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Carburetor Theory
Variable Venturi or “slide”
carburetors
  The goal of providing

  the stochiometric
  ratio, (14.7:1) is
  tempered with the
  goal of providing
  extra fuel to cool (by
  evaporation) the
  engine.
 Carburetor tuning
  must be done to
  provide max power
  without overheating
  the 2 stroke engine.
VM Carburetor
    Slide carburetor

    provides smoother
    variation and better
    adjustment than a
    throttle plate
    carburetor.
    VM is a Mikuni round

    slide carburetor.
    Various circuits control

    fuel and air flow for
    different conditions
    ◦ Starting, (idle) pilot, and
      main
Integrated carburetor systems
    The carburetor has

    multiple adjustments
    for different throttle
    positions;
    ◦ 0-1/4 Pilot jet
    ◦ 1/8-1/2 Throttle cutaway
    ◦ ¼-3/4 Jet needle (clip)
    ◦ ¼-3/4 Needle jet
    ◦ ½-Full Main jet
    ◦ ½-Full Air adjustment
      screw
    ◦ ½-full Power jet
      (optional)
Starter Circuit
  Mini- slide carburetor

  used for starting
 “Choking” the
  carburetor actually
  opens plunger to
  allow gas flow
 Gas is drawn from the
  bottom of the bowl
  through a starter jet
 Air is drawn from in
  front of the slide
Starter circuit
Starter Circuit
  Starter can only function when slide is

  closed and vacuum is high
 Starter jet may need to be changed if
  using a snowmobile carb on a
  motorcycle, or vice-versa
 Plunger positions – Open
  (choked), half-open, closed
 Starter circuit can be used to enrichen
  mixture at other times to check
  carburetor problems.
Pilot circuit
    Used at idle to ¼

    throttle
    Gas flow is controlled

    by pilot jet size, this jet
    is the first to plug if gas
    thickens
    Air flow is controlled by

    air adjustment needle
    At idle, air flows in at 5

    to further mix with fuel
    At just off idle, mixed

    fuel-air flows out at both
Pilot Circuit
  Stumble coming off

  idle indicates plugged
  pilot jet or air screw
  too tight
 Idle speed controlled
  by a separate screw
  that determines how
  tightly the slide
  closes.
 Slides with different
  shape cutouts are
  also sold for tuning
  applications.
Mid range operation
  ¼ to ¾ operation is

  controlled by needle
  jet and jet needle. As
  slide pulls up the long
  tapered needle is
  drawn out of needle
  jet.
 The air jet controls
  the air bled in to
  atomize the fuel.
 The main jet is so
  large that it does not
  limit flow
Mid range operation
  Both needle jet and

  jet needles can be
  changed, as can the
  position of the clip on
  the end of the needle.
 Needles can have up
  to four different tapers
  on them for different
  performance
  throughout the slide
  travel.
Tuning
  Simple tuning can

  begin with moving the
  needle up or down
  one clip position.
  This can be done
  before changing
  needles or needle
  jets.
 Any tuning
  adjustments should
  be made by stepping
  jets up or down one
  size at a time.
Full throttle operation
    At ¾ to full throttle, the

    needle is so far
    removed from the
    needle jet, that it no
    longer limits flow.
    At this throttle

    range, the main jet
    limits gas flow.
    Air jet limits air flow.

    Always jet main rich

    and work down.
    Air jet is typically not

Power jets
    Not found on all carbs – Provides richer mix at

    top end
Jetting adjustments
    To make proper

    carburetor
    adjustments the
    mixture ratio at each
    range will have to be
    determined. There
    are various methods:
    Plug reading – plug

    chop
    Piston wash

    Pyrometer readings

    Condition corrections

Plug Reading – Plug Chop
    To get an accurate read

    of the condition, perform
    a “plug chop”
    ◦ Install a new plug
    ◦ Warm engine up
    ◦ Run engine at selected
      throttle setting for 30
      seconds – 1 minute.
    ◦ Cut ignition and
      simultaneously close-off
      carb
    ◦ Study insulator down
      toward the base of the
      insulator, not on the tip!
    ◦ Appearance of tip better for
      determining detonation
Plug appearance
Center electrodes
    Another valuable indicator on

