Jump to content

Mean effective pressure: Difference between revisions

From Wikipedia, the free encyclopedia
Content deleted Content added
m Uniform citation style
No edit summary
 
(23 intermediate revisions by 8 users not shown)
Line 1: Line 1:
{{Short description|Measure of an engine's capacity to do work}}
{{ Infobox physical quantity
{{ Infobox physical quantity
| name = Mean effective pressure
| name = Mean effective pressure
Line 8: Line 9:
}}
}}


The '''mean effective pressure''' is a quantity relating to the operation of a [[reciprocating engine]] and is a valuable measure of an engine's capacity to do work that is independent of [[engine displacement]].<ref>Heywood, J. B., "Internal Combustion Engine Fundamentals", McGraw-Hill Inc., 1988, p. 50</ref> When quoted as an ''indicated'' mean effective pressure or IMEP (defined below), it may be thought of as the average [[pressure]] acting on a piston during the different portions of its cycle.
The '''mean effective pressure''' ('''MEP''') is a quantity relating to the operation of a [[reciprocating engine]] and is a measure of an engine's capacity to do work that is independent of [[engine displacement]].<ref>Heywood, J. B., "Internal Combustion Engine Fundamentals", McGraw-Hill Inc., 1988, p. 50</ref> Despite having the dimension of pressure, MEP cannot be measured.<ref name="Schreiner 2011 p. 41" /> When quoted as an ''indicated mean effective pressure'' (''IMEP''), it may be thought of as the average [[pressure]] acting on a [[piston]] during the different portions of its [[engine cycle|cycle]]. When friction losses are subtracted from the IMEP, the result is the brake mean effective pressure ('''BMEP''').


==Derivation==
==Derivation==
Let:
Let:
:<math>W</math> = work per cycle in joule;
:<math>P</math> = power output in watt;
:<math>P</math> = power output in watt;
:<math>p_\text{me}</math> = mean effective pressure in pascal;
:<math>p_\text{me}</math> = mean effective pressure in megapascal;
:<math>V_\text{d}</math> = displacement volume in cubic metre;
:<math>V_\text{d}</math> = displacement volume in cubic centimetre;
:<math>n_\text{c}</math> = number of revolutions per power stroke (for a 4-stroke engine, <math>n_\text{c} =2</math>);<ref name="Wankel" group="Note">Wankel engines are four-stroke engines, so <math>n_\text{c} =2</math>; the displacement <math>V_\text{d}</math> is derived from the chamber volume <math>V_\text{c}</math> by multiplying it with the number of rotary pistons <math>i</math> and 2: <math>V_\text{d} = 2 V_\text{c} i</math> (see Wolf-Dieter Bensinger: ''Rotationskolben-Verbrennungsmotoren'', Springer, Berlin/Heidelberg/New York 1973, {{ISBN|978-3-642-52174-4}}, p. 66)</ref>
:<math>i</math> = number of cycles per revolution (for a 4-stroke engine, <math>i =0.5</math>, for a 2-stroke engine, <math>i =1</math>);<ref name="Wankel" group="Note">Wankel engines are four-stroke engines, so <math>i =0.5</math>; the displacement <math>V_\text{d}</math> is derived from the chamber volume <math>V_\text{c}</math> by multiplying it with the number of rotary pistons <math>i</math> and 2: <math>V_\text{d} = 2 V_\text{c} i</math> (see [[Wolf-Dieter Bensinger]]: ''Rotationskolben-Verbrennungsmotoren'', Springer, Berlin/Heidelberg/New York 1973, {{ISBN|978-3-642-52174-4}}, p. 66)</ref>
:<math>N</math> = number of revolutions per second;
:<math>n</math> = number of revolutions per second;
:<math>T</math> = torque in newton-metre.
:<math>\omega = </math> angular velocity, i.e. <math>\omega = 2 \pi n</math>;
:<math>M</math> = torque in newton-metre.


