CEE 230 quiz 1 practice problems solutions
docx
keyboard_arrow_up
School
University of Michigan *
*We aren’t endorsed by this school
Course
230
Subject
Communications
Date
Feb 20, 2024
Type
docx
Pages
16
Uploaded by AdmiralTiger4006
CEE 230: Quiz 1 Study Problems
NOTE: Question 1 is much harder and longer than the other problems that are provided.
Question 1:
This will incorporate a lot of different skills required to create T-V and P-V diagrams, analyze the state of a substance, and use the property Tables. This question can be LONG and very CHALLENGING, but it should be good practice!
Given:
A system consisting of 1 kg of H
2
O undergoes a power cycle of the following processes.
Process 1-2: Constant Pressure Heating at 10 bar from saturated vapor
Process 2-3: Constant-Volume Cooling to P
3
=
5
¯
¿
, T
3
=
160
℃
Process 3-4: Isothermal compression with Q
3
−
4
=−
815.8
kJ
Process 4-1: Constant volume heating
Find:
Create a T-V diagram and P-V diagram for the cycle of processes and find the Pressure, specific volume (v), and specific internal energy (u) at each state in the table below:
State 1
State 2
State 3
State 4
Unit
Pressure
[bar]
Specific Volume, v
[m
3
/kg]
Specific Internal Energy, u
[kJ/kg]
Start with T-V diagram basics:
Process 1-2: Constant Pressure Heating
at 10 bar from saturated vapor
Because you have saturated vapor, state 1 will be located somewhere on the right side of the curve.
To get to state 2, we undergo constant pressure heating, so we follow an isobar (a line of constant
pressure) to the right to increase the pressure. Think about how a pressure cooker works. Adding heat, increases pressure.
Process 2-3: Constant-Volume Cooling
to P
3
=
5
¯
¿
, T
3
=
160
℃
To get to state 3, we undergo constant volume cooling. So we decrease temperature (cooling) without moving along the x-axis (volume does not change). BUT we have a problem. We don’t know if we have cooled enough to fall under the saturated liquid-vapor dome on the left diagram (resulting in a mix of liquid and vapor) or if we are a cooled vapor on the right diagram (still only vapor).
OR
USE Pressure Chart A-5 in appendix
Convert bar to kPa. P
3
=
5
¯
¿
500
kPa
Look up T
sat
at P=500kPa. T
sat
=151.83
o
C. But what does mean T
sat
and where is it on the graph?
Your preview ends here
Eager to read complete document? Join bartleby learn and gain access to the full version
- Access to all documents
- Unlimited textbook solutions
- 24/7 expert homework help
We know that our given T
3
=
160
℃
is greater than T
sat
=151.83
o
C. So our point 3 will be above this since it’s a higher temperature, we will just follow the y-axis! Since it’s still above the saturated liquid-vapor dome, we remain only vapor! If T3 was less than 151.83, we would be a mixture of liquid and vapor like the diagram on the left, above.
Process 3-4: Isothermal compression
with Q
3
−
4
=−
815.8
kJ
To get to state 4, we know that we undergo isothermal (constant temperature) compression (decrease in volume). Because it’s constant temperature, we follow an isotherm, and because we
decrease volume, we go to the left. BUT we have another problem. How far to the left (decrease in volume) do we go???
Because we are a
CYCLE, we must begin and end at the same state. So we can look at process 4-1 to guide us. Process 4-1 is Constant volume heating, so increasing the temperature (going up
on y-axis) without changing volume (not moving on the x-axis). This is just a vertical line!
SO, to answer how far left we go from Process 3-4 (aka how much we decrease volume), we decrease the volume to be immediately below state 1.
And that’s our T-V diagram! We can remove the rest of the isobar to clean it up:
For the P-V diagram, start with the basics:
Your preview ends here
Eager to read complete document? Join bartleby learn and gain access to the full version
- Access to all documents
- Unlimited textbook solutions
- 24/7 expert homework help
Isotherms switch angles!
Process 1-2: Constant Pressure Heating
at 10 bar from saturated vapor
Because you have saturated vapor, state 1 will be located somewhere on the right side of the curve.
