- #1
variation
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Some examples in textbook make me confused when these two works are discussed at the same time.
One of the works is the (mechanical) work in work-energy theorem:
[tex]
\Delta K = \sum_iW_i,
[/tex]
where [tex]K[/tex] is the kinetic energy and [tex]W_i[/tex] was the work done by the [tex]i[/tex]-th force.
The other is the (thermodynamical) work in the first law of thermodynamics:
[tex]
\Delta U = Q + W,
[/tex]
where [tex]U[/tex] is the internal energy of the system, [tex]Q[/tex] is the heat transfered, and [tex]W[/tex] is the work done on the system by surroundings.
Are the two works the same when we want to use work-energy theorem and the first law of thermodynamics at the same time?
Can anyone give some criterion to distinguish these two works ?
Thank you .
One of the works is the (mechanical) work in work-energy theorem:
[tex]
\Delta K = \sum_iW_i,
[/tex]
where [tex]K[/tex] is the kinetic energy and [tex]W_i[/tex] was the work done by the [tex]i[/tex]-th force.
The other is the (thermodynamical) work in the first law of thermodynamics:
[tex]
\Delta U = Q + W,
[/tex]
where [tex]U[/tex] is the internal energy of the system, [tex]Q[/tex] is the heat transfered, and [tex]W[/tex] is the work done on the system by surroundings.
Are the two works the same when we want to use work-energy theorem and the first law of thermodynamics at the same time?
Can anyone give some criterion to distinguish these two works ?
Thank you .