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CHAPTER 4. THERMODYNAMICS: THE FIRST LAW

CHAPTER 4. THERMODYNAMICS: THE FIRST LAW

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4-8<br />

Therefore,<br />

dH = dU + P dV. ext<br />

at constant pressure.<br />

For liquids and solids, (PV) is usually very small (typically - 0.1% of U), and hence H<br />

. U. For ideal gases,<br />

H = U + PV = U + nRT,<br />

so<br />

H = U + nRT<br />

at constant temperature. It should be noted that n is the change in the number of moles of gas.<br />

Exercise:<br />

A total of 885.7 kJ of heat is evolved in the reaction<br />

CH + 2O ! CO + 2H O<br />

4(g) 2(g) 2(g) 2 (l)<br />

o<br />

Carried out at fixed volume and 25 C. Calculate U and H for this reaction.<br />

U = q = !885.7 kJ<br />

H = U + (PV) = U + nRT; n = 1 ! 3 = !2<br />

!3<br />

H = !885.7 ! 2(8.314)(298)x10 = !890.6 kJ<br />

Exercise:<br />

A 10.0 g sample of benzene at its boiling temperature (353.2 K) is placed in contact<br />

with a resistance heater. It evaporates when 3942 J of heat have been produced by<br />

the heater. Calculate the molar enthalpy change and the the molar internal energy<br />

change. (Neglect the volume of the liquid).<br />

This is a constant pressure process in which H = U + (PV) = q.<br />

n = 10.0 g C H x 1 mol C H /78 g C H = 0.128 mol<br />

6 6 6 6 6 6<br />

H = 3942 J/0.128 mol = 30797 J/mol = 30.8 kJ/mol<br />

m<br />

U = H ! (PV ! PV )/n = H ! RT<br />

m m gas liq m

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