2 operating parameters
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22TOPICTOPIC
Engine design andEngine design andoperating parametersoperating parameters
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Satisfactory performance over its operating range
Low fuel consumption
Low noise and emissions Low initial cost
High reliability and durability
What do we need from engine?What do we need from engine?
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Maximum rated power The highest power an engine is
allowed to develop for short periods of operation
Normal or nominal rated power.The highest power an
engine is allowed to develop in continuous operation
Rated speed The cran!shaft rotational speed at which
rated power is developed
Engine performance definitionsEngine performance definitions
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Geometrical propertiesGeometrical properties
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Geometrical propertiesGeometrical properties
d cc
c
V Vr
V
+=
Compression ratio
" # $% for SI
$% # %& for CI
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Geometrical propertiesGeometrical properties
d cc
c
V Vr
V
+=
bsR B L=
Compression ratio
'atio of cylinder bore to piston stro!e
" # $% for SI
$% # %& for CI
(" # $% Small
() Large* slow speed
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Geometrical propertiesGeometrical properties
d cc
c
V Vr
V
+=
bsR B L=
R l a=
2L a=
Compression ratio
'atio of cylinder bore to piston stro!e
'atio of connecting rod length to cran! radius
" # $% for SI
$% # %& for CI
(" # $% Small
() Large* slow speed
+ # & Small
) # , Large* slow speed
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Cylinder volume at any crank positionCylinder volume at any crank position
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Cylinder volume at any crank positionCylinder volume at any crank position
cV V=
cV V V= +
c dV V V= +
( )2
4
BV l a s
= +
( )1 22 2 2cos sins a l a = +
( )( )2 211 1 1 cos sin2
c
c
Vr R R
V
= + +
Piston at T-C
Piston at .-C
/t any cran! angle
where sis the distance between the cran! a0is
and the piston pin a0is and is given by
Cylinder volume at any cran! position
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Comustion chamer surface areaComustion chamer surface area
( )ch pA A A B l a s= + + +
( )2 21 cos sin2
ch p
BLA A A R R
= + + +
chA
2
4p
BA
=
Cylinder head surface area
Piston crown surface area
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!iston speed!iston speed
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!iston speed!iston speed
pds ds d Sdt d dt
= =
2d
N
dt
= =
2pds
S Nd
=
2 2
cossin 1
sin
pS LN
R
= +
Instantaneous piston speed
/fter differentiation
( )1 2
2 2 2cos sins a l a = +
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!iston speed vs crank angle!iston speed vs crank angle
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Mean piston speedMean piston speed
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.etter than using rotational speed 1'P23
4as flow velocities in the inta!e manifold and cylinder all scale with
mean piston speed
5low resistance and stresses limit ma0imum values to within therange " to $) m6s
Lower end is typical for large industrial engines
High end is typical of automotive engines
Mean piston speedMean piston speed
2pS LN=
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"rake tor#ue and power"rake tor#ue and power
Tor7ue is a wor! Power is a rate at which wor! is done
.ra!e power is a usable power delivered by engine to consumer
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"rake tor#ue and power"rake tor#ue and power
Tor7ue is a wor! Power is a rate at which wor! is done
.ra!e power is a usable power delivered by engine to consumer
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"rake tor#ue and power"rake tor#ue and power
Tor7ue is a wor! Power is a rate at which wor! is done
.ra!e power is a usable power delivered by engine to consumer
FbT=
2P T NT = =
( ) ( ) ( )
3.kW 2 rev/s N m 10P N T =
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$ndicated work per cycle$ndicated work per cycle
,c iW pdV =
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$ndicated work per cycle$ndicated work per cycle
,c iW pdV =
Gross indicated work per cycle is the wor! delivered to the piston
over the compression and e0pansion stro!es only,c igW
area + areac igW A C=,
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$ndicated work per cycle$ndicated work per cycle
,c iW pdV =
Gross indicated work per cycle is the wor! delivered to the piston
over the compression and e0pansion stro!es only
Net indicated work per cycle is the wor! delivered to the pistonover the entire four8stro!e cycle
,c igW
,c inW
area + areac igW A C=,
area area,c inW A B=
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$ndicated work per cycle$ndicated work per cycle
,c iW pdV =
Gross indicated work per cycle is the wor! delivered to the piston
over the compression and e0pansion stro!es only
Net indicated work per cycle is the wor! delivered to the pistonover the entire four8stro!e cycle
!umping work is the wor! transfer between piston and cylinder
gases during inlet and e0haust stro!es
,c igW
,c inW
area + areac igW A C=,
pW
area area,c inW A B=
area areapW B C= +
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!umping work!umping work
Pumping wor! transfer will be
8 from piston to gases if the pressure during the inta!e stro!e is less
than the pressure during the e0haust stro!e 1naturally aspirated
engines3
8 from gases to piston if the e0haust stro!e pressure is lower than
inta!e pressure 1turbocharged engines3
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$ndicated power$ndicated power
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$ndicated power$ndicated power
The power per cylinder is related to the indicated wor! per cycle by
,c i
i
R
W NP
n=
where nRis the number of cran! revolutions for each power stro!e per
cylinder
5or four8stro!e cycles* nR =%* for two8stro!e cycles* nR=$
Indicated power differs from bra!e power by the power absorbed inovercoming engine friction* driving engine accessories* and 1in the case of
gross indicated power3 the pumping power
9e will use mostly gross indicated wor! and power
Terms brakeand indicatedare used to describe other parameters
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Mechanical efficiencyMechanical efficiency
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Mechanical efficiencyMechanical efficiency
.ra!e power is the gross indicated power diminished by the friction power
b ig f P P P=
5riction power is defined as power re7uired to overcome the flow friction*
friction of the bearings* pistons* and other mechanical components of theengine* and to drive the engine accessories
5riction power may be determine by driving unfired engine with a
dynamometer
1 fb
m
ig ig
PP
P P = = ,( to :); under load
( at idling
2echanical
efficiency
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Road-load poweris the power re7uired to drive a vehicle on a level road
at a steady speed
Coefficient of rolling resistance
Drag coefficient
Road%load powerRoad%load power
212
r R v a D v v vP C M g C A S S = +
0 012 0 015RC<
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Mean effective pressureMean effective pressure
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Mean effective pressureMean effective pressure
Mean effective pressure# the ratio of wor! per cycle and
swept volume can be increased without increase in mean
piston speed and* conse7uently* without increase of frictional
losses* both flow and rubbing
# Increased volumetric efficiency due to lower flow velocity and
increased valve area
# -ecreased heat transfer to cooling system
Cons
# Increased mass 1length and width increases* height is thesame3
# Higher probability of !noc! combustion for SI Fngines
# -esign consideration 1balancing counterweights can meet
piston at .-C3
2igher ",3 ratio4 pros and cons2igher ",3 ratio4 pros and cons
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