Diesel Comparison

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Diesel Cycle Revision + Comparison An ideal Diesel cycle with air as the working fluid has a compression ratio of 18 and a cutoff ratio of 2. At the beginning of the compression process, the working fluid is at 100 kPa, 27°C, and 1917 cm 3 . Using the THREE different methods, detennine: The maximum temperature and pressure that occur during the cycle, the net work output, the thermal efficiency, and the mean effective pressure for the cycle. Case (I): Adiabatic Compression & Expansion + Constant Specific Heat Sm hi, CjL rrc L. J i) r.:::- I (9Q F: H .. I 1':::- $0 0 Ie- I 1"11:)-'* 106 m :1 Yh -:=- 100* f9J9--.t1:: = . J2.-1' .-- 0 3 () c> \\J =- 0,-8-( e\.t _ .2) r - <T t-- S- ,1 1<:- JCR. f'l.-":- Pt cfl .... tz - 5"}- UJ c...\) ::: '\dO S r/ :=. I, 'L e> -::- p,,- / 12 k... T; 6, ( k.. J 2- .1 :::0. Yc. -:=.. ") \:J- J:C- :2 ,11-4' I 6 /'Y1 o \Iv,: Id-() 7-9/·':}-1c.. P y <:0- :l 6lf , .. \'Y\ I, o4y ::- YY\ CAs &3 -Cftt).t :: \(-} Q o.,s- "2. VY\ CAt C1; r- 'T; ) Q .;}-2> '3 M :: W =- 0,,,,_Qud ::::: \. 1 \A:) 1\1\ = - 7--'fS: 6 {j 'Y)#- £ sI (' J -\:1 'l- ll-Pq'

description

Summery comparison for Diesel engine between the various processes.

Transcript of Diesel Comparison

Page 1: Diesel Comparison

Diesel Cycle Revision + Comparison

An ideal Diesel cycle with air as the working fluid has a compression ratio of 18 and a cutoff ratio of 2. At the beginning of the compression process, the working fluid is at 100 kPa, 27°C, and 1917 cm3

.

Using the THREE different methods, detennine: The maximum temperature and pressure that occur during the cycle, the net work output, the thermal efficiency, and the mean effective pressure for the cycle.

Case (I): Adiabatic Compression & Expansion + Constant Specific Heat

G)\'~\ 1),~ Sm hi, CjL ~l'6f rrc ~ L. J

i) r.:::- I(9Q F:H.. I 1':::-$0 0 Ie- I ~,-::.. 1"11:)-'* 106 m :1

Yh ~ R~ -:=- 100* f9J9--.t1:: = .2,'LLtl.f~'? ~ . J2.-1' .--0 ,tL~" ~ 3 () c>

\\J =- 0,-8-( ~ e\.t _.2) r - <T t-- ~ S-~ ,1 1<:­~- JCR. ~~

f'l.-":- Pt cfl....tz - 5"}-UJ ~_J?", c...\) ::: '\dO S r/

~~ ~ :=. I, a6~r~4 ~ 'L

e> -::- p,,- / 12 ~ k... ':::~T; ~ I~o 6, ( k.. ~ J 2- -~ .1J· :::0. Yc. -:=..") \:J-J:C- :2 ,11-4' I 6 /'Y1

o \Iv,: Id-() ~:::-T;(~~)-\ ~ 7-9/·':}-1c..

Py <:0- f~ (~"')~ ~ :l 6lf tP~ , .. W~r ~ \'Y\ ~ (~-II") ~ I, o4y ~J

\N~\D ::- YY\ CAs &3 -Cftt).t ~&~.Jd'L) :: ~,y \(-} Qo.,s- "2. VY\ CAt C1; r-'T; ) ~ Q.;}-2> ~ ~'3

~\'v'\- ~ M ~lli-T<-,) :: ~,\~ ~.:: W ~ =- 0,,,,_Qud ::::: \. 1 ~ \A:)

1\1\ t~p =~ -7--'fS:6{j 'Y)#- ~ o· £sI~ (' J ~-\:1'l- ll-Pq'

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Case (U): Polytropic Compression & Expansion + Constant Specific Heat I n =-) f..?

i) ~~ 'Y'N- CV) ~~

:l.) '-;::::~ L rt' -I -== ?-I 4 1<:. •

P1- 2:- p\ uz..lI\ ::= Lt~y \CJ Slc Pq

~ ~::-PL r.- --Y:~ L ) f ~ - <:-- \ 2.. ::: '4'2-2 t<: Y. ~ '"" t1, ~ ......'1

) J - o("',..s ~(~ M 1

~ ~~ T3(:sttJn-l~ 1-3 8 ~'1-k D P()~ , I I' ~v... '::. V\rLJ::: > ~ ~ 2-L,\JI 'L L k}q

\N4ry '=- '(Y) ~ trL-I;) ~ q8~\ <g ~'Y (~' ~ ~r1-::: CJ •'L'L-Ic. '3 W~~QI-~1n~ ('I; ~)

W~f~ '~~ (T>~)-t ~("l-~L) :::c (,1'l1fY 1<-3

~3-'1::::f)\CJ (T~-\i) ~ \tJ~p =- 0, lG ~ 2.- l':S3-y

-', C?\)~~ ~ G).;", '"\- CQ N ::. \. '1 6'] ~ I.A-~

~C>§~ '"::- <14,.J- '\ (!) \'l. ::. 0-1 1. 1'L Ln

\JJ~ -= 1,- 0 Yu ~-S I rY\ r;; ~ ~ y.l~- -::c 5'1-1-97 r-pq ~ ",l=, - ~\r-'cJL

N\ftJ\ ':-- ~~ ~ Q.5;­0,t'\#-W­

(Q,,/\ ':- YY\ Cp (T1 :r'l__) ;> Q~ ~ mCv ~ -~)

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Case (Ill) : Variable Specific Heat ~v.~ q,;;'VI -::: CJ s.i-. '7-(~ . )~

I) 17 ::3M\<:.. -=) U,::. ,;).\L).d1-{; I "J;-\ ':- 62.-/. 'L