noobish Question(high end power)
#1
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My 92' Miata 1.6: Greddy 15g-td40h, 8 psi, no brain tune/just FMU 12:1 disc, no IC, 8 degrees from base timing, aluminum 8lbs. Flywheel, A/C removed
has decent low-end and good midrange power. But top end, it's laggy in my opinion and is revving high around 4000 rpm at 60mph. It's not been properly tuned either. Is it normal for miata's to be revving that high? I never had/drove a stock miata so it seems so.
Where do I start? I can't seem to find anything helpful. What's everyone's take on this. I am retarded I know.
has decent low-end and good midrange power. But top end, it's laggy in my opinion and is revving high around 4000 rpm at 60mph. It's not been properly tuned either. Is it normal for miata's to be revving that high? I never had/drove a stock miata so it seems so.
Where do I start? I can't seem to find anything helpful. What's everyone's take on this. I am retarded I know.
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#5
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No thats not how gears work.
If you engine is spinning at 4k (assuming no clutch slippage) there is only one speed the rear wheels can rotate at. The ratio between the engine and rear wheels is fixed (in any one gear) and doesn't change.
If you have a stock clutch its very possible its slipping which would cause you to be at a higher rpm than you should be at a given speed. This should only be an issue under hard acceleration.
As I stated previously, get a MS. Then you can know what your engine is doing and change it as needed.
If you engine is spinning at 4k (assuming no clutch slippage) there is only one speed the rear wheels can rotate at. The ratio between the engine and rear wheels is fixed (in any one gear) and doesn't change.
If you have a stock clutch its very possible its slipping which would cause you to be at a higher rpm than you should be at a given speed. This should only be an issue under hard acceleration.
As I stated previously, get a MS. Then you can know what your engine is doing and change it as needed.
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If I remember right, at around 65-70 I'm around 3200 rpm in my 91.
When my stock clutch was slipping, it was WAY more likely to slip in 4th and 5th than lower gears. Simply trying to accelerate while in 5th would cause the clutch to slip if I wasn't very gingerly.
RPM aside, it makes sense because the clutch would "see" more torque in a higher gear than a lower one...same reason it is easier to start a car rolling in first than in third.
When my stock clutch was slipping, it was WAY more likely to slip in 4th and 5th than lower gears. Simply trying to accelerate while in 5th would cause the clutch to slip if I wasn't very gingerly.
RPM aside, it makes sense because the clutch would "see" more torque in a higher gear than a lower one...same reason it is easier to start a car rolling in first than in third.
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This same issue has an effect in transmissions for DC electric motors, which have nearly flat torque curves (actually somewhat backwards from ICEs).
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thanx for all the feedback.
I have a 6 puck Spec Stage 3 carbon/metallic clutch. It's a good clutch, and not used that much 5k miles maybe? But It may be that my flywheel is too light(8lbs.), plus I got all aluminum wheels that weigh just 10lbs each.
I have a 6 puck Spec Stage 3 carbon/metallic clutch. It's a good clutch, and not used that much 5k miles maybe? But It may be that my flywheel is too light(8lbs.), plus I got all aluminum wheels that weigh just 10lbs each.
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There are 360 degrees in one rotation of the crankshaft. When you change the timing from 10 degrees BTDC to 14 degrees BTDC you actually move the point where the spark is fired from 350 degrees of rotation to 346 degrees of rotation of the crank. Imagine the end of the crank being a clock dial with 12 o'clock being 0 degrees. At 11.58 and 20 seconds the ignition process starts at 10 degrees BTDC. Change the timing to 14 degrees BTDC and the ignition process starts at 11.57 and 20 seconds.
When the crank reaches the timing point an electric current is fired off to the spark plug. The spark ignites the air and fuel mixture. This ignition starts at the spark plug and flame fronts travel up to the top of the chamber, out to the sides of the chamber and down to the top of the piston. When the flame front reaches the top of the piston it pushes it down, the crank rotates and there is movement in the drive train.
Whereas the engine revs can vary between 900 and 7,000 rpm; there are a constants for the speed at which the current passes to the spark plug, the ignition process and the burn rate of the fuel.
There is a point in the piston's downward movement where the flame front impacts on piston. For this example we assume that this point is when the crank has turned to be 15 degrees after TDC. On a 1.6 litre engine the location of the piston is now 1.865mm below its TDC position on its downward stroke. To check this use the formula {HT = (r + c) - (r cos (a)) - SQRT(c^2 - (r sin (a))^2)} where HT = position location ATDC, r = stroke/2, c = con rod length, a = radians of crank angle. For a 1.6 litre the stroke is 83.6mm and the con rod is 132.9 (+/-0.05) mm
At 900 rpm the crank rotates one degree in 0.18519 milliseconds.
The crank turns 360 degrees in one rpm. Therefore 360 degrees X 900 rpm = 324,000 degrees per minute = 5,400 degrees per second = 1/5400 of a second per degree = 0.00018519 seconds or 0.18519 milliseconds per degree.
