1. As shown in the figure below, Refrigerant 134a enters a condenser operating at steady state at 70 lbf/in2, 160 °F and is condensed to saturated liquid at 60 lbf/in on the outside of tubes through which cooling water flows. In passing through the tubes, the cooling water increases in temperature by 20 'F and experiences no significant pressure drop. Cooling water can be modeled as incompressible with v-0.0161 ft'/lb and c = 1 Btu/lb R. The mass flow rate of the refrigerant is 3100 lb/h. Neglecting kinetic and potential energy effects and ignoring heat transfer from the outside of the condenser, determine: (a) The volumetric flow rate of the entering cooling water, in gal/min (b) The rate of heat transfer, in Btu/h, to the cooling water from the condensing refrigerant (5 points) Refrigerant 134a P= 70 in. T= 160 F 3100 heh 7,-7,-20F-20R Reirigerant 134a [P-60 lbin V Saturated liquid

Elements Of Electromagnetics
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Author:Sadiku, Matthew N. O.
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1. As shown in the figure below, Refrigerant 134a enters a condenser operating at steady state
at 70 lbf/in2, 160 °F and is condensed to saturated liquid at 60 lbf/in on the outside of tubes
through which cooling water flows. In passing through the tubes, the cooling water increases
in temperature by 20 'F and experiences no significant pressure drop. Cooling water can be
modeled as incompressible with v-0.0161 ft'/lb and c = 1 Btu/lb R. The mass flow rate of
the refrigerant is 3100 lb/h. Neglecting kinetic and potential energy effects and ignoring heat
transfer from the outside of the condenser, determine:
(a) The volumetric flow rate of the entering cooling water, in gal/min
(b) The rate of heat transfer, in Btu/h, to the cooling water from the condensing refrigerant (5
points)
Refrigerant 134a
P= 70 in.
T= 160 F
3100 heh
7,-7,-20F-20R
Reirigerant 134a
[P-60 lbin
V Saturated liquid
Transcribed Image Text:1. As shown in the figure below, Refrigerant 134a enters a condenser operating at steady state at 70 lbf/in2, 160 °F and is condensed to saturated liquid at 60 lbf/in on the outside of tubes through which cooling water flows. In passing through the tubes, the cooling water increases in temperature by 20 'F and experiences no significant pressure drop. Cooling water can be modeled as incompressible with v-0.0161 ft'/lb and c = 1 Btu/lb R. The mass flow rate of the refrigerant is 3100 lb/h. Neglecting kinetic and potential energy effects and ignoring heat transfer from the outside of the condenser, determine: (a) The volumetric flow rate of the entering cooling water, in gal/min (b) The rate of heat transfer, in Btu/h, to the cooling water from the condensing refrigerant (5 points) Refrigerant 134a P= 70 in. T= 160 F 3100 heh 7,-7,-20F-20R Reirigerant 134a [P-60 lbin V Saturated liquid
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