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Chapter 13 | 703

It can also be expressed in the rate form as

(13–55)

where W

.
min,inis the minimum power input required to separate a solution that
approaches at a rate of (or ) into its compo-
nents. The work of separation per unit mass of mixture can be determined
from , where Mmis the apparent molar mass of the
mixture.
The minimum work relations above are for complete separation of the
components in the mixture. The required work input will be less if the exit-
ing streams are not pure. The reversible work for incomplete separation can
be determined by calculating the minimum separation work for the incoming
mixture and the minimum separation works for the outgoing mixtures, and
then taking their difference.

Reversible Mixing Processes
The mixing processes that occur naturally are irreversible, and all the work
potential is wasted during such processes. For example, when the fresh water
from a river mixes with the saline water in an ocean, an opportunity to pro-
duce work is lost. If this mixing is done reversibly (through the use of semi-
permeable membranes, for example) some work can be produced. The
maximum amount of work that can be produced during a mixing process is
equal to the minimum amount of work input needed for the corresponding
separation process (Fig. 13–22). That is,

(13–56)

Therefore, the minimum work input relations given above for separation can
also be used to determine the maximum work output for mixing.
The minimum work input relations are independent of any hardware or
process. Therefore, the relations developed above are applicable to any sepa-
ration process regardless of actual hardware, system, or process, and can be
used for a wide range of separation processes including the desalination of
sea or brackish water.

Second-Law Efficiency
The second-law efficiency is a measure of how closely a process approxi-
mates a corresponding reversible process, and it indicates the range available
for potential improvements. Noting that the second-law efficiency ranges
from 0 for a totally irreversible process to 100 percent for a totally reversible
process, the second-law efficiency for separation and mixing processes can
be defined as

(13–57)

where W

.
act,inis the actual power input (or exergy consumption) of the separa-
tion plant and W

.
act,outis the actual power produced during mixing. Note that

hII,separation

W

#
min,in
W

#
act,in



wmin,in
wact,in

¬and¬hII,mixing


W

#
act,out
W

#
max,out



wact,out
wmax,out

Wmax,out,mixingWmin,in,separation

wmin,inwmin,in>Mm

m

#
mN

#
N mMm kg>s

#
m kmol>s

W

#

min,inRuT (^0) a
i
N



i ln yiN



mRuT (^0) a
i
yi ln yi¬¬ 1 kW 2
Mixing
chamber
A
B
(a) Mixing
(b) Separation
A + B
mixture
A + B
mixture
yA
yB
A
B
yA
yB
Separation
unit
Wmax,out = 5 kJ/kg mixture
Wmax,in = 5 kJ/kg mixture
FIGURE 13–22
Under reversible conditions, the work
consumed during separation is equal
to the work produced during the
reverse process of mixing.
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