Then, BMEP may be used to determine an engine's power output as follows:
The [[Power (physics)|power]] produced by the engine is equal to the work done per operating cycle times the number of operating cycles per second. If ''N'' is the number of revolutions per second, and <math>n_\text{c}</math> is the number of revolutions per power stroke, the number of power strokes per second is just their ratio. We can write:
:<math>
P = {W {N \over n_\text{c}}}.
</math>
Reordering to put work on the left:
:<math>
W = {P {n_\text{c} \over N}}.
</math>


By definition:
:<math>
:<math>
W = p_\text{me} V_\text{d},
P=i \cdot n \cdot V_\text{d} \cdot p_\text{me}
</math>
so that
:<math>
p_\text{me} = {P n_\text{c} \over V_\text{d} N}.
</math>
</math>


Since we know that power is:
Since the [[torque]] ''T'' is related to the angular speed (which is just ''N''·2π) and power produced,

:<math>
:<math>P = \omega \cdot M = 2 \pi \cdot n \cdot M</math>
P = {2 \pi} T N,
</math>


then the equation for MEP in terms of torque is:
We now see that, BMEP is a measure of expressing torque per displacement:

:<math>P = i \cdot n \cdot V_\text{d} \cdot p_\text{me} = 2 \pi \cdot n \cdot M</math>

And thus, the equation for BMEP in terms of torque is:
:<math>
:<math>
p_\text{me} = {2 \pi} {n_\text{c}} {T \over V_\text{d}}.
p_\text{me} = {{M \cdot 2 \pi} \over {V_\text{d} \cdot i}}.
</math>
</math>


Speed has dropped out of the equation, and the only variables are the torque and displacement volume. Since the range of maximum brake mean effective pressures for good engine designs is well established, we now have a displacement-independent measure of the torque-producing capacity of an engine design{{snd}} a specific torque of sorts. This is useful for comparing engines of different displacements. Mean effective pressure is also useful for initial design calculations; that is, given a torque, standard MEP values can be used to estimate the required engine displacement. However, mean effective pressure does not reflect the actual pressures inside an individual combustion chamber{{snd}} although the two are certainly related{{snd}} and serves only as a convenient measure of performance.
Speed has dropped out of the equation, and the only variables are the torque and displacement volume. Since the range of maximum brake mean effective pressures for good engine designs is well established, we now have a displacement-independent measure of the torque-producing capacity of an engine design{{snd}} a specific torque of sorts. This is useful for comparing engines of different displacements. Mean effective pressure is also useful for initial design calculations; that is, given a torque, standard MEP values can be used to estimate the required engine displacement. However, mean effective pressure does not reflect the actual pressures inside an individual combustion chamber{{snd}} although the two are certainly related{{snd}} and serves only as a convenient measure of performance.<ref name="Schreiner 2011 p. 41">{{cite book | last=Schreiner | first=Klaus | title=Basiswissen Verbrennungsmotor | publisher=Vieweg+Teubner Verlag | publication-place=Wiesbaden | date=2011-05-25 | isbn=978-3-8348-1279-7 | language=de | page=41}}</ref>


Brake mean effective pressure (BMEP) is calculated from measured [[dynamometer]] torque. Net indicated mean effective pressure (IMEP<sub>n</sub>) is calculated using the [[horsepower|indicated power]]; i.e., the pressure volume integral in the work per cycle equation. Sometimes the term FMEP (friction mean effective pressure) is used as an indicator of the mean effective pressure lost to friction (or friction torque), and is just the difference between IMEP<sub>n</sub> and BMEP.
Brake mean effective pressure (BMEP) is calculated from measured [[dynamometer]] torque. Net indicated mean effective pressure (IMEP) is calculated using the [[horsepower|indicated power]]; i.e., the pressure volume integral in the work per cycle equation. Sometimes the term FMEP (friction mean effective pressure) is used as an indicator of the mean effective pressure lost to friction (or friction torque) and is just the difference between IMEP and BMEP.<ref name="Spicher_2017_24" />


== Examples ==
== Examples ==
Line 56: Line 48:
;MEP from torque and displacement
;MEP from torque and displacement


A four-stroke engine produces 160&nbsp;N·m of torque, and displaces 2000&nbsp;cm<sup>3</sup>=2&nbsp;dm<sup>3</sup>=0.002&nbsp;m<sup>3</sup>:
A four-stroke engine produces 159&nbsp;N·m of torque, and displaces 2000&nbsp;cm<sup>3</sup>

