What Are the Steps to Solve a Thermodynamics Piston Problem?

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SUMMARY

The discussion focuses on solving a thermodynamics problem involving a vertical cylinder with a piston containing air at an initial temperature of 285 K, pressure of 325 kPa, and volume of 0.425 m³. Key calculations include determining the specific heat at constant volume (CV), the mass of air using the ideal gas equation (n = PV/RT), and the energy input required to raise the temperature to 675 K under both isovolumetric and isobaric conditions. The relevant equations include Q = nCVΔT for constant volume and Q = nCPΔT - P(Vf - Vi) for constant pressure scenarios.

PREREQUISITES
  • Understanding of the ideal gas law (PV = nRT)
  • Knowledge of specific heat capacities (CV and CP)
  • Familiarity with thermodynamic processes (isovolumetric and isobaric)
  • Basic algebra for manipulating equations
NEXT STEPS
  • Learn about the derivation and application of the ideal gas law in thermodynamic problems
  • Study the differences between isovolumetric and isobaric processes in thermodynamics
  • Explore the concept of specific heat capacities and their significance in energy calculations
  • Investigate the first law of thermodynamics and its applications in real-world scenarios
USEFUL FOR

Students studying thermodynamics, engineers working with thermal systems, and anyone involved in energy calculations related to gases and pistons.

Denn
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Homework Statement


A vertical cylinder with a heavy piston contains air at 285 K. The initial pressure is 3.25 105 Pa, and the initial volume is 0.425 m3. Take the molar mass of air as 28.9 g/mol and assume
CV = 5/2R.

(a) Find the specific heat of air at constant volume in units of J/kg · °C.
J/kg · °C.

(b) Calculate the mass of the air in the cylinder.
kg

(c) Suppose the piston is held fixed. Find the energy input required to raise the temperature of the air to 675 K.
kJ

(d) Assume again the conditions of the initial state and assume the heavy piston is free to move. Find the energy input required to raise the temperature to 675 K.
kJ

Homework Equations


So far I've identified ill need to use these equations:

-Q=m*C*deltaT
-c=Q/m*deltaT
-W=-P(Vf-Vi) (For a isobaric process)
-Q=n*Cv*deltaT (For a gas with constant volume)
-Q=n*Cp*deltaT (For a gas with constant pressure)
-PV=nRT
- Cp-Cv=R

The Attempt at a Solution



To begin i equated the first and the second equation to recieve:
C=n*Cv/m

Mass is the unknown quantity and now I'm stuck.

If the piston is held in place then the volume is constant and the process is isovolumetric and therefore Eint=Q and does Q = n*Cv*deltaT?

If the piston is allowed to move freely then the process is isobaric and the Work = -P(Vf-Vi). Does Eint therefore = Q + W = n*Cp*deltaT - P(Vf-Vi) ?

Any help is greatly appreciated!

Thanks
 
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Denn said:

Homework Statement


A vertical cylinder with a heavy piston contains air at 285 K. The initial pressure is 3.25 105 Pa, and the initial volume is 0.425 m3. Take the molar mass of air as 28.9 g/mol and assume
CV = 5/2R.

(a) Find the specific heat of air at constant volume in units of J/kg · °C.
J/kg · °C.

(b) Calculate the mass of the air in the cylinder.
kg

(c) Suppose the piston is held fixed. Find the energy input required to raise the temperature of the air to 675 K.
kJ

(d) Assume again the conditions of the initial state and assume the heavy piston is free to move. Find the energy input required to raise the temperature to 675 K.
kJ

Homework Equations


So far I've identified ill need to use these equations:

-Q=m*C*deltaT
-c=Q/m*deltaT
-W=-P(Vf-Vi) (For a isobaric process)
-Q=n*Cv*deltaT (For a gas with constant volume)
-Q=n*Cp*deltaT (For a gas with constant pressure)
-PV=nRT
- Cp-Cv=R

The Attempt at a Solution



To begin i equated the first and the second equation to recieve:
C=n*Cv/m

Mass is the unknown quantity and now I'm stuck.
Is the initial pressure supposed to be 325 KPa?

You can calculate the mass from the number of moles, n. You can determine n simply by using the ideal gas equation: n = PV/RT
If the piston is held in place then the volume is constant and the process is isovolumetric and therefore Eint=Q and does Q = n*Cv*deltaT?
Yes. Isochoric = constant volume.

If the piston is allowed to move freely then the process is isobaric and the Work = -P(Vf-Vi). Does Eint therefore = Q + W = n*Cp*deltaT - P(Vf-Vi) ?
If P is constant, the heat flow is: \Delta Q = nC_p\Delta T. This takes into account the work that is done since Cp = Cv+R and PdV = nRdT. So in applying the first law for isobaric process:

\Delta Q = \Delta U + P\Delta V = nC_v\Delta T + nR\Delta T= n(C_v+R)\Delta T = nC_p\Delta T

AM
 

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