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If ∆Q is the heat supplied to a gas so that the internal energy of the system increases by ∆U, then the work done ∆W by the gas is equal to: ∆Q – ∆U ∆Q + ∆U ∆Q x ∆U ∆U/∆Q
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this is the law of conservation of energy as it applies to the study thermodynamics it yields the first law of thermodunamics: ∆U = ∆Q - ∆W change in internal energy of system = heat added to system - work done BY system you can fiddle about with that to get your answer.....
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