24.11.2012 Views

Space Grant Consortium - University of Wisconsin - Green Bay

Space Grant Consortium - University of Wisconsin - Green Bay

Space Grant Consortium - University of Wisconsin - Green Bay

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

The enthalpy (h3) <strong>of</strong> the 2 nd stage fluid entering the precooling evaporator is calculated using:<br />

( amb, nd , nd<br />

high )<br />

h = enthalpy T P y<br />

(7)<br />

3 ,2 2<br />

The ratio <strong>of</strong> the mass flow rate in the 1 st to the mass flow rate in the 2 nd stage (MR) is defined as:<br />

MR = m� m�<br />

(8)<br />

st nd<br />

1 2<br />

and is computed using an energy balance on the precooling evaporator:<br />

MR = h −h h − h<br />

(9)<br />

( ) ( )<br />

3 4 8 11<br />

The rate <strong>of</strong> precooling heat transfer as well as all subsequent energy transfer rates are computed<br />

on a per unit <strong>of</strong> 2 nd stage mass flow rate basis.<br />

Q� m� = MR h −h<br />

(10)<br />

pc<br />

2 nd<br />

( )<br />

8 11<br />

The precooling heat exchanger is divided into a number ( N pc ) <strong>of</strong> small heat exchangers, as<br />

shown in FIGURE 2(a), where each section transfers an equal fraction (1/Npc) <strong>of</strong> the total<br />

precooling load. Dividing the heat exchanger into equal heat transfer segments rather than equal<br />

physical sizes facilitates direct computation <strong>of</strong> the enthalpy distribution in the heat exchangers<br />

and significantly improves computation speed and convergence. The first heat exchanger section<br />

is located at the hot end <strong>of</strong> the precooling evaporator and is shown in FIGURE 2(b). The<br />

enthalpy <strong>of</strong> the 1 st stage working fluid leaving the precooling evaporator is equal to the enthalpy<br />

<strong>of</strong> the 1 st stage fluid at the first node <strong>of</strong> the heat exchanger.<br />

h = h<br />

(11)<br />

st<br />

1 , pc,0<br />

The enthalpy <strong>of</strong> the mixture entering the precooling evaporator is equal to the enthalpy for the<br />

mixture at the first node <strong>of</strong> the heat exchanger.<br />

h2 nd, pc,0<br />

= h3<br />

(12)<br />

The enthalpies <strong>of</strong> the hot and cold exit streams at the interface <strong>of</strong> each segment are computed<br />

using an energy balance.<br />

heat exchanger<br />

section index - i<br />

1<br />

2<br />

3<br />

N pc -1<br />

N pc<br />

h h<br />

st<br />

1 , pc,0<br />

h h<br />

= 8 nd<br />

2 , pc,0<br />

3<br />

.<br />

.<br />

h = h<br />

heat exchanger<br />

node index - i<br />

0<br />

1<br />

2<br />

3<br />

h = h<br />

N pc -2<br />

N pc -1<br />

N pc<br />

st =<br />

1 , pc, N 11 nd<br />

4<br />

pc 2 , pc, N pc<br />

8<br />

1st <strong>of</strong> N differential segments <strong>of</strong> HX<br />

h st = h<br />

1 , pc,0<br />

8<br />

Q�<br />

pc<br />

m�nd 2<br />

1<br />

Npc<br />

h nd = h<br />

2 , pc,0<br />

3<br />

Q�<br />

1<br />

h st = h st −<br />

1 , pc,1 1 , pc,0<br />

m N MR<br />

Q�<br />

pc 1<br />

= −<br />

m� N<br />

pc<br />

h nd h nd<br />

� 2 , pc,1 2 , pc,0<br />

nd<br />

2 pc<br />

(a) (b)<br />

FIGURE 2. a) Precooling heat exchanger divided into Npc sections and (Npc + 1) nodes. b) First differential heat<br />

exchanger element.<br />

( )<br />

h = h −Q m N MR<br />

� � i = 1…Npc (13)<br />

st st nd<br />

1 , pc, i 1 , pc, i−1<br />

pc 2 pc<br />

32<br />

nd<br />

2<br />

pc

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!