Torque distribution to thrust?

In summary: I'm trying to figure out how it functioned in it's designed life as a handicapped scooter motor. I am thinking the 0.85Nm on the label is an average/standard value, not a stall torque? Because I don't see how (per that calculation) it could have moved an 82Kg/180lb person generating only 62 Newtons of thrust from a dead stop.In its designed life, the gearing on this motor would be much higher. In your first description, you reckoned 6f/s, or 7km/h. That's rather fast for a handicapped scooter. Probably would be half that, and limited to shallow inclines and decent surfaces.
  • #1
magnethead494
28
0
I'm working with a 3000 RPM @ 0.85 Nm motor in the transaxle from a powered scooter (like for disabled/elderly people). The differential has a 67:4 (16.75) reduction, which puts the output shafts around 179 RPM @ 14.23 Nm.

I'm passing this to a 25:9 chain drive, which makes the final output 64.4 RPM @ 39.5 Nm, or 29.13 pound-force-feet.

Each tire has an 11 inch radius, for a top speed of 6 feet per second, and a max thrust of 31.77 pound-force.

My question is, is the thrust at this point distributed evenly among 6 tires, or is it additive per tire? If I hooked a load to this this robot/ATV I'm building, would it stall at a 31 pound load with each tire providing 5.3 pound-force, or a (6*31.77 = ) 190 pound load with each tire providing 31 pound-force?

Thanks.

This is the axle carriage as I have it right now in my CAD program. Slowly getting more drawn.

https://fbcdn-sphotos-a.akamaihd.net/hphotos-ak-ash4/461089_10150962129059606_771454605_12935442_879036768_o.jpg
 
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  • #2
It's shared by the six tires. Power = force x speed. You have the same power and the same speed whether it's across six tires or one, so the total force must be the same.
 
  • #3
haruspex said:
It's shared by the six tires. Power = force x speed. You have the same power and the same speed whether it's across six tires or one, so the total force must be the same.

Thanks. At this I hypothesize: in "stock" form, with 9 inch wheels,

3000 @ 0.85nM -> 16.75:1 -> 179 @ 14.23 Nm = 179 RPM @ 10.5 pound force feet, 9" tire, equals 7 feet per second at 14 pound-force-feet of thrust. How would this be able to move, say, a 180 pound rider, and not stall?
 
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  • #4
I guess you mean 14 pound-force of thrust.
That's ok, ignoring rolling resistance, as long as the upward incline is not too steep, i.e. less than 1 in 13 (sin(slope angle) = 14/180). A bit limiting by the sound of it.
Might need smaller wheels or a bigger gear ratio.
 
  • #5
haruspex said:
I guess you mean 14 pound-force of thrust.
That's ok, ignoring rolling resistance, as long as the upward incline is not too steep, i.e. less than 1 in 13 (sin(slope angle) = 14/180). A bit limiting by the sound of it.
Might need smaller wheels or a bigger gear ratio.
If my approximations are correct, 82kG person * g = 804.42 Newtons, with an approx mu/rolling resistance of 0.30, yields 241 Newtons. To do this on a 9 inch tire, would take 55.5 Newton-meters of torque, or 3.3 Newtons from the electric motor.

Is that right?

or working mu off the .85Nm rating on the sticker,

14.23 Nm / .23m = 61.87 Newtons of thrust, against a load of 804.42 Newtons, would require a mu of 0.077-------

The motor is made by Electro-Craft, a division of Reliance Electric.
Model number E675
Serial number G006497
Date code week 20 of 1997
Part number E675-07-042

3.375" or so diameter casing with a 1/2" diameter shaft

E_675_Pride_800_344.jpg
 
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  • #6
So.. you're never going uphill, so you only care about rolling resistance?
In your last calculation you seem to have left out the chain drive.
 
  • #7
haruspex said:
So.. you're never going uphill, so you only care about rolling resistance?
In your last calculation you seem to have left out the chain drive.

I'm trying to figure out how it functioned in it's designed life as a handicapped scooter motor. I am thinking the 0.85Nm on the label is an average/standard value, not a stall torque? Because I don't see how (per that calculation) it could have moved an 82Kg/180lb person generating only 62 Newtons of thrust from a dead stop. I could understand it during constant motion, but not under acceleration.

