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For a simple compressible system, $v, s, p$ and $T$ are specific volume, specific entropy, pressure and temperature, respectively. As per Maxwell’s relations, $\big( \frac{\partial v}{\partial s} \big) _p$ is equal to

  1. $\big( \frac{\partial s}{\partial T} \big) _p \\$
  2. $\big( \frac{\partial p}{\partial v} \big) _T \\$
  3. $ – \big( \frac{\partial T}{\partial v} \big) _p \\$
  4. $\big( \frac{\partial T}{\partial p} \big) _s$
in Thermodynamics by (21.2k points) 4 64 208
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