Chapter 6: Problem 148
For most biological processes, \(\Delta H \approx \Delta U\). Explain.
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Chapter 6: Problem 148
For most biological processes, \(\Delta H \approx \Delta U\). Explain.
These are the key concepts you need to understand to accurately answer the question.
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Describe the interconversions of forms of energy occurring in these processes: (a) You throw a softball up into the air and catch it. (b) You switch on a flashlight. (c) You ride the ski lift to the top of the hill and then ski down. (d) You strike a match and let it burn down.
Given the thermochemical equations: $$\begin{array}{c}\mathrm{Br}_{2}(l)+\mathrm{F}_{2}(g) \longrightarrow 2 \mathrm{BrF}(g) \\ \Delta H^{\circ}=-188 \mathrm{~kJ} / \mathrm{mol} \\ \mathrm{Br}_{2}(l)+3 \mathrm{~F}_{2}(g) \longrightarrow 2 \mathrm{BrF}_{3}(g) \\\ \Delta H^{\circ}=-768 \mathrm{~kJ} / \mathrm{mol}\end{array} $$calculate the \(\Delta H_{\mathrm{rxn}}^{\circ}\) for the reaction$$\operatorname{BrF}(g)+\mathrm{F}_{2}(g) \longrightarrow \operatorname{BrF}_{3}(g)$$
In general, compounds with negative \(\Delta H_{i}^{\circ}\) values are more stable than those with positive \(\Delta H_{i}^{\circ}\) values. \(\mathrm{H}_{2} \mathrm{O}_{2}(l)\) has a negative \(\Delta H_{\mathrm{f}}^{\circ}\) (see Table 6.4 ). Why, then, does \(\mathrm{H}_{2} \mathrm{O}_{2}(l)\) have a tendency to decompose to \(\mathrm{H}_{2} \mathrm{O}(l)\) and \(\mathrm{O}_{2}(g) ?\)
A quantity of \(2.00 \times 10^{2} \mathrm{~mL}\) of \(0.862 \mathrm{MHCl}\) is mixed with an equal volume of \(0.431 M \mathrm{Ba}(\mathrm{OH})_{2}\) in a constant-pressure calorimeter of negligible heat capacity. The initial temperature of the \(\mathrm{HCl}\) and \(\mathrm{Ba}(\mathrm{OH})_{2}\) solutions is the same at \(20.48^{\circ} \mathrm{C}\), For the process $$\mathrm{H}^{+}(a q)+\mathrm{OH}^{-}(a q) \longrightarrow \mathrm{H}_{2} \mathrm{O}(l)$$ the heat of neutralization is \(-56.2 \mathrm{~kJ} / \mathrm{mol}\). What is the final temperature of the mixed solution?
A quantity of 0.020 mole of a gas initially at \(0.050 \mathrm{~L}\) and \(20^{\circ} \mathrm{C}\) undergoes a constant-temperature expansion until its volume is \(0.50 \mathrm{~L}\). Calculate the work done (in joules) by the gas if it expands (a) against a vacuum and (b) against a constant pressure of 0.20 atm. (c) If the gas in (b) is allowed to expand unchecked until its pressure is equal to the external pressure, what would its final volume be before it stopped expanding, and what would be the work done?
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