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Indicator Diagrams and Internal Combustion Engine Performance Parameters

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Title: Indicator Diagrams and Internal Combustion Engine Performance Parameters


1
Indicator Diagrams and Internal Combustion
EnginePerformance Parameters
  • Much can be learned from a record of the cylinder
    pressure and volume. The results can be analyzed
    to reveal the rate at which work is being done by
    the gas on the piston, and the rate at which
    combustion is occurring. In its simplest form,
    the cylinder pressure is plotted against volume
    to give an indicator diagram.

2
Pressure-Volume Graph 4-stroke SI engine One
power stroke for every two crank shaft revolutions
Pressure
Spark
Exhaust valve opens
Exhaust valve closes
Intake valve closes
1 atm
Intake valve opens
TC
BC
Cylinder volume
3
Efficiency
  • In general, energy conversion efficiency is the
    ratio between the useful output of a device and
    the input. For thermal efficiency, the input, to
    the device is heat, or the heat-content of a fuel
    that is consumed. The desired output is
    mechanical work, or heat, or possibly both.
    Because the input heat normally has a real
    financial cost, a memorable, generic definition
    of thermal efficiency is

4
  • When expressed as a percentage, the thermal
    efficiency must be between 0 and 100. Due to
    inefficiencies such as friction, heat loss, and
    other factors, thermal engines' efficiencies are
    typically much less than 100. For example, a
    typical gasoline automobile engine operates at
    around 25 efficiency. The largest diesel engine
    in the world peaks at 51.7.

5
  • Work done on the piston due to pressure

6
  • The term indicated work is used to define the net
    work done on the piston per cycle
  • the indicated mean effective pressure (imep),can
    be defined by

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  • The imep is a hypothetical pressure that would
    produce the same indicated work if it were to act
    on the piston throughout the expansion stroke.
    The concept of imep is useful because it
    describes the thermodynamic performance of an
    engine, in a way that is independent of engine
    size and speed and frictional losses.
  • Unfortunately, not all the work done by the gas
    on the piston is available as shaft work because
    there are frictional losses in the engine. These
    losses can be quantified by the brake mean
    effective pressure (bmep,), a hypothetical
    pressure that acts on the piston during the
    expansion stroke and would lead to the same brake
    work output in a frictionless engine.

9
Mechanical Efficiency
Some of the power generated in the cylinder is
used to overcome engine friction and to pump gas
into and out of the engine. The term friction
power, , is used to describe collectively
these power losses, such that
Friction power can be measured by motoring the
engine. The mechanical efficiency is defined as
10
Mechanical Efficiency, contd
  • Mechanical efficiency depends on pumping losses
    (throttle position) and
  • frictional losses (engine design and engine
    speed).
  • Typical values for automobile engines at WOT
    are
  • 90 _at_2000 RPM and 75 _at_ max speed.
  • Throttling increases pumping power and thus the
    mechanical efficiency
  • decreases, at idle the mechanical efficiency
    approaches zero.

11
  • Brake Specific Fuel Consumption (BSFC) is a
    measure of fuel efficiency within a
    shaft reciprocating engine. It is the rate
    of fuel consumption divided by the power produced.
    Specific fuel consumption is based on the torque
    delivered by the engine in respect to the fuel
    mass flow delivered to the engine. Measured after
    all parasitic engine losses is brake specific
    fuel consumption BSFC and measuring specific
    fuel consumption based on the in-cylinder
    pressures (ability of the pressure to do work) is
    indicated specific fuel consumption ISFC.

12
  • The final parameter to be defined is the
    volumetric efficiency of the engine the ratio of
    actual air flow to that of a perfect engine is
  • In general, it is quite easy to provide an engine
    with extra fuel therefore, the power output of
    an engine will be limited by the amount of air
    that is admitted to an engine.

13
The Ideal Air Standard Otto Cycle
14
  • Systems which are thermally insulated from their
    surroundings undergo processes without any heat
    transfer such processes are called adiabatic.
    Thus during an isentropic process there are no
    dissipative effects and the system neither
    absorbs nor gives off heat.
  • A reversible process, is a process that can be
    "reversed" by means of infinitesimal changes in
    some property of the system without loss
    or dissipation of energy.
  • Isentropic process is a process which is a
    process is both adiabatic and reversible .

15
  • A closed cylinder with a locked piston contains
    air. The pressure inside is equal to the outside
    air pressure. This cylinder is heated to a
    certain target temperature. Since the piston
    cannot move, the volume is constant, while
    temperature and pressure rise. When the target
    temperature is reached, the heating is stopped.
    The piston is now freed and moves outwards,
    expanding without exchange of heat (adiabatic
    expansion). Doing this work cools the air inside
    the cylinder to below the target temperature. To
    return to the target temperature (still with a
    free piston), the air must be heated. This extra
    heat amounts to about 40 more than the previous
    amount added. In this example, the amount of heat
    added with a locked piston is proportional to CV,
    whereas the total amount of heat added is
    proportional to CP. Therefore, the heat capacity
    ratio in this example is 1.4

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The Ideal Air Standard Diesel Cycle
18
Efficiencies of Real Engines
  • The efficiencies of real engines are below those
    predicted by the ideal air standard cycles for
    several reasons. Most significantly, the gases in
    internal combustion engines do not behave
    perfectly with a ratio of heat capacities.

