calculus_jy
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I would like to know if someone here can help sort out my confusion...
It is easy to derive that
dU=TdS-pdV (no particle exchange)
Then enthalpy H=U+pV
will imply dH=TdS+Vdp
That means under a constant temperature (dT=0) and constant pressure (dp=0) situation
dH=TdS>(=) dQ
Why is it then that if we look at C_6 H_{12} +6O_2 + 6O_2\rightarrow O_2+6H_2O
\Delta H=-2803kJ/mol
\Delta G=-2879kJ/mol
T\Delta S=77.2 kJ/mol
(all above data are obtained at constant temperature and pressure)
now WHy is it that \Delta H =/= T\Delta S...
but that \Delta G= \Delta H- T\Delta S which i know will hold generally but should reduce to \Delta G= 0 under (dT=0, dp=0) when no other work done excluding expansion work...
I thought that \Delta H should be the heat flow in a constant temperature and pressure process...
but in this case why is the heat flow T\Delta S=77.2 kJ/mol instead...
It is easy to derive that
dU=TdS-pdV (no particle exchange)
Then enthalpy H=U+pV
will imply dH=TdS+Vdp
That means under a constant temperature (dT=0) and constant pressure (dp=0) situation
dH=TdS>(=) dQ
Why is it then that if we look at C_6 H_{12} +6O_2 + 6O_2\rightarrow O_2+6H_2O
\Delta H=-2803kJ/mol
\Delta G=-2879kJ/mol
T\Delta S=77.2 kJ/mol
(all above data are obtained at constant temperature and pressure)
now WHy is it that \Delta H =/= T\Delta S...
but that \Delta G= \Delta H- T\Delta S which i know will hold generally but should reduce to \Delta G= 0 under (dT=0, dp=0) when no other work done excluding expansion work...
I thought that \Delta H should be the heat flow in a constant temperature and pressure process...
but in this case why is the heat flow T\Delta S=77.2 kJ/mol instead...
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