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Mathematics 18 Online
ganeshie8 (ganeshie8):

Suppose I have some gas confined in a cylinder with a movable piston as shown. I add some heat \(Q\) keeping the pressure constant. The volume changes by \(\Delta V\) and the temperature by \(\Delta T\). Next, keeping that volume constant, I remove the previously added heat \(Q\). What would be the change in temperature ? Options : 1) \(\Delta T\) 2) \(\gt \Delta T\) 3) \(\lt \Delta T\)

ganeshie8 (ganeshie8):

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ganeshie8 (ganeshie8):

let me know if the question is ambiguous...

Parth (parthkohli):

\[Q=\underbrace{p\Delta V}_{\text{as work}}+ \underbrace{nC_v \Delta T}_{\text{as internal energy}}\]Next, we remove \(Q\).\[-Q = -nC_v \Delta T'\]Well, this certainly seems to answer the question.

Parth (parthkohli):

In the second one, there is no work - only change in internal energy.

ganeshie8 (ganeshie8):

I think that shows the work done by the system(gas) is positive

Parth (parthkohli):

Here, we see that the decrease in temperature is way more than what it increased by earlier.

Parth (parthkohli):

\[nC_v \Delta T' = p\Delta V + nC_v \Delta T\]\[|\Delta T' | > |\Delta T|\]

ganeshie8 (ganeshie8):

that means \(\Delta T\) is not same in both the steps ?

ganeshie8 (ganeshie8):

Ohk gotcha !

Parth (parthkohli):

No, it is not because we're using two different processes.

ganeshie8 (ganeshie8):

the quantity \(Q\) does not uniquely determine the change in temperature of one \(mol\) of gas then ?

Parth (parthkohli):

In a constant-volume process, it does.

ganeshie8 (ganeshie8):

we're keeping pressure constant when adding heat and keeping volume constant when removing heat

Miracrown (miracrown):

\[PV = nRT\] http://hyperphysics.phy-astr.gsu.edu/hbase/kinetic/idegas.html

Miracrown (miracrown):

There is also one more thing we need:' the 1st law of thermodynamics

Parth (parthkohli):

oh nice, it also determines the constant-pressure\[p\Delta V = nR\Delta T \]

ganeshie8 (ganeshie8):

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