Chap.4 ideal gases and thermodynamic processes
-
Upload
lj-polytechnic -
Category
Engineering
-
view
52 -
download
10
Transcript of Chap.4 ideal gases and thermodynamic processes
CHAPTER 5Thermodynamic
cycles
Missam Raza Mechanical Dept LJ Polytechnic
Thermodynamic cycles Introduction
Is a series of processes which form a closed path.
The initial and the final states are coincident
Thermal engines work in a cyclic process.
A Thermal engines draws heat from a hot source and rejects heat to a cold source producing work
Missam Raza Mechanical Dept LJ Polytechnic
Thermodynamic cycles Heat Engine Power Cycles
Hot body or source
Cold body or sink
System, or heat engine
Qin
Qout
Wcycle
Missam Raza Mechanical Dept LJ Polytechnic
Thermodynamic cycles Energy analysis of cycles
4
1
3
2
For the cycle, E1 E1 = 0, or
0ΔE cycle
0 W Q ΔE cycle cyclecycle
Missam Raza Mechanical Dept LJ Polytechnic
Thermodynamic cycles formula
Q Wcycle cycle
Qcycle and Wcycle represent net amounts
which can also be represented as:
Qcycle = Wcycle
Missam Raza Mechanical Dept LJ Polytechnic
Thermodynamic cycles Carnot Cycle
The Carnot cycle is a reversible cycle that is composed of four internally reversible processes.
Two isothermal processes
Two adiabatic processesMissam Raza Mechanical Dept
LJ Polytechnic
Thermodynamic cycles The Carnot cycle for a gas might occur as visualized below.
Missam Raza Mechanical Dept LJ Polytechnic
Thermodynamic cycles Introduction
This is a Carnot cycle involving two phases -- it is still two adiabatic processes and two isothermal processes.
It is always reversible -- a Carnot cycle is reversible by definition.Missam Raza Mechanical Dept
LJ Polytechnic
Thermodynamic cycles Otto Cycle
P-V diagram (Work)
T-S diagram (Heat Transfer)
Missam Raza Mechanical Dept LJ Polytechnic
Otto cycle Performance of cycle
H
L
H
net
Q
Q1
Q
w
Thermal Efficiency:
Need to know QH and QL
Missam Raza Mechanical Dept LJ Polytechnic
Otto cycle Process
• Heat addition 2-3 QH = mCV(T3-T2)• Heat rejection 4-1 QL = mCV(T4-T1)
• or in terms of the temperature ratios
23V
14V
H
L
TTmC
TTmC1
Q
Q1
1TTT
1TTT1
Q
Q1
232
141
H
L
qout
qi
n
Missam Raza Mechanical Dept LJ Polytechnic
Otto cycle Process
• 1-2 and 3-4 are adiabatic process, using the adiabatic relations between T and V
4
3
1
2
4
3
1
3
4
1
2
1
1
2
T
T
T
T
T
T
V
V
V
V
T
T
RATIOVOLUMESAME
2
11
2
1
V
V r ;
r
11
T
T1
qout
qin
Missam Raza Mechanical Dept LJ Polytechnic
Otto cycle Process
• Heat addition 2-3 QH = mCV(T3-T2)• Heat rejection 4-1 QL = mCV(T4-T1)
• or in terms of the temperature ratios
23V
14V
H
L
TTmC
TTmC1
Q
Q1
1TTT
1TTT1
Q
Q1
232
141
H
L
qout
qi
n
Missam Raza Mechanical Dept LJ Polytechnic
Otto cycle
Cycle performance with cold air cycle assumptions
1k2
1Otto,th r
11
T
T1
This looks like the Carnot efficiency, but it is not! T1 and T2 are not constant.
What are the limitations for this expression?
Missam Raza Mechanical Dept LJ Polytechnic
THANK YOU
Missam Raza Mechanical Dept LJ Polytechnic