Here we want to vaporize water at room temperature, which will require more heat than at .
Heat flow is a path function, so we can separate this into specific steps. All of this is done at constant pressure, so the heat flow is equal to the enthalpy, a state function, and the order of these steps doesn't matter.
We set a "boiling point" at , and thus have two steps:
1. Heat from to
2. Vaporize at
Step 1 would be a simple heating at constant pressure:
where
m is mass in g ,
is the specific heat capacity at constant atmospheric pressure in
ΔT is the change in temperature until the phase change temperature.
In this case we specify
Step 2 would be vaporization at constant pressure again, but at a CONSTANT, lower temperature than usual.Recall that
at constant pressure (provided they have the same units).
Thus, we just have:
where,
n is number of moles of water
is heat of vaporization in
T is the temperature at which this phase change occurs.
(Answer)
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