε L (T L1 - T Y ) (7)<br />

Q H = C H ε H (T X – T H1 ) (8)<br />

On rearranging,<br />

C L = Q L / ε L (T L1 - T Y ) (9)<br />

Where,<br />

C L = m L C pL (10)<br />

ε L = 1 - exp (-U L A L / m L C pL ) (11)<br />

and,<br />

C H = Q H / ε H (T X – T H1 ) (12)<br />

Where,<br />

C H = m H C pH (13)<br />

ε H = 1 - exp (-U H A H / m H C pH ) (14)<br />

29

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