*<math>n_\text{c}=2</math>
*<math>T=160 \, \text{N} {\cdot} \text{m}</math>
*<math>V_\text{d}=0.002 \, \text{m}^3</math>

:<math>p_\text{me} = {2 \pi} {2} {{160 \, \text{N} {\cdot} \text{m}} \over {0.002 \, \text{m}^3}} = {2 \pi} {2} {{160 \, \text{N} \cancel{\cdot \text{m}}} \over {0.002 \, \text{m}^{{\cancel 3} 2}}}=1,005,310 \, \text{N} {\cdot} \text{m}^{-2} = 10.05 \, \text{bar} = 1.005 \, \text{MPa}</math>

We also get the megapascal figure if we use cubic centimetres for <math>V_\text{d}</math>:


*<math>n_\text{c}=2</math>
*<math>i=0.5</math>
*<math>T=160 \, \text{N} {\cdot} \text{m}</math>
*<math>M=159 \, \text{N} {\cdot} \text{m}</math>
*<math>V_\text{d}=2000 \, \text{cm}^3</math>
*<math>V_\text{d}=2000 \, \text{cm}^3</math>


:<math>p_\text{me} = {2 \pi} {2} {{160 \, \text{N} {\cdot} \text{m}} \over {2000 \, \text{cm}^3}} = {2 \pi} {2} {{160 \, \text{N} \cancel{\cdot \text{m}}} \over {2000 \, \text{cm}^{{\cancel 3} 2}}}= 1.005 \, \text{MPa}</math>
:<math>p_\text{me} = {2 \pi} \cdot {0.5^{-1}} {{159 \, \text{N} {\cdot} \text{m}} \over {2000 \, \text{cm}^3}} = {2 \pi} \cdot {0.5^{-1}} {{15900 \, \text{N} \cancel{\cdot \text{cm}}} \over {2000 \, \text{cm}^{{\cancel 3} 2}}} \approx 100 \, N \cdot cm^{-2} = 1 \, \text{MPa}</math>


;Power from MEP and crankshaft speed
;Power from MEP and crankshaft speed
If we know the crankshaft speed, we can also determine the engine's power output from the MEP figure: <math>P= {V_\text{d} \cdot p_\text{me} \cdot N \over n_\text{c}}</math><br />
If we know the crankshaft speed, we can also determine the engine's power output from the MEP figure: <math>P=i \cdot n \cdot V_\text{d} \cdot p_\text{me}</math><br />
In our example, the engine puts out 160&nbsp;N·m of torque at 3600&nbsp;min<sup>&minus;1</sup>:
In our example, the engine puts out 159&nbsp;N·m of torque at 3600&nbsp;min<sup>&minus;1</sup> (=60&nbsp;s<sup>&minus;1</sup>):


*<math>n_\text{c}=2</math>
*<math>i=0.5</math>
*<math>N= 3600 \, \text{min}^{-1} = 60 \, \text{s}^{-1}</math>
*<math>n= 60 \, \text{s}^{-1}</math>
*<math>V_\text{d}=2000 \, \text{cm}^3</math>
*<math>V_\text{d}=2000 \, \text{cm}^3</math>
*<math>p_\text{me}= 1.005 \, \text{MPa}</math>
*<math>p_\text{me}= 1 \, \text{MPa}</math>
Thus:
<br />
:<math>{2000 \cdot 1.005 \cdot 60 \over 2}= 60,300 \, \text{W}</math>
:<math>P={2000 \, cm^{3} \cdot 1 \, N \cdot cm^{-2} \cdot 60 \, s^{-1} \cdot 0.5}= 60,000 \, N \cdot m \cdot s^{-1} = 60,000 \, \text{W} = 60 \, \text{kW}</math>


As piston engines usually have their maximum torque at a lower rotating speed than the maximum power output, the BMEP is lower at full power (at higher rotating speed). If the same engine is rated 76&nbsp;kW at 5400&nbsp;min<sup>&minus;1</sup> = 90&nbsp;s<sup>&minus;1</sup>, and its BMEP is 0.844&nbsp;MPa, we get the following equation:
As piston engines usually have their maximum torque at a lower rotating speed than the maximum power output, the BMEP is lower at full power (at higher rotating speed). If the same engine is rated 72&nbsp;kW at 5400&nbsp;min<sup>&minus;1</sup> = 90&nbsp;s<sup>&minus;1</sup>, and its BMEP is 0.80&nbsp;MPa, we get the following equation:


