Work done isothermal, adiabatic ideal gas

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SUMMARY

The discussion focuses on calculating the work done on one mole of an ideal gas during isothermal and adiabatic processes. For isothermal compression from 5L to 2L, the work done is expressed as W_isothermal = 7.618T, where T is the temperature in Kelvin. The initial temperature T_i is calculated as 60.92 K using the ideal gas law. The participants emphasize the necessity of knowing the specific heat ratio (γ = C_p/C_v) to compute the work done during adiabatic compression accurately.

PREREQUISITES
  • Understanding of ideal gas laws and equations
  • Familiarity with isothermal and adiabatic processes
  • Knowledge of thermodynamic concepts such as work and heat transfer
  • Basic calculus for integration in thermodynamic equations
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  • Learn about the derivation of the ideal gas law and its applications
  • Study the concept of specific heat capacities (C_p and C_v) for different types of gases
  • Explore the calculations of work done in adiabatic processes using the formula W = (P_fV_f - P_iV_i)/(γ - 1)
  • Investigate the implications of monatomic vs. diatomic gases on thermodynamic calculations
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Samuelriesterer
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Problem statement, work done, and relevant equations:

One mole of ideal gas is initially at 1 atm and has a volume of 5L.

a) Calculate the work done on the gas during an isothermal, reversible compression to a volume of 2L.

##W_isothermal = - \int_{v_i}^{v_f} p dv = - \int_{v_I}^{v_f} \frac{nRT}{V} dV = -nRT \int_{v_I}^{v_f} \frac{1}{V} dV = -nRT ln \frac{V_I}{V_f} = -(1 mol)(8.314 \frac{J}{molK})T ln \frac{.005 m^3}{.002 m^3} = 7.618T##

b) Calculate the work done during a reversible adiabatic compression to 2L.

##P_i = \frac{nRT_I}{V} → T_i = \frac{V_I P_i}{nR} = \frac{(.005 m^3)(101300 Pa)}{(1 mol)(8.314 \frac{J}{molK})} = 60.92 K##

I think I'm a little stuck here because the problem statement does not give me whether its a monatomic or diatomic gas in order to get the ##\frac{C_p}{C_v}## value. Is there something I'm not seeing?

c) What are the final pressures for (a) and (b)?
 
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Samuelriesterer said:
a) Calculate the work done on the gas during an isothermal, reversible compression to a volume of 2L.

##W_isothermal = - \int_{v_i}^{v_f} p dv = - \int_{v_I}^{v_f} \frac{nRT}{V} dV = -nRT \int_{v_I}^{v_f} \frac{1}{V} dV = -nRT ln \frac{V_I}{V_f} = -(1 mol)(8.314 \frac{J}{molK})T ln \frac{.005 m^3}{.002 m^3} = 7.618T##

b) Calculate the work done during a reversible adiabatic compression to 2L.

##P_i = \frac{nRT_I}{V} → T_i = \frac{V_I P_i}{nR} = \frac{(.005 m^3)(101300 Pa)}{(1 mol)(8.314 \frac{J}{molK})} = 60.92 K##

I think I'm a little stuck here because the problem statement does not give me whether its a monatomic or diatomic gas in order to get the ##\frac{C_p}{C_v}## value. Is there something I'm not seeing?
The first part is correct and your determination of ##T_i## is correct, assuming you have done the arithmetic properly. You do need to know the value for ##\gamma = \frac{C_p}{C_v}## in order to calculate the adiabatic work and the final pressure and temperature (applying the adiabatic condition). I would suggest that you assume a true ideal gas (monatomic).

AM
 

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