Carburetor Theory


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Carburetor Theory

  1. 1. Carburetor Theory
  2. 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. 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. 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. 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
  6. 6. Starter circuit
  7. 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. 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. 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. 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. 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. 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. 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. 14. Power jets Not found on all carbs – Provides richer mix at  top end
  15. 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. 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
  17. 17. Plug appearance
  18. 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. 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. 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. 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. 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. 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. 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. 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. 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. 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. 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. 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. 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. 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. 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. 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. 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