Airbox Mod explained (includes diagrams)
Last edited by Corpsie; Jan 25, 2002 at 03:35 PM.
Interesting stuff... do you have any diagrams of stock airbox and modified air box at the same throttle setting? The pics you have are mixing apples and oranges, and I'd like to see the effects of the air box mod at the same part throttle as the stocker.
Thanks
Thanks
Airbox
Corpsie,
Thanks for the info, very interesting. I have to agree with BeastRider about the "apples and oranges" thing. Maybe I'm missing something or don't understand the assumptions but wouldn't it be better to show the graphs of modified and stock airbox at WOT and part throttle. Please explain. TIA
Thanks for the info, very interesting. I have to agree with BeastRider about the "apples and oranges" thing. Maybe I'm missing something or don't understand the assumptions but wouldn't it be better to show the graphs of modified and stock airbox at WOT and part throttle. Please explain. TIA
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easy airbox mod
I have a much easier air box mod explaination. Take a look at my gallery and do what I did to your truck, then start it up, point it in a safe direction, and FLOOR IT! That's all the explaination that I need. :-)
cajun
cajun
I'm a little confused. Looking at your diagrams, as I recall, specific volume is the reciprocal of density. At BDC, both diagrams indicate the same specific volume, the air would, therefore, have to have the same density in both cases.
The pressure in "a" certainly is higher than the pressure in "b."
From the ideal gas law we also know that density=pressure/(specific gas constant x absolute temperature). If density a = density b and pressure a >pressure b, then temperature a > temperature b.
So I must be missing something, because to me, "a" is just hotter than "b."
Don't get me wrong I generally agree with logic in the text, I just think the exhibits don't acturately demonstrate the text.
I think of it when the engine is off - atmospheric pressure at the entrance to the airbox and at the throttle body.
When the engine is on - atmospheric pressure at the airbox entrance and less than atmospheric pressure at the throttle body for 2 reasons. static pressure energy is converted to kinetic energy and energy losses in the air box system. the 2 causes for the losses are friction beween the air and the pipe walls and losses caused be changes in flow direction and changes in flow area. By modifing the airbox you eliminate a portion of both of these energy losses. therefore less static energy is used and the pressure is higher at the throttle body. there is more available pressure to push more air into the cylinder.
The pressure in "a" certainly is higher than the pressure in "b."
From the ideal gas law we also know that density=pressure/(specific gas constant x absolute temperature). If density a = density b and pressure a >pressure b, then temperature a > temperature b.
So I must be missing something, because to me, "a" is just hotter than "b."
Don't get me wrong I generally agree with logic in the text, I just think the exhibits don't acturately demonstrate the text.
I think of it when the engine is off - atmospheric pressure at the entrance to the airbox and at the throttle body.
When the engine is on - atmospheric pressure at the airbox entrance and less than atmospheric pressure at the throttle body for 2 reasons. static pressure energy is converted to kinetic energy and energy losses in the air box system. the 2 causes for the losses are friction beween the air and the pipe walls and losses caused be changes in flow direction and changes in flow area. By modifing the airbox you eliminate a portion of both of these energy losses. therefore less static energy is used and the pressure is higher at the throttle body. there is more available pressure to push more air into the cylinder.


