Applying first law of thermo to a closed spring piston

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SUMMARY

This discussion focuses on applying the first law of thermodynamics to a closed spring piston system containing 0.5 kg of saturated vapor water at 120ºC. Key calculations include determining the final temperature, which is approximately 875ºC, the change in internal energy (ΔU) of 638.18 kJ, the work done against the spring (20.7 kJ), and the heat transfer (Q) of 617.475 kJ. The calculations utilize steam tables, the linear spring equation (F=kx), and the work integral W=∫ PdV to derive results, confirming the system transitions to a superheated gas state.

PREREQUISITES
  • Understanding of the first law of thermodynamics (ΔU=Q+W)
  • Familiarity with steam tables for saturated and superheated water
  • Knowledge of linear spring mechanics (F=kx)
  • Ability to perform integration for work calculations (W=∫ PdV)
NEXT STEPS
  • Study the properties of superheated steam and its applications in thermodynamic systems
  • Learn advanced integration techniques for calculating work done in non-linear systems
  • Explore the use of MATLAB or Python for simulating thermodynamic processes
  • Investigate the impact of varying spring constants on system behavior in thermodynamic applications
USEFUL FOR

Mechanical engineers, thermodynamics students, and professionals working with steam systems or energy transfer processes will benefit from this discussion.

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Homework Statement


A cylinder having a piston restrained by a linear spring (of spring constant 15 kN/m) contains 0.5 kg of saturated vapor water at 120ºC. Heat is transferred to the water causing piston to rise. If the piston’s cross sectional area is 0.05 m2 and the pressure varies linearly with volume until a final pressure of 500 kPa is reached,

1-Find the final temperature in the cylinder.

2-Calculate the amount of heat transfer.

3-Calculate the change in the internal energy of water.

4-Calculate the work is done against the spring.

5-Sketch the process on a T-v phase diagram.

Homework Equations


ΔU=Q+W
W=∫ PdV
F=kx , linear spring displacement equation
v=V/m
u=U/m

The Attempt at a Solution



So I'd like some fresh opinions to just verify that my approaches are sensible and I correctly understand everything here. Firstly - I'm imagining this system initially as a "saturated vapor of 100% steam quality".

Finding the final temperature

Using the given temperature I look in the steam tables for saturated water and find a specific volume of vg=.891 m3/kg. I multiply this by the mass
.5 kg to get an initial volume of .4459 m3. I then use the final pressure
and area of the piston face (to find force) with the spring equation to find that the spring is compressed by 1.666m. This times the piston area gives a newly added volume of .529 m3. I add this to the original volume to find new total volume. I find the new specific volume, and
look in the steam tables to verify that it is greater than saturation specific
volume of gas at the new final temperature, confirming the system ends
up as a superheated gas. I look in the appropriate steam table to locate
this new specific volume and final pressure, finding that the temperature is approximately 875 C after some extrapolation.

Finding the change in Internal Energy ΔU
Going back to the steam table for the initial state, I find that the specific internal energy ug (since it's 100% gas), is 2529.24 KJ/kg. Using the
mass, I find an initial internal energy U1 of 1264.6 KJ. Using the data
for the final state found earlier in the superheated region, I find a new specific internal energy of 3805.7 KJ/kg. Using the constant mass,
I find a final internal energy U2 of 1902.8 KJ. The change in internal
energy ΔU is therefore 638.18 KJ.


Finding the amount of Work done
I make a line graph of Pressure vs Volume, plotting the initial and final
states. I found the initial pressure by looking at the saturated steam
tables, finding it to be 198.5 KPa. Using the listed equation for finding
Work, I understand that the Work is equal to the area under the curve of
P vs V. However, because I don't have two endpoints and the function
is linear, instead of determining the function relating P and V and integrating it I just segment the area under the curve into a triangle and a
rectangle. I find the area of each and sum them, coming out to a Work of
20.7 KJ.
It's positive because the system has expanded and done work
against its surroundings. (left out all the numbers for sake of brevity/clarity)

Finding the heat transfer Q
To find Q, I rearrange the first law of thermodynamics to find that
Q=ΔU-W. Then simply use the values of ΔU and W from earlier to find
a Q of 617.475 KJ.

To sum up - I expected energy change, work, and heat transfer to be positive as the system underwent a large increase in pressure while increasing in volume. These numbers make sense to me, at least as far as their signs. If you see any glaring issues with my approach to the problem please let me know. Any and all advice is appreciated, thank you.
 
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I got a work of 29.1973 KJ

Area Under Curve=0.5(P1+P2)(V2-V1)=(0.5)(0.529-0.4454)(500-198.5)=29.1973 KJ
 
RyanFrancis said:
I got a work of 29.1973 KJ

Area Under Curve=0.5(P1+P2)(V2-V1)=(0.5)(0.529-0.4454)(500-198.5)=29.1973 KJ

I think you're right. I think since I set the baseline of my pressure axis at 100 KPa, I used 98.5 as the height of the rectangle instead of 198.5. Thanks for catching that mistake!
 

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