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Question 15.11: The following data are given for a lithium bromide–water sys......

The following data are given for a lithium bromide–water system of the type shown in Fig. 15-30: condensing temperature, 100 F; evaporating temperature, 40 F; temperature of strong solution leaving absorber, 100 F; temperature of strong solution entering generator, 180 F; and generator temperature, 200 F.

Saturated conditions exist for states 3, 4, 8, and 10. Pressure drop in components and lines is negligible. The system cooling capacity is 10 tons. Determine (a) the thermodynamic properties P, t, x, and i for all necessary state points, (b) the mass flow rate for each part of the system, (c) the system coefficient of performance, (d) the system refrigerating efficiency, and (e) the steam rate for the generator if saturated steam at 220 F is used.

15.30
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Parts (a) and (b) will be solved concurrently. Table 15-4 shows a tabulation of data. Properties of pure water were obtained from Table A-1, and solution properties were btained from Chart 5 in Appendix E. Note that Chart 5 expresses concentration in terms of the absorbent lithium bromide.

The high- and low-side pressures are found from the temperatures t_{8}  and  t_{10},  and  i_{8}  and   i_{10} are found in Table A-1. The enthalpy of the pure water vapor at state 7 may be computed by Eq. 3-19, since it behaves as an ideal gas at the low pressure. States 3 and 4 are saturated conditions and may be located on Chart 5 as shown in Fig. 15-33. Enthalpy and concentration values may then be read for states 3 and 4.

i_{\text{v}}  =  i_{g}  +  c_{p\text{v}}  t              (3-19)

For the evaporator

\dot{m}_{9}  =  \frac{\dot{q}_{e}}{i_{10}  –  i_{9}}  =  \frac{10 (200)}{1011}  =  1.98  lb/min

For the absorber

\dot{m}_{6}  =  \dot{m}_{10}  \frac{x_{1}  –  x_{10}}{x_{6}  –  x_{1}}  =  \frac{1.98 (0.60)}{0.05}  =  23.8  lb/min

\dot{m}_{1}  =  \dot{m}_{6}  +  \dot{m}_{10}  =  25.8  lb/min

For the generator

\dot{q}_{g}  =  \dot{m}_{4} i_{4}  +  \dot{m}_{7} i_{7}  –  \dot{m}_{3} i_{3}

=  23.8 (-27)  +  1.98 (1151)  –  25.8 (-35)

\dot{q}_{g}  =  2538  Btu/min

Neglecting the pump work,

COP  =  \frac{\dot{q}_{c}}{\dot{q}_{g}}  =  \frac{200(10)}{2538}  =  0.79

For a generator source temperature of 220 F and a refrigerated medium temperature of 45 F, and assuming an environment temperature of 100 F, the maximum COP becomes

(COP)_{max}  =  \frac{505(680  –  560)}{680 (560  –  505)}  =  1.62

and

\eta_{R}  =  \frac{0.79}{1.62}  =  0.49

Assuming saturated water at 220 F leaves the steam coil,

\dot{m}_{s}  =  \frac{60 \dot{q}_{g}}{i_{fg}}  =  \frac{60(2538)}{965}  =  158 lb/hr

Table 15-4 Properties and Flow Rates for Example 15-11
 

State

P,

mm/Hg

t,

F

x,

lb LiBr/lbm

i,

Btu/lbm

\dot{m},

lbm/min

1 6.3 100 0.6 _ 25.8
2 49.1 _ 0.6 _ 25.8
3 49.1 180 0.6 -35 25.8
4 49.1 200 0.65 -27 23.8
5 49.1 _ 0.65 _ 23.8
6 6.3 _ 0.65 _ 23.8
7 49.1 200 0 1151 1.98
8 49.1 100 0 68 1.98
9 6.3 40 0 68 1.98
10 6.3 40 0 1079 1.98
15.33

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