    the spark plug is the center
    firing electrode; as the plug
    color starts to lighten up when
    properly jetted, the center
    firing electrode will start to
    have a “silver” tip, or crown. As
    the mixture becomes
    leaner, this silver crown will
    start to creep down the side of
    the electrode; this is your
    target. This metallic
    appearance on the end of the
    electrode should not extend
    any further than 1/4 - 1/3 of the
    way down the tip. Many tuners
    are happy with the margin
    afforded by simply seeing the
    silver tip; then they’re close
    enough for trail riding with a bit
    of margin to spare.
Side electrode
    The ground electrode is

    also an indicator; on
    many engines you will
    see a “shadow” (darker
    area) just up to the radius
    (bend) that will usually
    coincide with the color
    and firing electrode
    appearance. If this
    shadow is further down
    the ground strap towards
    the plug threads, you’re
    likely too lean. If this dark
    shadow is all the way
    across the strap to the
    center of the plug, you’re
    too rich.
NGK plug numbering system
    The plug heat range can be

    adjusted to keep a plug tip
    clean, or avoid detonating on
    an engine that otherwise has
    the right mixture.
    For NGK and most foreign

    manufacturer’s spark plugs
    there is a simple rule of
    thumb:Low heat rating number
    (for inst. BP4ES) quot;Hot spark
    plugquot;.high heat intake due to
    long insulator tip.
    .High heat rating number (for

    inst. BP8ES) quot;Cold spark
    plugquot;.Low heat intake, due to
    short insulator tip.
    For Champion and most

    domestic manufacturer’s spark
    plugs (e.g. in ATVs, the
    numbering is opposite.
Piston reading




    Normally done for an engine that has been run for ¼

    mile at constant speed. By looking down the spark
    plug hole with piston at BDC, a clear look at the top
    of the piston can determine how much carbon is left.
    A ½” ring of wash (clean) is “normal”, typically a
    little variation at transfer and exhaust ports will be
    noted.
Exhaust gas pyrometers
    Uses the Exhaust

    temperature as a check
    on mixture, and relative
    changes, not for baseline
    tuning. Thermocouples
    are typically installed
    permanently 5-10” from
    exhaust port and they
    must be centered in pipe.
    Manufacturers will often
    give you an exact
    location.
Interpreting EGT values
    Each gauge is used

    for relative readings
    ◦ Guidelines
      Below 1100 – Rich
      1200-Ideal
      Above 1250 Lean
    Changing a Mikuni
     carburetor jet one size
     will cause about a 50
     degree temperature
     change
Relative Air Density correction
    Once an ideal jetting has

    been developed for one
    condition, it will need to
    be corrected for changing
    environmental conditions:
    ◦ Temperature (Loss of 2%
      per 10 degree F increase)
    ◦ Altitude (loss of 3.5% per
      1000’ increase)
    ◦ Barometric pressure
    ◦ Relative Humidity – Moist
      air is less dense
Relative Air density
calculations
    Calculating Air Density

    Air density is expressed in units of mass per unit volume, in this

    case kg/m3. The formula for this calculation is derived from basic
    physics.
    Air Density (kg/m3) = 1.2929 * (273.13/(T+273.13)) * ((P-

    MN*RH)/760)
    Simplified = 0.46464*(P-MN*RH)/(T+273.13)

    where

    T = temperature in Celsius

    P = barometric pressure in mm of mercury

    MN = moisture number from the following chart - include chart

    RH = relative humidity, expressed as a decimal (0.55, not 55%)

    For example:

    T = 13C

    P = 770 mmHg

    MN per the chart for 13C is 11.24

    RH = .21 (21%)

    Air Density = 1.25 kg/m3

Relative air density use
    In simple form, the change in relative air density

    corresponds to the change in jet size.
    ◦ e.g. – If relative air density goes from 100 to 103 (a 3
      % change) the jet size should increase by 3%. If you
      are using a 300 jet, the new jet size will be (300 x
      1.03) = 309. Since jets only come in multiples of
      5, you could use a 310.
       Jetting changes in direct proportion to changes in absolute
        temp on the Rankine scale (460 + Farenheit temp)
       Jetting changes only 70% as much as absolute barometric
        pressure changes. This is due to the fact that the bowl is
        vented, and less pressure is exerted on the gas in the bowl as
        well
       Hex head jets are marked in area, round head jets in diameter.
Correcting jet size for RAD
    For instance, if you get the jetting perfect at AD = 1.05

    and the air density changes to 1.08, you know that you
    will need to go up at least one size. If it goes from 1.05
    to 1.06, is it time to change a jet or not? This is why you
    need to check all the way through the range. I know that
    for my bike, AD = 1.03-1.05 is one jet size and 1.06-1.08
    is the next size up. In the above example, I would have
    known to go up one size. If it had gone up to 1.08 and
    looked like it was going to continue rising, I would go up
    two sizes.
Engine sound
  An engine running

  way too rich will “four
  cycle” or miss ignition
  on every other stroke.
 An engine running
  way too lean will be
  running very fast and
  not return to idle
TM Carburetor
  TM is a flat slide carb