By advancing the timing by 4 degrees you start the ignition process 0.741 (0.18519 X 4) milliseconds sooner at 900-rpm (0.111 milliseconds at 6,000 rpm).
At 900 rpm it takes 4.629 milliseconds for the crank to travel the 25 degrees from 10 degrees before TDC to 15 degrees after TDC. At 6,000 rpm this movement takes just 0.694 milliseconds. Remembering that the flame front has a constant burn rate then to have the flame front and piston converge when the piston is just after TDC requires the combustion process to start earlier in the cycle at higher rpm. Otherwise the piston would be lower down in its location before the flame front reached it.
Therefore as the rpm increases the ECU changes the timing so that, in a stock 1.6 litre, the advance increases through the rev range to a maximum of 36 BTDC at 5,500.
If you advance the timing at idle to 14 degrees BTDC then you increase the timing by 4 degrees across the rev range.
In our stock model we had the flame front meeting the piston when the crank is at 15 degrees ATDC (when the piston is 1.865mm on its downward stroke). Therefore by advancing the ignition process by 4 degrees the piston receives the flame front 4 degrees sooner. Ie at 11 degrees ATDC. The piston is located 1.00753 mm from TDC at 11 degrees ATDC.
When the combustion commences there is an expansion of the volume (remember the formula for volume of gasses at various temperatures from our first year physics classes). The rate of expansion is determined by the burn rate of the fuel. In our model this is constant.
Combustion actually commences while the piston is on its upward journey. The time it takes for the flame kernel at spark plug to expand to the top and sides of the chamber permits the piston to pass top dead centre before it receives the flame front. The expansion of the gasses during the period from ignition point (BTDC) to flame front reception (ATDC) increases the volume in the chamber and effectively creates higher compression.
Now we can see why it is that when the timing is advanced the higher position of the piston at 11 degrees ATDC (compared to 15 degrees ATDC) increases the effective compression and gives more power on the downward stroke. That equals more torque.
#18
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Lol, I was TOTALLY ******* around with my responses. Good explanation though ![wink](https://www.miataturbo.net/images/smilies/wink.gif)
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There are 360 degrees in one rotation of the crankshaft. When you change the timing from 10 degrees BTDC to 14 degrees BTDC you actually move the point where the spark is fired from 350 degrees of rotation to 346 degrees of rotation of the crank. Imagine the end of the crank being a clock dial with 12 o'clock being 0 degrees. At 11.58 and 20 seconds the ignition process starts at 10 degrees BTDC. Change the timing to 14 degrees BTDC and the ignition process starts at 11.57 and 20 seconds.
When the crank reaches the timing point an electric current is fired off to the spark plug. The spark ignites the air and fuel mixture. This ignition starts at the spark plug and flame fronts travel up to the top of the chamber, out to the sides of the chamber and down to the top of the piston. When the flame front reaches the top of the piston it pushes it down, the crank rotates and there is movement in the drive train.
Whereas the engine revs can vary between 900 and 7,000 rpm; there are a constants for the speed at which the current passes to the spark plug, the ignition process and the burn rate of the fuel.
There is a point in the piston's downward movement where the flame front impacts on piston. For this example we assume that this point is when the crank has turned to be 15 degrees after TDC. On a 1.6 litre engine the location of the piston is now 1.865mm below its TDC position on its downward stroke. To check this use the formula {HT = (r + c) - (r cos (a)) - SQRT(c^2 - (r sin (a))^2)} where HT = position location ATDC, r = stroke/2, c = con rod length, a = radians of crank angle. For a 1.6 litre the stroke is 83.6mm and the con rod is 132.9 (+/-0.05) mm
At 900 rpm the crank rotates one degree in 0.18519 milliseconds.
The crank turns 360 degrees in one rpm. Therefore 360 degrees X 900 rpm = 324,000 degrees per minute = 5,400 degrees per second = 1/5400 of a second per degree = 0.00018519 seconds or 0.18519 milliseconds per degree.
By advancing the timing by 4 degrees you start the ignition process 0.741 (0.18519 X 4) milliseconds sooner at 900-rpm (0.111 milliseconds at 6,000 rpm).
At 900 rpm it takes 4.629 milliseconds for the crank to travel the 25 degrees from 10 degrees before TDC to 15 degrees after TDC. At 6,000 rpm this movement takes just 0.694 milliseconds. Remembering that the flame front has a constant burn rate then to have the flame front and piston converge when the piston is just after TDC requires the combustion process to start earlier in the cycle at higher rpm. Otherwise the piston would be lower down in its location before the flame front reached it.
Therefore as the rpm increases the ECU changes the timing so that, in a stock 1.6 litre, the advance increases through the rev range to a maximum of 36 BTDC at 5,500.