The robot I will be putting it in will only weigh 150 pounds max, but will be traversing property which is not safe to walk through due to snakes and other critters (A wetlands area) where the grass/weeds/vegetation is as high as 4 feet, as part of a research project. It will be running on 2 car batteries in series in a watertight aluminum hull with 24V/50A speed controller, controlled over R/C with remote camera broadcasting. Extreme case design is for moderate surface speed with significant amount of torque for pulling itself through the vegetation. The tires are 22"H x 11"W ATV tires. The 6 tires alone could support a { [[V(22,11)-V(8,8)]/1728]*7.48*8.34 }*6 = [[4181-402]/1728] = 2.18 CF * 7.48 gal/CF * 8.34 lb/gal * 6 = 818 pound vehicle if fully submerged. And make for good surface flotation over thick/muddy/cakey water.
 
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  • #8
As I read it, you are supplying the drive chain. Maybe in its designed role the gearing was much higher. In your first description, you reckoned 6f/s, or 7km/h. That's rather fast for a handicapped scooter. Probably would be half that, and limited to shallow inclines and decent surfaces.

To go through vegetation you're going to need a lot more thrust. I'd be surprised if you could get 3km/h with 150 pound load (including the vehicle?).
 
  • #9
Found some new data. The batteries are 22V/55A or 24V/70A depending on options, and the chairs were rated for a 20-25 mile range per charge at up to 4.5 miles per hour.

55A/20Mi = 2.75A/Mi * 4.5Mi/Hr = 12.375 A/Hr @ 22V = 272.25W
55A/25Mi = 2.20A/Mi * 4.5Mi/Hr = 09.900 A/Hr @ 22V = 217.80W
70A/20Mi = 3.50A/Mi * 4.5Mi/Hr = 15.750 A/Hr @ 24V = 378.00W
70A/25Mi = 2.80A/Mi * 4.5Mi/Hr = 12.600 A/Hr @ 24V = 302.40W

= Tao * Radians/sec * efficiency (arbitrary 0.8 sound good?)

3000 RPM = 314 rad/sec

0.8 * 314 = 251.33

272.25 = 251.33 * tao = 1.083 Nm
217.80 = 251.33 * tao = 0.866 Nm
378.00 = 251.33 * tao = 1.504 Nm
302.40 = 251.33 * tao = 1.203 Nm

Of which the second value matches the 0.85 on the motor, for all effective reasons.
 
  • #10
haruspex said:
As I read it, you are supplying the drive chain. Maybe in its designed role the gearing was much higher. In your first description, you reckoned 6f/s, or 7km/h. That's rather fast for a handicapped scooter. Probably would be half that, and limited to shallow inclines and decent surfaces.

To go through vegetation you're going to need a lot more thrust. I'd be surprised if you could get 3km/h with 150 pound load (including the vehicle?).

Original design is 4/67 differential gearing and 9" tires. That's it. I posted a picture of the entire motor assy a couple posts up.

I'm taking that assy, removing the wheels, and putting 9 tooth sprockets there instead. These then go to 25 tooth sprockets on the center axle. 12 tooth sprockets distribute to the outboard axles (1:1 of course).

The scooter weighed 200 pounds on it's own, with spec for a max 250 pound rider. My entire robot will be under 150 pounds when done (80 of that will be the car batteries).

stock config said:
3000 @ 0.85nM -> 16.75:1

179 @ 14.23 Nm = 179 RPM @ 10.5 pound force feet

9" tire, equals 7 feet per second [rated for 4.5mph by mfgr] at 14 pound-force of thrust.

robot config said:
3000 @ 0.85nM -> 16.75:1 ->

179 @ 14.23 Nm -> 2.77:1 ->

64.62 @ 39.42 Nm = 64.62 RPM @ 29 pound force feet

22" tire, equals 6.2 feet per second at 31.63 pound-force of thrust
 
  • #11
haruspex said:
As I read it, you are supplying the drive chain. Maybe in its designed role the gearing was much higher. In your first description, you reckoned 6f/s, or 7km/h. That's rather fast for a handicapped scooter. Probably would be half that, and limited to shallow inclines and decent surfaces.