 Less disruption of air
  flow in venturi gives
  carbs better response
  and power.
 Rack mounted for
  twins and triples
  reduce throttle
  effort, and are held in
  synchronization
 Circuits similar to VM
Mikuni CV Carb
  Used on four

  strokes, this is a
  “Constant Velocity” or
  “Constant Vacuum”
  carb.
 Butterfly throttle is
  combined with a slide
  to give the carb good
  response to quick
  throttle opening.
 Butterfly controlled by
  operator, Slide is
  controlled by vacuum
CV Carb Operation
    Operator controls

    butterfly from idle to ¼
    throttle, during this slide
    is held ¼ open
    Past ¼ throttle, the

    engine vacuum is applied
    to the slide, and the slide
    movement is controlled
    by vacuum
    Slide will not open until

    sufficient engine vacuum
    has been developed.
    Opening throttle quickly

    will not produce “flat spot”
    Setting Idle speed too

    high will cause carburetor
    to “hang”, or not return to
    idle
Carburetor size
                                 Carburetor Throttle
                             
    Carburetor size must

                                 Bore Diameter
    be matched to flow
                                 D = K x SQRT( C x N )
                             
    for displacement and
                                 D is throttle bore
                             
    rpms that engine is
                                 diameter, in millimeters
    used. Changing
                                 K is a constant (
                             
    either will require an       approx. 0.65 to 0.9,
    adjustment to the            derive from existing
    carburetor to match.         carburetor bore)
                                 C is cylinder
                             
                                 displacement, in liters
                                 N is RPM at peak
                             
                                 power
Tuned intake
                              Resonance Effects
                          
    Intake (airbox) can

    also be “tuned” to         F = Vs / 2¼ * the square
                          
                              root of A / Vc (L + 1/2 the
    match resonance of
                              square root of ¼ A
    intake with peak
                              Vs is the sonic speed
                          
    power band.               Usually about 1100 ft/sec)
                              A is the cross-sectional
                          
                              area of the inlet
                              L is the inlet pipe length
                          
                              Vc is the flask (crankcase)
                          
                              volume
Ignition safety
    To avoid having the

    slides freeze open and
    customer stuck on a
    runaway sled, the safety
    switch on the side of carb
    measures a magnet on
    the slide to be sure the
    slide closes when throttle
    is released.
    When replacing throttle