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  • Consider a spark ignition engine with a
    compression ratio of 10, for which the Otto cycle
    efficiency predicts an efficiency of 60 and the
    fuel-air cycle predicts an efficiency of 47 for
    stoichiometric operation. In reality, such an
    engine might have a full throttle brake
    efficiency of 30, and this means 17 percentage
    points must be accounted

21
Ignition and Combustion in Spark Ignitionand
Diesel Engines
  • Spark ignition (SI) engines usually have
    pre-mixed combustion, in which a flame front
    initiated by a spark propagates across the
    combustion chamber through the unburned mixture.
    Compression ignition (CI) engines normally inject
    their fuel toward the end of the compression
    stroke, and the combustion is controlled
    primarily by diffusion.
  • Whether combustion is pre-mixed (as in SI
    engines) or diffusion controlled (as in CI
    engines) has a major influence on the range of
    air-fuel ratios (AFRs) that will burn.
  • In pre-mixed combustion, the AFR must be close to
    stoichiometric-the AFR value that is chemically
    correct for complete combustion. In practice,
    dissociation and the limited time available for
    combustion will mean that even with the
    stoichiometric AFR, complete combustion will not
    occur.
  • In diffusion combustion, much weaker AFRs can be
    used (i.e., an excess of air) because around each
    fuel droplet will be a range of flammable AFRs.
  • Typical ranges for the (gravimetric) air-fuel
    ratio are as follows

22
  • Diesel engines have a higher maximum
    efficiency than spark ignition engines for three
    reasons
  • 1. The compression ratio is higher.
  • 2. During the initial part of compression, only
    air is present.
  • 3. The air-fuel mixture is always weak of
    stoichiometric.

23
Simple Combustion Equilibrium
  • For a given combustion device, say a piston
    engine, how much fuel and air should be injected
    in order to completely burn both? This question
    can be answered by balancing the combustion
    reaction equation for a particular fuel. A
    stoichiometric mixture contains the exact amount
    of fuel and oxidizer such that after combustion
    is completed, all the fuel and oxidizer are
    consumed to form products.

24
  • Combustion stoichiometry for a general
    hydrocarbon fuel, with air can be expressed as
  • The amount of air required for combusting a
    stoichiometric mixture is called stoichiometric
    or theoretical air.

25
Methods of Quantifying Fuel and Air Contentof
Combustible Mixtures
  • In practice, fuels are often combusted with an
    amount of air different from the stoichiometric
    ratio. If less air than the stoichiometric amount
    is used, the mixture is described as fuel rich.
    If excess air is used, the mixture is described
    as fuel lean. For this reason, it is convenient
    to quantify the combustible mixture using one of
    the following commonly used methods
  • Fuel-Air Ratio (FAR) The fuel-air ratio, f, is
    given by

26
  • Equivalence Ratio Normalizing the actual
    fuel-air ratio by the stoichiometric fuel air
    ratio gives the equivalence ratio,
  • The subscript s indicates a value at the
    stoichiometric condition. f lt1 is a lean mixture
    , f¼1 is a stoichiometric mixture, and f gt1 is a
    rich mixture
  • Lambda is the ratio of the actual air-fuel ratio
    to the stoichiometric air-fuel ratio defined as

27
Fuel Requirements
  • Gasoline is a mixture of hydrocarbons (with 4 to
    approximately 12 carbon atoms) and a boiling
    point range of approximately 30-200C. Diesel
    fuel is a mixture of higher molarmass
    hydrocarbons (typically 12 to 22 carbon atoms),
    with a boiling point range of approximately180-380
    C. Fuels for spark ignition engines should
    vaporize readily and be resistant to
    self-ignition, as indicated by a high octane
    rating. In contrast, fuels for compression
    ignition engines should self-ignite readily, as
    indicated by a high cetane number.

28
  • Octane number is a standard measure of the
    anti-knock properties (i.e. the performance) of a
    motor or aviation fuel. The higher the octane
    number, the more compression the fuel can
    withstand before detonating. In broad terms,
    fuels with a higher octane rating are used in
    high-compression engines that generally have
    higher performance.
  • Knocking (also called knock, detonation, spark
    knock, pinging or pinking) in spark-ignition
    internal combustion engines occurs when
    combustion of the air/fuel mixture in the
    cylinder starts off correctly in response to
    ignition by the spark plug, Effects of engine
    knocking range from inconsequential to completely
    destructive.
  • .

29
  • Cetane number or CN is a measurement of the
    combustion quality of diesel fuel during
    compression ignition. It is a significant
    expression of diesel fuel quality among a number
    of other measurements that determine overall
    diesel fuel quality.

30
  • The octane or cetane rating of a fuel is
    established by comparing its ignition quality
    with respect to reference fuels in CFR
    (Co-operative Fuel Research) engines, according
    to internationally agreed standards. The most
    common type of octane rating worldwide is the
    Research Octane Number (RON). RON is determined
    by running the fuel in a test engine with a
    variable compression ratio under controlled
    conditions, and comparing the results with those
    for mixtures of iso-octane and n-heptane.

31
Engine Configuration
  • After the type and size of engine have been
    determined, the number and disposition of the
    cylinders must be decided. The main constraints
    influencing the number and disposition of the
    cylinders are as follows
  • 1. The number of cylinders needed to produce a
    steady output
  • 2. The minimum swept volume for efficient
    combustion
  • 3. The number and disposition of cylinders for
    satisfactory balancing
  • 4. The number of cylinders needed for an
    acceptable variation in the torque output

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  • The "V" engines form a very compact power unit. A
    more compact arrangement is the "H" configuration
    (in effect, two horizontally opposed engines with
    the crankshafts geared together), but this is an
    expensive and complicated arrangement that has
    had limited use. Whatever the arrangement, it is
    unusual to have more than six or eight cylinders
    in a row because torsional vibrations in the
    crankshaft then become much more troublesome.
    Nonetheless, the final decision on the engine
    configuration also will be influenced by
    marketing, packaging, and manufacturing
    constraints.

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