*<math>n_\text{c}=2</math>
*<math>i=0.5</math>
*<math>N= 5400 \, \text{min}^{-1} = 90 \, \text{s}^{-1}</math>
*<math>n= 90 \, \text{s}^{-1}</math>
*<math>V_\text{d}=2000 \, \text{cm}^3</math>
*<math>V_\text{d}=2000 \, \text{cm}^3</math>
*<math>p_\text{me}= 0.844 \, \text{MPa}</math>
*<math>p_\text{me}= 0.80 \, \text{MPa}</math>
Then:
<br />
:<math>{2000 \cdot 0.844 \cdot 90 \over 2}= 75,960 \, \text{W} \approx 76 \, \text{kW}</math>
:<math>P={2000 \, cm^{3} \cdot 0.80 \, N \cdot cm^{-2} \cdot 90 \, s^{-1} \cdot 0.5}= 72,000 \, N \cdot m \cdot s^{-1} = 72 \, \text{kW}</math>


==Types of mean effective pressures==
==Types of mean effective pressures==
Mean effective pressure (MEP) is defined by the location measurement and method of calculation, some commonly used MEPs are given here.
Mean effective pressure (MEP) is defined by the location measurement and method of calculation, some commonly used MEPs are given here:


* Brake mean effective pressure (BMEP) - Mean effective pressure calculated from measured brake torque.
* Brake mean effective pressure (BMEP, <math>p_{me}</math>) - Mean effective pressure calculated from measured brake torque.
* Indicated mean effective pressure (IMEP, <math>p_{mi}</math>) - Mean effective pressure calculated from in-cylinder pressure over the complete engine cycle (720° in a four-stroke, 360° in a two-stroke). IMEP may be determined by planimetering the area in an engine's [[Pressure–volume diagram|pV-diagram]]. Since naturally aspirated four-stroke engines must perform pumping work to suck the charge into the cylinder, and to remove the exhaust from the cylinder, IMEP may be split into the high-pressure, gross mean effective pressure (GMEP, <math>p_{mg}</math>) and the pumping mean effective pressure (PMEP, <math>p_{miGW}</math>). In naturally aspirated engines, PMEP is negative, and in super- or turbocharged engines, it is usually positive. IMEP may be derived from PMEP and GMEP: <math>p_{mi} = p_{mg}-p_{miGW}</math>.<ref name="Spicher_2017_24">Ulrich Spicher: ''Kapitel 3 · Kenngrößen – table 3.16: Effektiver Mitteldruck heutiger Motoren'', in Richard van Basshuysen, Fred Schäfer (eds.): ''Handbuch Verbrennungsmotor – Grundlagen · Komponenten · Systeme · Perspektiven'', 8th edition, Springer, Wiesbaden 2017, ISBN 978-3-658-10901-1, DOI 10.1007/978-3-658-10902-8_3, p. 24</ref>
* Gross indicated mean effective pressure (IMEP<sub>g</sub>) - Mean effective pressure calculated from in-cylinder pressure over compression and expansion portion of engine cycle (360° in a [[four-stroke]], 180° in a [[two-stroke]]). Direct measurement requires cylinder pressure sensing equipment.
* Friction mean effective pressure (FMEP, <math>p_{mr}</math>) - Theoretical mean effective pressure required to overcome engine friction, can be thought of as mean effective pressure lost due to friction: <math>p_{mr}=p_{mi}-p_{me}</math>. FMEP rises with an increase in engine speed.<ref>Ulrich Spicher: ''Kapitel 3 · Kenngrößen – table 3.16: Effektiver Mitteldruck heutiger Motoren'', in Richard van Basshuysen, Fred Schäfer (eds.): ''Handbuch Verbrennungsmotor – Grundlagen · Komponenten · Systeme · Perspektiven'', 8th edition, Springer, Wiesbaden 2017, ISBN 978-3-658-10901-1, DOI 10.1007/978-3-658-10902-8_3, p. 26, formula 3.48</ref>
* Net indicated mean effective pressure (IMEP<sub>n</sub>) - Mean effective pressure calculated from in-cylinder pressure over the complete engine cycle (720° in a four-stroke, 360° in a two-stroke). Direct measurement requires cylinder pressure sensing equipment.
* Pumping mean effective pressure (PMEP) - Mean effective pressure from work moving air in and out of the cylinder, across the intake and exhaust valves. Calculated from in-cylinder pressure over intake and exhaust portions of engine cycle (360° in a four-stroke, 0° in a two-stroke). Direct measurement requires cylinder pressure sensing equipment. PMEP = IMEP<sub>g</sub> - IMEP<sub>n</sub>.
* Friction mean effective pressure (FMEP) - Theoretical mean effective pressure required to overcome engine friction, can be thought of as mean effective pressure lost due to friction. Friction mean effective pressure calculation requires accurate measurement of cylinder pressure and dynamometer brake torque. FMEP = IMEP<sub>n</sub> - BMEP.