    cable, BE SURE TO SET
    FREE PLAY or engine
    may not start

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Carburetor Theory

  • 2. Variable Venturi or “slide” carburetors The goal of providing  the stochiometric ratio, (14.7:1) is tempered with the goal of providing extra fuel to cool (by evaporation) the engine.  Carburetor tuning must be done to provide max power without overheating the 2 stroke engine.
  • 3. VM Carburetor Slide carburetor  provides smoother variation and better adjustment than a throttle plate carburetor. VM is a Mikuni round  slide carburetor. Various circuits control  fuel and air flow for different conditions ◦ Starting, (idle) pilot, and main
  • 4. Integrated carburetor systems The carburetor has  multiple adjustments for different throttle positions; ◦ 0-1/4 Pilot jet ◦ 1/8-1/2 Throttle cutaway ◦ ¼-3/4 Jet needle (clip) ◦ ¼-3/4 Needle jet ◦ ½-Full Main jet ◦ ½-Full Air adjustment screw ◦ ½-full Power jet (optional)
  • 5. Starter Circuit Mini- slide carburetor  used for starting  “Choking” the carburetor actually opens plunger to allow gas flow  Gas is drawn from the bottom of the bowl through a starter jet  Air is drawn from in front of the slide
  • 7. Starter Circuit Starter can only function when slide is  closed and vacuum is high  Starter jet may need to be changed if using a snowmobile carb on a motorcycle, or vice-versa  Plunger positions – Open (choked), half-open, closed  Starter circuit can be used to enrichen mixture at other times to check carburetor problems.
  • 8. Pilot circuit Used at idle to ¼  throttle Gas flow is controlled  by pilot jet size, this jet is the first to plug if gas thickens Air flow is controlled by  air adjustment needle At idle, air flows in at 5  to further mix with fuel At just off idle, mixed  fuel-air flows out at both
  • 9. Pilot Circuit Stumble coming off  idle indicates plugged pilot jet or air screw too tight  Idle speed controlled by a separate screw that determines how tightly the slide closes.  Slides with different shape cutouts are also sold for tuning applications.
  • 10. Mid range operation ¼ to ¾ operation is  controlled by needle jet and jet needle. As slide pulls up the long tapered needle is drawn out of needle jet.  The air jet controls the air bled in to atomize the fuel.  The main jet is so large that it does not limit flow
  • 11. Mid range operation Both needle jet and  jet needles can be changed, as can the position of the clip on the end of the needle.  Needles can have up to four different tapers on them for different performance throughout the slide travel.
  • 12. Tuning Simple tuning can  begin with moving the needle up or down one clip position. This can be done before changing needles or needle jets.  Any tuning adjustments should be made by stepping jets up or down one size at a time.
  • 13. Full throttle operation At ¾ to full throttle, the  needle is so far removed from the needle jet, that it no longer limits flow. At this throttle  range, the main jet limits gas flow. Air jet limits air flow.  Always jet main rich  and work down. Air jet is typically not 
  • 14. Power jets Not found on all carbs – Provides richer mix at  top end
  • 15. Jetting adjustments To make proper  carburetor adjustments the mixture ratio at each range will have to be determined. There are various methods: Plug reading – plug  chop Piston wash  Pyrometer readings  Condition corrections 
  • 16. Plug Reading – Plug Chop To get an accurate read  of the condition, perform a “plug chop” ◦ Install a new plug ◦ Warm engine up ◦ Run engine at selected throttle setting for 30 seconds – 1 minute. ◦ Cut ignition and simultaneously close-off carb ◦ Study insulator down toward the base of the insulator, not on the tip! ◦ Appearance of tip better for determining detonation
  • 18. Center electrodes Another valuable indicator on  the spark plug is the center firing electrode; as the plug color starts to lighten up when properly jetted, the center firing electrode will start to have a “silver” tip, or crown. As the mixture becomes leaner, this silver crown will start to creep down the side of the electrode; this is your target. This metallic appearance on the end of the electrode should not extend any further than 1/4 - 1/3 of the way down the tip. Many tuners are happy with the margin afforded by simply seeing the silver tip; then they’re close enough for trail riding with a bit of margin to spare.
  • 19. Side electrode The ground electrode is  also an indicator; on many engines you will see a “shadow” (darker area) just up to the radius (bend) that will usually coincide with the color and firing electrode appearance. If this shadow is further down the ground strap towards the plug threads, you’re likely too lean. If this dark shadow is all the way across the strap to the center of the plug, you’re too rich.
  • 20. NGK plug numbering system The plug heat range can be  adjusted to keep a plug tip clean, or avoid detonating on an engine that otherwise has the right mixture. For NGK and most foreign  manufacturer’s spark plugs there is a simple rule of thumb:Low heat rating number (for inst. BP4ES) quot;Hot spark plugquot;.high heat intake due to long insulator tip. .High heat rating number (for  inst. BP8ES) quot;Cold spark plugquot;.Low heat intake, due to short insulator tip. For Champion and most  domestic manufacturer’s spark plugs (e.g. in ATVs, the numbering is opposite.