To go through vegetation you're going to need a lot more thrust. I'd be surprised if you could get 3km/h with 150 pound load (including the vehicle?).

Just to be on the safe side, I'll change the 9:25 chain to a 9:32. "Only" a 9 pound-force difference in thrust for a 1.4 foot per second decrease. But as you said, Torque is what I'll need given the conditions.

40.64 pounds of thrust / 6 tires = 6.77 pounds of thrust per tire.

robot config said:
3000 @ 0.85nM -> 16.75:1 ->

179 @ 14.23 Nm -> 3.55:1 ->

50.42 @ 50.52 Nm = 50.52 RPM @ 37.26 pound force feet

22" tire, equals 4.84 feet per second at 40.64 pound-force of thrust
 
  • #12
Sorry if I write something redundant here, I'm in a small hurry.

Rolling friction is not the same as sliding friction. You need a horizontal force of about F = k·mg where k ≈ 0.01 for car tires on asphalt, give or take ±0.005 or so.

So a 100 kg vehicle needs about 10 N to move. Multiply with velocity (in m/s) to get the required motor power output (in watts).
 
  • #13
Microcephalus said:
Sorry if I write something redundant here, I'm in a small hurry.

Rolling friction is not the same as sliding friction. You need a horizontal force of about F = k·mg where k ≈ 0.01 for car tires on asphalt, give or take ±0.005 or so.

So a 100 kg vehicle needs about 10 N to move. Multiply with velocity (in m/s) to get the required motor power output (in watts).

Thanks. So that would make the numbers indeed make sense, since I came up with a MuK of about .077
 
  • #14
Two key questions:
1. what slope the worst terrain you encounter will be equivalent to. You won't want to risk it's getting stuck often. I would guess something like 30 degrees.
2. How the motor responds to increased load. There'll be a stall torque, but even before that there may be a falling off of power? If that's unknown, just take the stall torque.

With the above assumptions, the fundamental need is to ensure you can get up a 30 degree slope, however slowly, at stall torque. What speed you manage on easier terrain is somewhat secondary.
 
  • #15
For safety/overhead tolerances, I say 45 degrees is a good design margin, especially for the size of tire.

For MuK of 0.03 (arbitrary for knobby tire on dirt), on flat ground,

0.03 * 9.8 m/s^2 * 68kg = 19.992 kilogram-meter per second squared = 19.992 Newtons of thrust.

friction force going down = Mu * cos(theta) * m * g

thrust going up = friction force + sin(theta) * m * g

For MuK of 0.03 at 45 degree angle,

friction force = 0.03 * 0.707 * 68 * 9.8 = 14.13N

thrust force = 14.13N + (0.707 * 68 * 9.8) = 14.13 + 471.1448 = 485.27 Newtons

For MuK of 0.03 on 20 degree plane:

friction force = 0.03 * 0.93 * 68 * 9.8 = 18.59N

thrust force = 18.59 + (0.34 * 68 * 9.8) = 18.59 + 226.57 = 245.166 Newtons

For MuK of 0.03 on 5 degree plane (handicap ramp is 4.73 degrees or shallower per ADA)

friction force = .03 * 0.996 * 68 * 9.8 = 19.92N

thrust force = 19.92 + (0.087 * 68 * 9.8) = 19.92 + 58.080 = 78.00 Newtons

------------------------------------------

Now that said, I o back to the designed spec for this motor. A 250 pound rider with a 200 pound dry weight is 450 pounds total- 204.5 Kg. I'm assuming they designed a minimum spec of going up a wheelchair ramp, ADA limited to 1 foot fo rise per 12 feet of run, or similar. Round off to 5 degrees.

friction force = 0.013 (arbitrary for smooth tire to concrete) * 0.996 * 204.5 * 9.8 = 25.95N

thrust force = 25.92 + (0.087 * 204.5 * 9.8) = 25.92 + 174.36 = 200.27 Newtons of thrust.

To generate that, 200.27 Newtons * (4.5" radius/39.25" per meter) = 22.96 Newton-meters of torque, through the 16.75 gearing, the electric motor had to generate 1.37 Newton Meters of torque to ascend that handicap ramp.