==BMEP typical values==
==BMEP typical values==
Line 112: Line 94:
|{{cvt|1.2|MPa|lbf/in2|1|abbr=on}}
|{{cvt|1.2|MPa|lbf/in2|1|abbr=on}}
|-
|-
|Race car engine (Formula 1)
|Race car engine (NA Formula 1)
|{{cvt|1.6|MPa|lbf/in2|1|abbr=on}}
|{{cvt|1.6|MPa|lbf/in2|1|abbr=on}}
|-
|-

Latest revision as of 23:05, 17 October 2024

Mean effective pressure
Common symbols
p
SI unitPascal (Pa)
In SI base units1 kgm−1s−2
Derivations from
other quantities
p = W·V−1
Dimension

The mean effective pressure (MEP) is a quantity relating to the operation of a reciprocating engine and is a measure of an engine's capacity to do work that is independent of engine displacement.[1] Despite having the dimension of pressure, MEP cannot be measured.[2] When quoted as an indicated mean effective pressure (IMEP), it may be thought of as the average pressure acting on a piston during the different portions of its cycle. When friction losses are subtracted from the IMEP, the result is the brake mean effective pressure (BMEP).

Derivation

[edit]

Let:

= power output in watt;
= mean effective pressure in megapascal;
= displacement volume in cubic centimetre;
= number of cycles per revolution (for a 4-stroke engine, , for a 2-stroke engine, );[Note 1]
= number of revolutions per second;
angular velocity, i.e. ;
= torque in newton-metre.

Then, BMEP may be used to determine an engine's power output as follows:

Since we know that power is:

We now see that, BMEP is a measure of expressing torque per displacement:

And thus, the equation for BMEP in terms of torque is:

Speed has dropped out of the equation, and the only variables are the torque and displacement volume. Since the range of maximum brake mean effective pressures for good engine designs is well established, we now have a displacement-independent measure of the torque-producing capacity of an engine design – a specific torque of sorts. This is useful for comparing engines of different displacements. Mean effective pressure is also useful for initial design calculations; that is, given a torque, standard MEP values can be used to estimate the required engine displacement. However, mean effective pressure does not reflect the actual pressures inside an individual combustion chamber – although the two are certainly related – and serves only as a convenient measure of performance.[2]

Brake mean effective pressure (BMEP) is calculated from measured dynamometer torque. Net indicated mean effective pressure (IMEP) is calculated using the indicated power; i.e., the pressure volume integral in the work per cycle equation. Sometimes the term FMEP (friction mean effective pressure) is used as an indicator of the mean effective pressure lost to friction (or friction torque) and is just the difference between IMEP and BMEP.[3]

Examples

[edit]
MEP from torque and displacement

A four-stroke engine produces 159 N·m of torque, and displaces 2000 cm3

Power from MEP and crankshaft speed

If we know the crankshaft speed, we can also determine the engine's power output from the MEP figure:
In our example, the engine puts out 159 N·m of torque at 3600 min−1 (=60 s−1):

Thus:

As piston engines usually have their maximum torque at a lower rotating speed than the maximum power output, the BMEP is lower at full power (at higher rotating speed). If the same engine is rated 72 kW at 5400 min−1 = 90 s−1, and its BMEP is 0.80 MPa, we get the following equation:

Then:

Types of mean effective pressures

[edit]

Mean effective pressure (MEP) is defined by the location measurement and method of calculation, some commonly used MEPs are given here:

