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P 6 – 26 The isothermal
compressibility of water is 50 x 10-6 atm-1 and cP
= 4.18 x 103 J kg-1 K-1. Other properties of water are given in the
previous problem. Calculate the work
done as the pressure on 1 g of water in a hydraulic press is increased
reversibly from 1 atm to 10,000 atm (a) isothermally, (b) adiabatically, (c)
Calculate the heat evolved in (a) the isothermal process. |
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Calculate
the work done as the pressure on 1 g of water in a hydraulic press is
increased reversibly from 1 atm to 10,000 atm (a) isothermally, |
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From
section 6-9 we are reminded that dv can be written as |
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So
work can be found from |
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Isothermal
reduces this to |
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From
problem 6-25, if we assume the temperature is 4°C, then v = 1 cm3
= 10-6 m3 |
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So
work per gram is |
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Calculate
the work done as the pressure on 1 g of water in a hydraulic press is
increased reversibly from 1 atm to 10,000 atm (b) adiabatically, |
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Again
work is found from |
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We
need to find dT for adiabatic, from eq (6-34) |
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But
β = 3 x 10-4 K-1 for water at 300 K, so |
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Compared
to dPs, we can ignore this term. So work can now be found from |
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We
now must replace k with ks = k/g |
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Eq
(6-12) gives us |
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So
cP = cv and g = 1 so ks = k, so the work adiabatically is the
same as the work isothermally. |
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(c)
Calculate the heat evolved in (a) the isothermal process. |
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Eq
(6-31) |
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Since
isothermal dT = 0 |
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Integrating |
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Thus
the heat evolved isothermally is |
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