How Is the Efficiency of the Diesel Cycle Derived Using Compression Ratios?

Click For Summary

Homework Help Overview

The discussion revolves around deriving the efficiency of the Diesel cycle in relation to the compression ratio. Participants are exploring the relationships between work done and heat transfer within the cycle, as well as the definitions of various points in the cycle.

Discussion Character

  • Conceptual clarification, Problem interpretation, Assumption checking

Approaches and Questions Raised

  • Participants are attempting to relate the efficiency formula to the work done and heat transfer in the Diesel cycle. Questions arise regarding the definitions of specific points in the cycle and the meaning of the variable δ. There is also exploration of the equations for work done during different strokes of the cycle.

Discussion Status

The discussion is active, with participants clarifying the roles of different points in the cycle and the nature of the strokes. Some guidance has been provided regarding the relationship between heat transfer and work done, and there is an ongoing exploration of how to calculate the heat inputs and outputs.

Contextual Notes

Participants note that the numbering of points in the cycle is arbitrary and that assumptions about the adiabatic exponent and heat capacities are under discussion. There is an emphasis on understanding the heat flow during specific strokes of the cycle.

xspook
Messages
19
Reaction score
0

Homework Statement



Derive a formula for the efficiency of the Diesel cycle, in terms of the compression ratio V1/V2

Homework Equations



e=\frac{W}{Q_{h}}
w= ∫pdV



The Attempt at a Solution



Now I know I should have used e=1-\frac{Q_{c}}{Q_{h}} to get it but he said it is possible using e=\frac{W}{Q_{h}}

I know that W_{4-1} is equal to zero and W_{2-3} is equal to P_{2}(V_{3}-V_{2})

what I don't know is how he got

W_{1-2} = \frac{e}{1-δ}*cv^{-δ+1} = \frac{1}{1-δ}*(P_{2}V_{2}-P_{1}V_{1})

and

W_{3-1} = \frac{e}{1-δ}*cv^{-δ+1} = \frac{1}{1-δ}*(P_{4}V_{4}-P_{3}V_{3})
 
Physics news on Phys.org
What are points 1,2,3, and 4? What is ##\delta##?
 
1,2,3 and 4 are the strokes of the cycle. Well the different points on the picture. and δ is supposed to be gamma, which is the adiabatic exponent.

I thought I could use

W=∫pdV = C_{v}(T_{1}-T_{2}
for the compression stroke...but I guess that is incorrect
 
xspook said:
1,2,3 and 4 are the strokes of the cycle. Well the different points on the picture.
You have to be more specific. The numbering of points on a cycle is arbitrary. For each part of the cycle, state something like: 1→2 isothermal expansion at ##T_2##.
 
From 1→2 is compression
From 2→3 is fuel injection/combustion
From 3→4 is the power stroke
From 4→1 is exhaust
 
xspook said:
1,2,3 and 4 are the strokes of the cycle. Well the different points on the picture. and δ is supposed to be gamma, which is the adiabatic exponent.

I thought I could use

W=∫pdV = C_{v}(T_{1}-T_{2}
for the compression stroke...but I guess that is incorrect
The ideal diesel cycle consists of a constant pressure expansion (2-3) followed by an adiabatic expansion (3-4) followed by constant volume cooling (4-1) followed by adiabatic compression (1-2).

So heat goes in only from 2-3 and heat goes out only from 4-1. Since W = Qh-Qc and η = W/Qh = 1-Qc/Qh you just have to deal with the two parts in which heat flows (ie. 4-1 and 2-3).

Can you work out Qh and Qc? (hint: it involves temperature change and heat capacity).

AM
 

Similar threads

Replies
10
Views
3K
  • · Replies 10 ·
Replies
10
Views
3K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 5 ·
Replies
5
Views
1K
  • · Replies 3 ·
Replies
3
Views
1K
Replies
14
Views
2K
  • · Replies 5 ·
Replies
5
Views
3K
Replies
8
Views
4K
Replies
4
Views
3K
Replies
1
Views
3K