Solution:
W = integral of p dV.
If we are working with an ideal gas, then
p ="\\dfrac{nRT}{V}" and
W = integral of nRT "\\dfrac{dV}{V}"= nRT ln("\\dfrac{V_{2}}{V_{1}}").
If we are not working with an ideal gas, we will have to supply more information.
Another possible answer is W = Q (because there is no internal energy change), but that's probably not what they're after.
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