তাপগতীয় প্রক্রিয়া

When an ideal gas at pressure p, temperature T and volume V is isothermally compressed to V/n, its pressure becomes pi\displaystyle p_i. If the gas is compressed adiabatically to Vn\displaystyle \frac{V}{n}, its pressure becomes pa\displaystyle p_a. The ratio pi/pa\displaystyle p_i/p_a is (γ=CpCV)\displaystyle \left( \gamma = \frac{C_p}{C_V} \right)

হানি নাটস

For isothermal process,
pV=\displaystyle pV= constant.
Therefore piVi=pV\displaystyle p_iV_i = pV
or piVn=pV\displaystyle p_i \frac{V}{n} = pV
or pi=np\displaystyle p_i =np .....(i)
For adiabatic process, pVγ=\displaystyle pV^{\gamma} = constant.
Therefore
pa(Va)γ=pVγ\displaystyle p_a(V_a)^{\gamma} = pV^{\gamma}
or pa(Van)γ=pVγ\displaystyle p_a \left( \frac{V_a}{n} \right)^{\gamma} = pV^{\gamma}
or pa=nγp\displaystyle p_a= n^{\gamma} p
From Eqs. (i) and (ii), we get
pipa=nnγ=n(1γ)\displaystyle \frac{p_i}{p_a} = \frac{n}{n^\gamma} = n^{(1- \gamma)}

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