If you advance the timing at idle to 14 degrees BTDC then you increase the timing by 4 degrees across the rev range.
In our stock model we had the flame front meeting the piston when the crank is at 15 degrees ATDC (when the piston is 1.865mm on its downward stroke). Therefore by advancing the ignition process by 4 degrees the piston receives the flame front 4 degrees sooner. Ie at 11 degrees ATDC. The piston is located 1.00753 mm from TDC at 11 degrees ATDC.
When the combustion commences there is an expansion of the volume (remember the formula for volume of gasses at various temperatures from our first year physics classes). The rate of expansion is determined by the burn rate of the fuel. In our model this is constant.
Combustion actually commences while the piston is on its upward journey. The time it takes for the flame kernel at spark plug to expand to the top and sides of the chamber permits the piston to pass top dead centre before it receives the flame front. The expansion of the gasses during the period from ignition point (BTDC) to flame front reception (ATDC) increases the volume in the chamber and effectively creates higher compression.
Now we can see why it is that when the timing is advanced the higher position of the piston at 11 degrees ATDC (compared to 15 degrees ATDC) increases the effective compression and gives more power on the downward stroke. That equals more torque.
When the crank reaches the timing point an electric current is fired off to the spark plug. The spark ignites the air and fuel mixture. This ignition starts at the spark plug and flame fronts travel up to the top of the chamber, out to the sides of the chamber and down to the top of the piston. When the flame front reaches the top of the piston it pushes it down, the crank rotates and there is movement in the drive train.
Whereas the engine revs can vary between 900 and 7,000 rpm; there are a constants for the speed at which the current passes to the spark plug, the ignition process and the burn rate of the fuel.
There is a point in the piston's downward movement where the flame front impacts on piston. For this example we assume that this point is when the crank has turned to be 15 degrees after TDC. On a 1.6 litre engine the location of the piston is now 1.865mm below its TDC position on its downward stroke. To check this use the formula {HT = (r + c) - (r cos (a)) - SQRT(c^2 - (r sin (a))^2)} where HT = position location ATDC, r = stroke/2, c = con rod length, a = radians of crank angle. For a 1.6 litre the stroke is 83.6mm and the con rod is 132.9 (+/-0.05) mm
At 900 rpm the crank rotates one degree in 0.18519 milliseconds.
The crank turns 360 degrees in one rpm. Therefore 360 degrees X 900 rpm = 324,000 degrees per minute = 5,400 degrees per second = 1/5400 of a second per degree = 0.00018519 seconds or 0.18519 milliseconds per degree.
By advancing the timing by 4 degrees you start the ignition process 0.741 (0.18519 X 4) milliseconds sooner at 900-rpm (0.111 milliseconds at 6,000 rpm).
At 900 rpm it takes 4.629 milliseconds for the crank to travel the 25 degrees from 10 degrees before TDC to 15 degrees after TDC. At 6,000 rpm this movement takes just 0.694 milliseconds. Remembering that the flame front has a constant burn rate then to have the flame front and piston converge when the piston is just after TDC requires the combustion process to start earlier in the cycle at higher rpm. Otherwise the piston would be lower down in its location before the flame front reached it.
Therefore as the rpm increases the ECU changes the timing so that, in a stock 1.6 litre, the advance increases through the rev range to a maximum of 36 BTDC at 5,500.
If you advance the timing at idle to 14 degrees BTDC then you increase the timing by 4 degrees across the rev range.
In our stock model we had the flame front meeting the piston when the crank is at 15 degrees ATDC (when the piston is 1.865mm on its downward stroke). Therefore by advancing the ignition process by 4 degrees the piston receives the flame front 4 degrees sooner. Ie at 11 degrees ATDC. The piston is located 1.00753 mm from TDC at 11 degrees ATDC.
When the combustion commences there is an expansion of the volume (remember the formula for volume of gasses at various temperatures from our first year physics classes). The rate of expansion is determined by the burn rate of the fuel. In our model this is constant.
Combustion actually commences while the piston is on its upward journey. The time it takes for the flame kernel at spark plug to expand to the top and sides of the chamber permits the piston to pass top dead centre before it receives the flame front. The expansion of the gasses during the period from ignition point (BTDC) to flame front reception (ATDC) increases the volume in the chamber and effectively creates higher compression.
Now we can see why it is that when the timing is advanced the higher position of the piston at 11 degrees ATDC (compared to 15 degrees ATDC) increases the effective compression and gives more power on the downward stroke. That equals more torque.
#19
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Now that's what I call help. It makes sense. I am not btdc. I actually moved a couple degrees too far. Thanks for the 'splanation, now to open the covers again and doing it right this time. Thank you all!
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#20
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It's just like the clutch experiences no torque (except for moving the internals of the transmission) when the transmission is out of gear, even though the clutch is spinning at the same rate as the engine, but it does experience differing amounts of torque depending on what gear the transmission is in accelerate or decelerate the car.