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

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 />

• U-Pipes in this two straight pipes are connected by a 180 turn at bottom<br />

• Concentric (coaxial) pipes<br />

3. THERMAL MODELING<br />

Thermodynamic analysis <strong>of</strong> a GSHP system is carried out initially in order to understand the performance <strong>of</strong><br />

individual components <strong>of</strong> the system. For this purpose First law <strong>of</strong> thermodynamic for open system is utilized<br />

to model the individual components. Then the energy flow analysis <strong>of</strong> each component is also studied in detailed<br />

to estimate the overall performance <strong>of</strong> GSHP system. The detail <strong>of</strong> thermodynamic modeling and energy analysis<br />

is discussed in the following section.<br />

For a general steady-state, steady flow process, the four balance equation, namely mass, energy balance<br />

equations are applied to ground source heat pump (GSHP) in order to find the heat input, the rate <strong>of</strong> mass <strong>of</strong> flow<br />

<strong>of</strong> refrigerant flowing into the circuit. Figure 3 show the schematic diagram <strong>of</strong> the GSHP considered for<br />

thermodynamic analysis. The GSHP system consists <strong>of</strong> compressor, condenser, Expansion Valve, Evaporator,<br />

Fan- Coil unit and ground heat exchanger. It is assumed that the flow is steady through every component <strong>of</strong> the<br />

GSHP system and heat loss is ignored. The governing equation for the individual Component <strong>of</strong> the system are<br />

derived as follow<br />

The mass balance equation can be expressed in the rate form as<br />

in= out ( 1 )<br />

Where is the mass flow rate, and the subscript is stand for inlet and outlet.<br />

in= out ( 2 )<br />

Energy balance equation can also be written more explicitly as<br />

Q + inh in = Ẁ + outh out ( 3 )<br />

Where, Q = Q net.in = Q in – Q out is the rate <strong>of</strong> net heat input Ẁ = Ẁ net, out = Ẁ out - Ẁ in is tge rate <strong>of</strong> net work output<br />

and h is the enthalpy per unit mass.<br />

The rate form <strong>of</strong> the entropy balance can be expressed as<br />

S in - S out + S gen =0………………………………………………(4)<br />

3.1 Compressor<br />

Figure 3. The Main Components and Schematic <strong>of</strong> the GSHP<br />

68

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