Hello forumers, I have some questions on Thermal Physics III.
There is this question where a situation is given and I need to fill in the boxes (delta U, Q, and W) with -, + or 0.
1) Pan filled with room temperature water over a hot stove. System: Water in pan
My Q is +, W is - , but I don't know how to find delta U.
2) Hot water in kettle vaporizing into water vapour as it reached its boiling point. System: Water originally in kettle
My Q is +, W is - , again I don't know how to find delta U.
Another side question. If something happens rapidly means the Q is 0? e.g. Rapidly pumping up a bicycle tyre - system: air in pump, and air quickly leaking out of a balloon - system: Air originally in balloon.
Thank you.
Hi,
The water at room temperature will increase on a hot stove, so internal energy will increase.
Water undergoes a change of phase from liquid to vapour. For this to happen, there has to be an increase in molecular energy to overcome the attraction that held the molecules together in the liquid state. Thus, internal energy must increase.
Thanks.
Cheers,
Wen Shih
Hi,
We may assume that pumping a tyre is an adiabatic change.
The laws of thermodynamics associated with the hand pump is not straightforward and much information is lacking in your description. This article may help to shed some light:
http://www.physics.princeton.edu/~mcdonald/examples/tirepump.pdf
Thanks.
Cheers,
Wen Shih
@Han chiang
The question depends on what type of gas it is. Yes, it is ideal gas, but is it monatomic or diatomic or what...3/2 is only for monatomic. 5/2 for diatomic and etc etc.
Be careful of using delta U = 3/2 delta NkT or the likes....it contains a lot of assumption such as monatomic ideal gas and all. Go back to basic formula first such as First Law of Thermodynamics (delta U = Q + W) .
Hi,
If I am not wrong, delta U = Q + W only apply for ideal gas.
But assuming can be used in the following case,
1) Heat supplied water, Q +ve, and common sense tells me temp of water increase, change in U increase, which means W -ve, and work down by system must be less than heat supplied for change in U to be +ve.
2) Change in state, means gain in PE and hence gain in U, for same KE. Gas expand so work done by gas, W -ve. Heat given to gas to change in state, Q +ve.
For adiabatic process, think must have either condition:
1. thermal insulator (no heat can enter or leave the system)
2. process done very quickly ( reason being process too fast for any significant heat exchange, no time for heat to enter or leave the gas)
Hope it helps. Do correct me if i am wrong.
Hi,
Warm welcome to Kouer78 and thanks for your reply :)
The first law of thermodynamics can be applied to other systems.
In Giancoli's book, the first law is applied to human metabolism.
Thanks.
Cheers,
Wen Shih
Ok I get it now. Thank you.
Another question: There are 3 different paths, abd, acd and ad whereby a system consisting of 4 moles of gas can undergoes from point a to d. Note that path ad is an isothermal curve of temperature T.
At a, P = 100000Pa, V = 0.5 m^3
At b, P = 100000Pa, V = 0.2 m^3
At c, P = 250000Pa, V = 0.5 m^3
At d, P = 250000Pa, V = 0.2m ^3
I need to fill up delta U, Q and W. So if I want to find Wabd, I use Wd - Wa correct or not? For delta Uabd, I also use Ud - Ua. Somehow it feels abit weird...
Hi,
a to b: Isobaric process
Work done on the gas = P x (delta V) = (1 x 10^5) x 0.3 = 3 x 10^4 J
b to d: Isovolumetric process
No work is done, since delta V = 0.
a to d: Isothermal process
No change in internal energy, since delta T = 0.
Hence, by the first law of thermodynamics, we have
0 = Q + 3 x 10^4 => Q = -3 x 10^4 J.
Thanks.
Cheers,
Wen Shih
Wow, I missed a lot of interesting Q&A in this thread :)
Hi eagle,
Welcome back :)
Cheers,
Wen Shih
Now I know, U is a state function. So to find delta Uxyz, I can just use final minus initial. But to find Wxyz, I need to look under the PV graph right? Alamak ideal gas and graph abit confusing leh...
Can you help me check my answer for Wacd also? My Wacd is 75000J.
Thank you.
Hi,
7.5 x 10^4 J is correct! Good effort!
Cheers,
Wen Shih