To get to state 2, we undergo constant pressure heating, so we follow an isobar (a line of constant
pressure) to the right to increase the pressure (in this case, this is just following the x-axis to the right. If you are confused as to why we go to the right, we are adding heat and increasing the temperature of our vapor so we have to “jump isotherms” from T2 to T1).
Process 2-3: Constant-Volume Cooling
to P
3
=
5
¯
¿
, T
3
=
160
C
To get to state 3, we undergo constant volume cooling. So we decrease temperature (cooling) without moving along the x-axis (volume does not change). Again we may wonder, how much do we cool? Do we fall under the dome? OR
Since we already calculated that we are not in the saturated liquid vapor dome at state 3, we choose the graph on the right.
Process 3-4: Isothermal compression
with Q
3
−
4
=−
815.8
kJ
To get to state 4, we know that we undergo isothermal (constant temperature) compression (decrease in volume). Because it’s constant temperature, we follow an isotherm, and because we
decrease volume, we go to the left.
Your preview ends here
Eager to read complete document? Join bartleby learn and gain access to the full version
- Access to all documents
- Unlimited textbook solutions
- 24/7 expert homework help
BUT we have another problem. How far to the left (decrease in volume) do we go???
Because we are a
CYCLE, we must begin and end at the same state. So we can look at process 4-1 to guide us. Process 4-1 is Constant volume heating, so increasing the temperature (going up
on y-axis) without changing volume (not moving on the x-axis). This is just a vertical line!
And that’s our P-V diagram! We can remove the rest of the isotherm to clean it up:
Now for the table:
Fill in given information!
State 1
State 2
State 3
State 4
Unit
Pressure
[kPa]
Specific Volume, v
[m3/kg]
Specific Internal Energy, u
[kJ/kg]
Process 1-2: Constant Pressure Heating
at 10 bar is given! Remember to convert units. This gives us P1 and P2 because P stays constant
State 1
State 2
State 3
State 4
Unit
Pressure
1000
1000
[kPa]
Specific Volume, v
[m
3
/kg]
Specific Internal Energy, u
[kJ/kg]
Process 2-3: Constant-Volume Cooling
to P
3
=
5
¯
¿
is given! Remember to convert units. This gives us P3
State 1
State 2
State 3
State 4
Unit
Pressure
1000
1000
500
[kPa]
Specific Volume, v
[m
3
/kg]
Specific Internal Energy, u
[kJ/kg]
This leaves P4 for us to find. From the given data we know that T
3
=
160
C
= T4. At T4, we are at the saturation pressure (follow the isobar and we know that psat is the pressure at the left and right edge of the dome. Since we have a P-V diagram, pressure is constant when moving left/right under the dome.
State 1
State 2
State 3
State 4
Unit
Pressure
1000
1000
500
618
[kPa]
Specific Volume, v
[m
3
/kg]
Specific Internal Energy, u
[kJ/kg]
So use Table A-4 and look up P
sat
for T=160
o
C
Now let’s go back to state 1.
Find specific volume and internal energy at P=1000kPa
Use Table A-5 and look up v and u for P=1000kPa. Since we are saturated vapor, use the saturated vapor values.
Your preview ends here
Eager to read complete document? Join bartleby learn and gain access to the full version
- Access to all documents
- Unlimited textbook solutions
- 24/7 expert homework help
State 1
State 2
State 3
State 4
Unit
Pressure
1000
1000
500
618
[kPa]
Specific Volume, v
0.194
[m
3
/kg]
Specific Internal Energy, u
2583
[kJ/kg]
Now for state 4 data since it’s the next easiest to find. Looking at our T-V diagram, we know that v1=v4.
State 1
State 2
State 3
State 4
Unit
Pressure
1000
1000
500
618
[kPa]
Specific Volume, v
0.194
0.194
[m
3
/kg]
Specific Internal Energy, u
2583
[kJ/kg]
We know that we are a mix of liquid and vapor, so we need to find the quality. From the given data we know that T
3
=
160
C
= T4.
