First law of thermodynamics

First law for isobaric processes

π‘‘π‘Š=βˆ’π‘π‘‘π‘‰π‘‘π‘„=𝑛𝐢𝑝𝑑𝑇

where

  • 𝐢𝑝 :Jβ‹…molβˆ’1β‹…Kβˆ’1 is the molar specific heat for gas of constant pressure

For ideal gas

By the Ideal gas law, if 𝑝 is constant,

𝑑𝑉=𝑛𝑅𝑝𝑑𝑇

and therefore

π‘‘π‘Š=βˆ’π‘›π‘…π‘‘π‘‡π‘‘π‘ˆ=𝑑𝑄+π‘‘π‘Š=π‘›πΆπ‘π‘‘π‘‡βˆ’π‘…π‘‘π‘‡

which, using the equation from First law for isovolumetric processes, shows

𝑛𝐢𝑉𝑑𝑇=π‘›πΆπ‘π‘‘π‘‡βˆ’π‘…π‘‘π‘‡πΆπ‘‰=πΆπ‘βˆ’π‘…

Monatomic

As a consequence of the above, for a monatomic ideal gas

𝐢𝑝=52𝑅

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