Thermodynamics piston-cylinder closed system

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SUMMARY

The discussion focuses on a thermodynamics problem involving an insulated piston-cylinder device containing 5 L of saturated liquid water at a constant pressure of 175 kPa. A current of 8 A flows for 45 minutes through a resistor, and the paddle-wheel work amounts to 400 kJ, leading to the evaporation of half the liquid. The voltage of the source is to be determined using the equation Welectric = VIΔt, while enthalpy values are derived from saturated water tables. The process is illustrated on a P-v diagram with respect to saturation lines.

PREREQUISITES
  • Understanding of thermodynamic principles, specifically the first law of thermodynamics.
  • Familiarity with saturated liquid properties and the use of saturated water tables.
  • Knowledge of electrical work calculations, particularly the formula Welectric = VIΔt.
  • Ability to interpret and construct P-v diagrams in thermodynamic processes.
NEXT STEPS
  • Learn how to apply the first law of thermodynamics to closed systems.
  • Study the use of saturated water tables for determining enthalpy values.
  • Explore the lever rule for calculating phase changes in thermodynamic systems.
  • Investigate the construction and interpretation of P-v diagrams for various thermodynamic processes.
USEFUL FOR

Students and professionals in mechanical engineering, particularly those specializing in thermodynamics, as well as anyone involved in energy systems and heat transfer analysis.

Andrew Pierce
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Homework Statement


An insulated piston-cylinder device contains 5 L of saturated liquid water at a constant pressure of 175 kPa. Water is stirred by a paddle wheel while a current of 8 A flows for 45 min through a resistor placed in the water, If one-half of the liquid is evaporated during this constant pressure process and the paddle -wheel work amounts to 400 kJ, determine the voltage of the source. Also, show the process on a P-v diagram with respect to saturation lines.

ElBL8rY.jpg


Homework Equations


ΔE = Ein - Eout
Welectric = VIΔt
if ΔP = 0, ΔH = m(h2 - h1)
ΔH = ΔU + Wboundary

The Attempt at a Solution


V = 5 L
m = 5 kg (by conversion)
P = 175 kPa
I = 8 A
Δt = 45*60 sec = 2700

Assuming that KE, and PE = 0,
ΔE = ΔU

Also since it is insulated we are assuming that the heat lost is 0

We + Wsh - Wboundary = ΔU
We + Wsh = ΔU + Wboundary
We + Wsh = ΔH
We + Wsh = m(h2 - h1)

Here is where I get lost. I know that we can find h1 from the saturated water tables
h1 = 487.01 kj/kg (at Psat = 175 kPa)
I'm confused as to where the second enthalpy value comes from since our state has constant P.

Also the P-v should look something like this I believe:

Bg1l7tO.jpg
 

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Andrew Pierce said:

Homework Statement


An insulated piston-cylinder device contains 5 L of saturated liquid water at a constant pressure of 175 kPa. Water is stirred by a paddle wheel while a current of 8 A flows for 45 min through a resistor placed in the water, If one-half of the liquid is evaporated during this constant pressure process and the paddle -wheel work amounts to 400 kJ, determine the voltage of the source. Also, show the process on a P-v diagram with respect to saturation lines.

ElBL8rY.jpg


Homework Equations


ΔE = Ein - Eout
Welectric = VIΔt
if ΔP = 0, ΔH = m(h2 - h1)
ΔH = ΔU + Wboundary

The Attempt at a Solution


V = 5 L
m = 5 kg (by conversion)
P = 175 kPa
I = 8 A
Δt = 45*60 sec = 2700

Assuming that KE, and PE = 0,
ΔE = ΔU

Also since it is insulated we are assuming that the heat lost is 0

We + Wsh - Wboundary = ΔU
We + Wsh = ΔU + Wboundary
We + Wsh = ΔH
We + Wsh = m(h2 - h1)

Here is where I get lost. I know that we can find h1 from the saturated water tables
h1 = 487.01 kj/kg (at Psat = 175 kPa)
I'm confused as to where the second enthalpy value comes from since our state has constant P.

Also the P-v should look something like this I believe:

Bg1l7tO.jpg
If you are using the saturation tables, you can get ##h_2## using the lever rule, or equivalently, as ##h_2=h_1+\Delta h_{vap}/2##.

Regarding the P-V diagram, your result is correct.
 

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