Use Table A-4 and look up v for T=160
x
=
(
v
4
−
v
liquid , sat
)
v
vap,sat
−
v
liquid , sat
=
.194
−
0.001102
0.30680
−
0.001102
=
0.63
or 63% Vapor!
Using this, we find u4. x
=
(
u
4
−
u
liquid ,sat
)
u
vap, sat
−
u
liquid ,sat
rearrange to solve for u4
u
4
=
u
liq ,sat
+
x
(
u
vap, sat
+
u
liq ,sat
)
=
674.49
+
0.63
(
2567.8
−
674.49
)
=
1871
State 1
State 2
State 3
State 4
Unit
Pressure
1000
1000
500
618
[kPa]
Specific Volume, v
0.194
0.194
[m
3
/kg]
Specific Internal Energy, u
2583
1871
[kJ/kg]
Now let’s look again at state 3, since there’s more given information that we haven’t used. Using Table A-6 let’s look up v at T=160C
We must interpolate from the Tsat of 151.83C and 200C to find the volume at 160C
v
160
=
0.383
Now for v2,
States 2 and 3 have the same v.
State 1
State 2
State 3
State 4
Unit
Pressure
1000
1000
500
618
[kPa]
Specific Volume, v
0.194
0.383
0.383
0.194
[m
3
/kg]
Specific Internal Energy, u
2583
1871
[kJ/kg]
Use A-6 let’s look up u at T=160
o
C and 5 bar = 0.5 MPa We must interpolate from the Tsat of 151.83C and 200C to find the internal energy at 160C
u
160
=
2574.7
State 1
State 2
State 3
State 4
Unit
Pressure
1000
1000
500
618
[kPa]
Specific Volume, v
0.194
0.383
0.383
0.194
[m
3
/kg]
Specific Internal Energy, u
2583
2574.7
1871
[kJ/kg]
Now last is u2:
We are given P1 = P2 = 10 bar = 1000kPa = 1MPa Use A-6. We don’t know the temperature, but we have the specific volume at P2! So let’s use the specific volumes at P2 and interpolate to find the internal energy u. U2= 3231!
State 1
State 2
State 3
State 4
Unit
Pressure
1000
1000
500
618
[kPa]
Specific Volume, v
0.194
0.383
0.383
0.194
[m
3
/kg]
Specific Internal Energy, u
2583
3231
2574.7
1871
[kJ/kg]
Question 2:
A rigid tank contains a gas mixture with a specific heat of c
V
= 0.748 kJ/(kg*K). The mixture is cooled from 200 kPa and 200
until its pressure is 100 kPa. Determine the heat transfer during ℃
the process, in kJ/kg.
The heat transfer is defined as:
∆u
=
∫
1
2
c
v
(
T
)
dT
=
c
v
∆T
So we need to find ΔT. The initial temperature is given, so we need to find the final temperature.
Notice that this ‘mixture’ is gas, and its temperature & pressure are neither too high nor too low, which meets the criteria for ideal gas behavior.
From the ideal gas law:
Pv
=
RT
⟹
P
T
=
R
v
Notice that the gas is in ‘a rigid tank’, which suggests no volume change and no mass transfer. So the specific volume remains constant, which means R/v remains constant.
So the final temperature:
T
2
=
P
2
P
1
T
1
=
100
kPa
200
kPa
×
473
K
=
236.5
K
The heat transfer is:
∆u
=
c
v
∆T
=
0.748
kJ
kg∙K
∙
236.5
K
=
176.9
kJ
kg
Your preview ends here
Eager to read complete document? Join bartleby learn and gain access to the full version
- Access to all documents
- Unlimited textbook solutions
- 24/7 expert homework help
Question 3:
A cylinder-piston system contains 2 kg of H
2
O at 150 kPa and has a volume of 0.35 m
3
. The piston is moved so that the final volume of the inside the cylinder is 2.319 m
3
. During the piston motion from the initial to the final state, there is heat transfer to the cylinder in such a way as to hold the temperature constant.
(a) What is the final pressure in the cylinder?
(b) How much work was done by the steam?
(c) Evaluate the heat transfer during the process.
*)Typo: both W and V are absolute work and volume (“upper case”) in the equation above.