Isothermal reversible condensation

AI Thread Summary
In the discussion on isothermal reversible condensation of water, participants clarify the thermodynamic principles involved in the process. The change in internal energy (ΔU) is zero because the temperature remains constant, but the change in enthalpy (ΔH) is equal to the negative standard enthalpy of vaporization, indicating heat is released during condensation. The confusion arises regarding work (w), where participants debate whether it should be calculated using constant external pressure or a variable pressure due to the reversible nature of the process. It is established that for this scenario, the external pressure is indeed constant at 1 atm, aligning with standard conditions. Understanding which equations apply to liquids versus ideal gases is emphasized as crucial for solving such thermodynamic problems.
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Homework Statement



A sample of 1.00 mol H20(g) is condensed isothermally and reversibly
to liquid water at 100°C. The standard enthalpy of vaporization of water at
100°C is 40.656 kJ mol-1. Find w, q, change in internal energy, and change in enthalpy for this process.

Homework Equations




The Attempt at a Solution



So since this is an isothermal reversible compression, change in temperature is equal to 0, so change in internal energy should also be equal to 0.
Because deltaH = deltaU + delta(pV), and for an ideal gas pV = nRT so deltaH = 0 + delta(nRT) = 0, change in enthalpy should also be equal to 0.

HOWEVER the solutions were quite different. Apparently deltaH = -standard enthalpy of vapourization, q = deltaH, w = -(external pressure) x deltaV, and deltaU = q + w.

What am I missing here? Why are the changes in internal energy and enthalpy not zero if the change in temperature is zero?

I know this is probably a really basic thermodynamics question but I just don't get it!
 
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Liquid water is not an ideal gas.
 
okay, so what are the expressions for deltaU and deltaH for a liquid?
 
kido said:
okay, so what are the expressions for deltaU and deltaH for a liquid?

Exactly what is given in the answer: the change in enthalpy is the enthalpy of vaporization. Condensation releases heat, so this value is negative. And by definition, the change in energy is the enthalpy without the work performed during the process.
 
Okay, i understand that now, thanks. There's one more thing that i am having trouble understanding, though. In the solutions, it says that because the condensation is done isothermally and reversibly, the external pressure is constant at 1atm.
I thought the whole point of a reversible process was that the pressure was not constant? Shouldn't the expression for work be
w = -nRTln(Vf/Vi),
not w = -(external pressure)*(Vf-Vi)?
 
Reversibility doesn't imply anything about the pressure being constant or not constant. And work is always \int P(V)\,dV. For ideal gases at constant temperature this expression can be reduced to the other expression you give, but again, we're not dealing with an isolated ideal gas here.
 
Ah, I see. I really must learn which expressions apply only to ideal gases!
So because this question mentions the standard enthalpy of vaporization, the external pressure is at standard conditions, which is 1atm?
Thank you very much for your help.
 
I am having the same problems in this question. Not sure if I did it correct.
I said "Delta H = -Enthalpy of Vaporization"
"W=0" because the final state (liquid) does not alter volume
"Delta H = q " this is true for isothermal processes
"Delta U= q + W, W=0 so Delta U=q"

is this thought correct?
 
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