- #1
PFuser1232
- 479
- 20
The first law can be stated as ΔU = Q + W and we adopt a sign convention as follows, if the system under study does work then W is negative and if work is done on the system W is positive.
Now consider the example of a gas expanding against a constant external pressure p. W would be negative as the gas does work, and from a classical mechanics approach this can be explained by imagining the external force from pressure moving through a displacement that is in an opposite direction to the force, so the work done ON the system is negative. But picture this; what if while the gas expands, i pull the piston so my force is in the same direction as the force by the gas, does that mean work done on the system is positive although the gas is clearly doing work? Would that violate the first law of thermodynamics?
Now consider the example of a gas expanding against a constant external pressure p. W would be negative as the gas does work, and from a classical mechanics approach this can be explained by imagining the external force from pressure moving through a displacement that is in an opposite direction to the force, so the work done ON the system is negative. But picture this; what if while the gas expands, i pull the piston so my force is in the same direction as the force by the gas, does that mean work done on the system is positive although the gas is clearly doing work? Would that violate the first law of thermodynamics?