--------------------

1.37 Nm * 16.75 = 22.96 Newton-meters at the output shaft * (32/9) = 81.635 Newton-meters at the axle shaft. 81.635 Newton-meters / (11" radius/39.25" per meter) = 81.635 / .280255 = 291.289 Newtons of thrust

If that new formula and calculations hold,

friction force going down = Mu * cos(theta) * m * g

thrust going up = friction force + sin(theta) * m * g

thus, thrust force = (Mu * cos(theta) * m * g) + (sin(theta) * m * g)

finding theta for a Mu of 0.03 = (0.03 * 68 * 9.8 * cos(theta)) + (68 * 9.8 * sin(theta)) = 19.992cos(theta) + 666.4 * sin(theta) = 291 Newtons

19.992cos(theta) + 666.4 * sin(theta) = 291 Newtons

plugging that in my calculator, shows a 289.31 N force at 24 degrees and a 299.75 N force at 25 degrees. So a 24 degree slope would be the upper limit.

---------------------

using the 0.85Nm rating on the sticker,

0.85 Nm * 16.75 = 14.24 Newton-meters at the output shaft * (32/9) = 50.622 Newton-meters at the axle shaft. 50.622 Newton-meters / (11" radius/39.25" per meter) = 50.622 / .280255 = 180.63 Newtons of thrust

finding theta for a Mu of 0.03 = (0.03 * 68 * 9.8 * cos(theta)) + (68 * 9.8 * sin(theta)) = 19.992cos(theta) + 666.4 * sin(theta) = 180.63 Newtons

Calculator shows a result of 180.61N at 14 degrees. So with a Mu of 0.03 and a weight of 68Kg/150 pounds, It could climb up to 14 degrees, possibly up to 24.

---------------------

finding theta for a Mu of 0.018 (arbitrary value for knobby tire on concrete) =
(0.018 * 68 * 9.8 * cos(theta)) + (68 * 9.8 * sin(theta)) = 11.995cos(theta) + 666.4 * sin(theta) = 291 Newtons = 24 degrees

finding theta for a Mu of 0.018 =
(0.018 * 68 * 9.8 * cos(theta)) + (68 * 9.8 * sin(theta)) = 11.995cos(theta) + 666.4 * sin(theta) = 180 Newtons = 14 degrees---------------------

finding theta for a Mu of 0.013 (arbitrary value for smooth tire on concrete) =
(0.013 * 68 * 9.8 * cos(theta)) + (68 * 9.8 * sin(theta)) = 8.6632cos(theta) + 666.4 * sin(theta) = 291 Newtons = 25 degrees

finding theta for a Mu of 0.013 =
(0.013 * 68 * 9.8 * cos(theta)) + (68 * 9.8 * sin(theta)) = 8.6632cos(theta) + 666.4 * sin(theta) = 180 Newtons = 15 degrees

-------------------

So the Mu isn't very effective of the total angle- So with this system of equations, 14 and 24 degrees are the lower and upper inclination limits.

180 Newtons = 40.5 pound-force

290 Newtons = 65.2 pound-force

------------------

The batteries of choice would be Group 26 size for a 2000-2001 dodge neon. Each battery is 28 pounds, 675CA, 530CCA. Based on an 18AH load, would be about 30-37 hours of runtime between charges.
 
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1. What is torque distribution to thrust?

Torque distribution to thrust is the process of converting rotational force, or torque, into linear force, or thrust, in a system or machine. This is commonly used in engines and motors to generate movement and power.

2. How is torque distribution to thrust achieved?

Torque distribution to thrust is achieved through the use of gears, pulleys, or other mechanical components that transfer the rotational force from the source to the output, resulting in linear force or thrust.

3. Why is torque distribution to thrust important?

Torque distribution to thrust is important because it allows for efficient and precise control of movement and power in machines and systems. It also enables the conversion of different types of energy, such as electrical or chemical energy, into mechanical energy.

4. What factors affect torque distribution to thrust?

The factors that affect torque distribution to thrust include the amount of torque applied, the gear ratio, the efficiency of the mechanical components, and external factors such as friction and load.

5. How can torque distribution to thrust be optimized?

To optimize torque distribution to thrust, it is important to have well-designed and properly maintained mechanical components, as well as an understanding of the principles of torque and thrust. Additionally, adjusting the gear ratio and minimizing friction can also help improve overall efficiency.

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