Tie rack calculations
From DDL Wiki
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- | + | substitute ω10 = ω6 into (7) | |
- | ω10 = | + | ω10 = [r5 r4 r3 r1 / r9 r8 r7 r2] ω1 (8) |
- | + | ω10/ ω1 = [r5 r4 r3 r1 / r9 r8 r7 r2] (9) | |
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- | + | ω1/ ω10 = [r9 r8 r7 r2 / r5 r4 r3 r1] (10) | |
- | + | ||
- | + | ||
- | + | ||
- | ω1/ ω10 = [r9 r8 r7 r2 / r5 r4 r3 r1] ( | + | |
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''τs = 0.0142 Nm = 14.24 mN-m'' | ''τs = 0.0142 Nm = 14.24 mN-m'' | ||
+ | |||
+ | |||
+ | '''Engine Torque''' | ||
+ | |||
+ | A relationship between torque and speed can provide an equation to calculate the torque output from the motor when it runs in the device. Assuming ideal motor function, thus a linear distribution: | ||
+ | |||
+ | τ = α ω + τs | ||
+ | |||
+ | α = τs / speed = 0.0142 mN-m / 51314.84 RPM = 2.77 x 10-7 | ||
+ | |||
+ | τ1 = α ω1 + τs = (2.77 x 10-7) (51314.84 RPM) + 0.0142 N-m | ||
+ | |||
+ | ''τ1 = 0.0284 N-m = motor torque while running'' |
Revision as of 15:44, 5 March 2007
Gear Train
Speed of Output
The gear train creates a decrease of speed and increase of torque from the actual motor output. The final speed is slow enough to measure with a stopwatch. This was done by marking a point on the rotating belt, and measuring the time that it took for one rotation (the point returns to where it started).
Setup:
Time for one rotation of belt gear = 5s : 38ms Circumference of belt gear = 0.126 m
Speed = length/time (m/s)
Angular speed = ω = 2π/T (radians/s)
ω10 = length / [r10 * time] = (0.126 m) / [(0.02m)(5.38 s)] = 1.17 rotations/sec
ω10 = 70.26 RPM
Gear Ratios/Calculations (Relating input to output)
ω1 r1 = ω2 r2 and ω2 = ω3
ω2 = ω4 = [r1 / r2] ω1 (1)
ω3 r3 = ω7 r7 and ω7 = ω4
ω7 = ω3 = [r3 / r7] ω3 (2)
substitute (1) into (2)
ω7 = ω4 = [r3 r1 / r7 r2] ω1 (3)
ω4 r4 = ω8 r8 and ω8 = ω5
ω8 = ω5 = [r4 / r8] ω34 (4)
substitute (3) into (4)
ω3 = ω5 = [r4 r3 r1 / r8 r7 r2] ω1 (5)
ω5 r5 = ω9 r9 and ω9 = ω6
ω9 = ω6 = [r5 / r9] ω5 (6)
substitute (5) into (6)
ω9 = ω6 = [r5 r4 r3 r1 / r9 r8 r7 r2] ω1 (7)
substitute ω10 = ω6 into (7)
ω10 = [r5 r4 r3 r1 / r9 r8 r7 r2] ω1 (8)
ω10/ ω1 = [r5 r4 r3 r1 / r9 r8 r7 r2] (9)
ω1/ ω10 = [r9 r8 r7 r2 / r5 r4 r3 r1] (10)
ω1 = [(0.019m)( 0.019m)(0.019m)(0.0115m) / (0.003m)(0.003m)
(0.003m)(0.004m)] * 70.26 RPM
ω1 = 51314.84 RPM = motor speed
Stall Torque
The stall torque of the motor was calculated by finding an equilibrium point between an opposing torque and motor output torque. This was done by turning the motor sideways, powering it, and hanging weights on the pulley attached to the motor shaft until weight suspension was reached (τ1 = τ2). The string is of negligible mass and was tightly affixed to the pulley to prevent slipping by both knotting it with a rubber band.
Setup:
Result:
Motor stalled when 0.8 lb weight was creating a torque. Thus:
0.8 lbs = 0.363 kg
Radius of motor pulley = 0.004 m
τs = Fr = (0.363 kg) (9.81 m/s2) (0.004 m)
τs = 0.0142 Nm = 14.24 mN-m
Engine Torque
A relationship between torque and speed can provide an equation to calculate the torque output from the motor when it runs in the device. Assuming ideal motor function, thus a linear distribution:
τ = α ω + τs
α = τs / speed = 0.0142 mN-m / 51314.84 RPM = 2.77 x 10-7
τ1 = α ω1 + τs = (2.77 x 10-7) (51314.84 RPM) + 0.0142 N-m
τ1 = 0.0284 N-m = motor torque while running