  • 21. Piston reading Normally done for an engine that has been run for ¼  mile at constant speed. By looking down the spark plug hole with piston at BDC, a clear look at the top of the piston can determine how much carbon is left. A ½” ring of wash (clean) is “normal”, typically a little variation at transfer and exhaust ports will be noted.
  • 22. Exhaust gas pyrometers Uses the Exhaust  temperature as a check on mixture, and relative changes, not for baseline tuning. Thermocouples are typically installed permanently 5-10” from exhaust port and they must be centered in pipe. Manufacturers will often give you an exact location.
  • 23. Interpreting EGT values Each gauge is used  for relative readings ◦ Guidelines  Below 1100 – Rich  1200-Ideal  Above 1250 Lean Changing a Mikuni carburetor jet one size will cause about a 50 degree temperature change
  • 24. Relative Air Density correction Once an ideal jetting has  been developed for one condition, it will need to be corrected for changing environmental conditions: ◦ Temperature (Loss of 2% per 10 degree F increase) ◦ Altitude (loss of 3.5% per 1000’ increase) ◦ Barometric pressure ◦ Relative Humidity – Moist air is less dense
  • 25. Relative Air density calculations Calculating Air Density  Air density is expressed in units of mass per unit volume, in this  case kg/m3. The formula for this calculation is derived from basic physics. Air Density (kg/m3) = 1.2929 * (273.13/(T+273.13)) * ((P-  MN*RH)/760) Simplified = 0.46464*(P-MN*RH)/(T+273.13)  where  T = temperature in Celsius  P = barometric pressure in mm of mercury  MN = moisture number from the following chart - include chart  RH = relative humidity, expressed as a decimal (0.55, not 55%)  For example:  T = 13C  P = 770 mmHg  MN per the chart for 13C is 11.24  RH = .21 (21%)  Air Density = 1.25 kg/m3 
  • 26. Relative air density use In simple form, the change in relative air density  corresponds to the change in jet size. ◦ e.g. – If relative air density goes from 100 to 103 (a 3 % change) the jet size should increase by 3%. If you are using a 300 jet, the new jet size will be (300 x 1.03) = 309. Since jets only come in multiples of 5, you could use a 310.  Jetting changes in direct proportion to changes in absolute temp on the Rankine scale (460 + Farenheit temp)  Jetting changes only 70% as much as absolute barometric pressure changes. This is due to the fact that the bowl is vented, and less pressure is exerted on the gas in the bowl as well  Hex head jets are marked in area, round head jets in diameter.
  • 27. Correcting jet size for RAD For instance, if you get the jetting perfect at AD = 1.05  and the air density changes to 1.08, you know that you will need to go up at least one size. If it goes from 1.05 to 1.06, is it time to change a jet or not? This is why you need to check all the way through the range. I know that for my bike, AD = 1.03-1.05 is one jet size and 1.06-1.08 is the next size up. In the above example, I would have known to go up one size. If it had gone up to 1.08 and looked like it was going to continue rising, I would go up two sizes.
  • 28. Engine sound An engine running  way too rich will “four cycle” or miss ignition on every other stroke.  An engine running way too lean will be running very fast and not return to idle
  • 29. TM Carburetor TM is a flat slide carb   Less disruption of air flow in venturi gives carbs better response and power.  Rack mounted for twins and triples reduce throttle effort, and are held in synchronization  Circuits similar to VM
  • 30. Mikuni CV Carb Used on four  strokes, this is a “Constant Velocity” or “Constant Vacuum” carb.  Butterfly throttle is combined with a slide to give the carb good response to quick throttle opening.  Butterfly controlled by operator, Slide is controlled by vacuum
  • 31. CV Carb Operation Operator controls  butterfly from idle to ¼ throttle, during this slide is held ¼ open Past ¼ throttle, the  engine vacuum is applied to the slide, and the slide movement is controlled by vacuum Slide will not open until  sufficient engine vacuum has been developed. Opening throttle quickly  will not produce “flat spot” Setting Idle speed too  high will cause carburetor to “hang”, or not return to idle
  • 32. Carburetor size Carburetor Throttle  Carburetor size must  Bore Diameter be matched to flow D = K x SQRT( C x N )  for displacement and D is throttle bore  rpms that engine is diameter, in millimeters used. Changing K is a constant (  either will require an approx. 0.65 to 0.9, adjustment to the derive from existing carburetor to match. carburetor bore) C is cylinder  displacement, in liters N is RPM at peak  power
  • 33. Tuned intake Resonance Effects  Intake (airbox) can  also be “tuned” to F = Vs / 2¼ * the square  root of A / Vc (L + 1/2 the match resonance of square root of ¼ A intake with peak Vs is the sonic speed  power band. Usually about 1100 ft/sec) A is the cross-sectional  area of the inlet L is the inlet pipe length  Vc is the flask (crankcase)  volume
  • 34. Ignition safety To avoid having the  slides freeze open and customer stuck on a runaway sled, the safety switch on the side of carb measures a magnet on the slide to be sure the slide closes when throttle is released. When replacing throttle  cable, BE SURE TO SET FREE PLAY or engine may not start