  • Brake mean effective pressure (BMEP, ) - Mean effective pressure calculated from measured brake torque.
  • Indicated mean effective pressure (IMEP, ) - Mean effective pressure calculated from in-cylinder pressure over the complete engine cycle (720° in a four-stroke, 360° in a two-stroke). IMEP may be determined by planimetering the area in an engine's pV-diagram. Since naturally aspirated four-stroke engines must perform pumping work to suck the charge into the cylinder, and to remove the exhaust from the cylinder, IMEP may be split into the high-pressure, gross mean effective pressure (GMEP, ) and the pumping mean effective pressure (PMEP, ). In naturally aspirated engines, PMEP is negative, and in super- or turbocharged engines, it is usually positive. IMEP may be derived from PMEP and GMEP: .[3]
  • Friction mean effective pressure (FMEP, ) - Theoretical mean effective pressure required to overcome engine friction, can be thought of as mean effective pressure lost due to friction: . FMEP rises with an increase in engine speed.[4]

BMEP typical values

[edit]
BMEP typical values[5]
Engine type Typical max. BMEP
Motorbike engine 1.2 MPa (174.0 lbf/in2)
Race car engine (NA Formula 1) 1.6 MPa (232.1 lbf/in2)
Passenger car engine (naturally aspirated Otto) 1.3 MPa (188.5 lbf/in2)
Passenger car engine (turbocharged Otto) 2.2 MPa (319.1 lbf/in2)
Passenger car engine (turbocharged Diesel) 2.0 MPa (290.1 lbf/in2)
Lorry engine (turbocharged Diesel) 2.4 MPa (348.1 lbf/in2)
High-speed industrial Diesel engine 2.8 MPa (406.1 lbf/in2)
Medium-speed industrial Diesel engine 2.5 MPa (362.6 lbf/in2)
Low-speed two-stroke Diesel engine 1.5 MPa (217.6 lbf/in2)

See also

[edit]

Notes and references

[edit]

Notes

[edit]
  1. ^ Wankel engines are four-stroke engines, so ; the displacement is derived from the chamber volume by multiplying it with the number of rotary pistons and 2: (see Wolf-Dieter Bensinger: Rotationskolben-Verbrennungsmotoren, Springer, Berlin/Heidelberg/New York 1973, ISBN 978-3-642-52174-4, p. 66)

References

[edit]
  1. ^ Heywood, J. B., "Internal Combustion Engine Fundamentals", McGraw-Hill Inc., 1988, p. 50
  2. ^ a b Schreiner, Klaus (2011-05-25). Basiswissen Verbrennungsmotor (in German). Wiesbaden: Vieweg+Teubner Verlag. p. 41. ISBN 978-3-8348-1279-7.
  3. ^ a b Ulrich Spicher: Kapitel 3 · Kenngrößen – table 3.16: Effektiver Mitteldruck heutiger Motoren, in Richard van Basshuysen, Fred Schäfer (eds.): Handbuch Verbrennungsmotor – Grundlagen · Komponenten · Systeme · Perspektiven, 8th edition, Springer, Wiesbaden 2017, ISBN 978-3-658-10901-1, DOI 10.1007/978-3-658-10902-8_3, p. 24
  4. ^ Ulrich Spicher: Kapitel 3 · Kenngrößen – table 3.16: Effektiver Mitteldruck heutiger Motoren, in Richard van Basshuysen, Fred Schäfer (eds.): Handbuch Verbrennungsmotor – Grundlagen · Komponenten · Systeme · Perspektiven, 8th edition, Springer, Wiesbaden 2017, ISBN 978-3-658-10901-1, DOI 10.1007/978-3-658-10902-8_3, p. 26, formula 3.48
  5. ^ Ulrich Spicher: Kapitel 3 · Kenngrößen – table 3.16: Effektiver Mitteldruck heutiger Motoren, in Richard van Basshuysen, Fred Schäfer (eds.): Handbuch Verbrennungsmotor – Grundlagen · Komponenten · Systeme · Perspektiven, 8th edition, Springer, Wiesbaden 2017, ISBN 978-3-658-10901-1, DOI 10.1007/978-3-658-10902-8_3, p. 27
[edit]