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The volume of a gas is halved during an adiabatic compression that increases the pressure by...

The volume of a gas is halved during an adiabatic compression that increases the pressure by a factor of 2.5. What is the specific heat ratio?
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Answer #1
Concepts and reason

The concept used to solve this problem is the ideal gas equation in a reversible adiabatic process.

Use the ideal gas equation to calculate the specific heat ratio.

Fundamentals

Expression for the ideal gas equation in a reversible adiabatic process is,

PVn=constantP{V^n} = {\rm{constant}}

But here n=γn = \gamma , since the equation becomes,

PVγ=constantP{V^\gamma } = {\rm{constant}}

Here, pressure is PP , volume is VV , and the specific heat ratio is γ\gamma .

Expression for the relation between the initial pressure and volume to the final pressure and volume is,

PiViγ=PfVfγ{P_i}V_i^\gamma = {P_f}V_f^\gamma

Here, initial pressure is Pi{P_i} , initial volume is Vi{V_i} , final pressure is Pf{P_f} , final volume is Vf{V_f} and the specific heat ratio is γ\gamma .

The pressure is increased by a factor and volume is halved during the adiabatic process.

Expression for the relation between initial pressure and volume to final pressure and volume is,

PiViγ=PfVfγ{P_i}V_i^\gamma = {P_f}V_f^\gamma

The product of pressure and volume in an adiabatic process is constant.

Which means that initial pressure multiplied with initial volume is equal to final pressure multiplied with volume.

Expression for relation between initial pressure and volume to final pressure and volume is,

PiViγ=PfVfγ{P_i}V_i^\gamma = {P_f}V_f^\gamma

Substitute 2.5Pi2.5{P_i} for Pf{P_f} and 0.5Vi0.5{V_i} for Vf{V_f} .

PiViγ=(2.5Pi)(0.5Vi)γ{P_i}V_i^\gamma = \left( {2.5{P_i}} \right){\left( {0.5{V_i}} \right)^\gamma }

Rearrange the above relation.

Pi2.5Pi=(0.5Vi)ViyγPi2.5Pi=(0.5ViVi)γ12.5=(0.5)γ0.4=(0.5)γ\begin{array}{c}\\\frac{{{P_i}}}{{2.5{P_i}}} = {\frac{{\left( {0.5{V_i}} \right)}}{{V_i^y}}^\gamma }\\\\\frac{{{P_i}}}{{2.5{P_i}}} = {\left( {\frac{{0.5{V_i}}}{{{V_i}}}} \right)^\gamma }\\\\\frac{1}{{2.5}} = {\left( {0.5} \right)^\gamma }\\\\0.4 = {\left( {0.5} \right)^\gamma }\\\end{array}

Take natural logarithm on both sides,

ln(0.4)=ln(0.5)γγln(0.5)=ln(0.4)\begin{array}{c}\\\ln \left( {0.4} \right) = \ln {\left( {0.5} \right)^\gamma }\\\\\gamma \ln \left( {0.5} \right) = \ln \left( {0.4} \right)\\\end{array}

The specific heat ratio is,

γ=ln(0.4)ln(0.5)=0.9160.693=1.322\begin{array}{c}\\\gamma = \frac{{\ln \left( {0.4} \right)}}{{\ln \left( {0.5} \right)}}\\\\ = \frac{{ - 0.916}}{{ - 0.693}}\\\\ = 1.322\\\end{array}

Therefore, the specific heat ratio is γ=1.322\gamma = 1.322 .

Ans:

Thus, the specific heat ratio of the gas is γ=1.322{\bf{\gamma = 1}}{\bf{.322}} .

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