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#71 | |
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This is right!! In machine design one often needs to incorporate a Power Transmission between an energy source and the desired output motion. Examples include elements include: gears, friction drives, timing belts, flat belts, levers, and screw drives. ![]() Mechanical Advantage refers to an increase in torque or force that a mechanism achieves through a power transmission element. For rotary devices the term Gear Ratio is used to define the Mechanical Advantage. The term Mechanical Advantage is used to describe components that include translation. The analysis below shows how one calculates the Gear Ratio and Mechanical Advantage of a Power Transmission component. The law of energy conservation dictates that one can never get more energy in the output motion than provided by the energy source. Indeed, one always has some energy loss in a Power Transmission. Energy loss rates can vary from 5% for a flat belt drive to up to 80% for a multi-stage gear transmission (higher and lower rates can occur too). Before the analysis we first define some notation: P => Power E => Energy W => Work f => Force t => torque d => distance of translational motion q => angle of rotational motion (in radians) v => velocity of translational motion w => angular speed (in radians per second) d => change Pd => Pitch diameter n => number of teeth on a gear nrev => number of revolutions For basic analysis of Gear Ratios we initially neglect frictional losses, and then incorporate their effect separately. With this assumption we can set the power in to equal to the power out. Pin = Pout Power is defined as the change in energy divided by the change in time. P = dE/dt In a mechanism energy is transferred by mechanical work. For translational motion work is given by: Work = Force X Motion (where the force and motion are parallel to each other) W = f dd The corresponding definition of work for rotational motion is given by: Work = Torque X Rotary Motion W = t dq In a Power Transmission the Work is the source of the change in energy, and thus: P = dE/dt = W/dt Substituting the rotary definition of work into the above equation, and noting that rotation velocity is given by w=dq/dt, the power transfer in a rotary device is given by: P = W/dt = t dq/dt P = t w In a similar fashion, for translational motion the power transfer is given by: P = W/dt = f dd/dt A gear train is shown below with an input gear on the left and an output gear on the right. For the purposes of this analysis we assume the input gear may is attached to a motor, and the output gear is attached to a shaft on a machine that performs a desired function. ![]() As shown the input gear is rotating counterclockwise with an angular velocity of win and the output gear is rotating clockwise with an angular velocity of wout. An input torque, tin, is applied by the motor onto the input gear, and an opposing output torque, tout, is applied by the machine onto the output gear. The radius of the gears is shown at the Pitch Circle of the gear, which is between the top and bottom of the gear tooth, and represents the radius at which contact occurs between the two gears. The development of gear shapes has been optimized significantly to reduce frictional losses, provide smooth power transfer, and reduce noise. The shape of the gear teeth are the some on both the input and output gears, and thus the larger gear has more teeth on it. The Pitch distance, Pd, is the distance between gears. Thus the number of teeth on the gear, n, times the Pitch is equal to the circumference of the gear. Accordingly, Pd nin = 2 p rin Pd nout = 2 p rout nin/ nout = rin/ rout The gear pair is analyzed with the following assumptions:
Since there are no frictional losses, the input and output power can be set equal to each other as: Pin = tin win Pout = tout wout tin win = tout wout We now need to consider the relative velocity of the two gears, which is determined by the meshing of the teeth. Since the teeth mesh, we know that the same number of teeth must mesh from both gears. For each revolution of the input gear the following number of teeth pass through the mesh area, where nrevin is the number of revolutions of the input gear: number of teeth that mesh = nrevin 2 p rin / Pd Applying the same equation to the output gear, and setting the number of meshed teeth equal to each other provides: nrevout 2 p rout / Pd = nrevin 2 p rin / Pd The above equation simplifies to: nrevout / nrevin = rin / rout If we multiple the number of revolutions by 2p, we get the angle of rotation of both gears in radians, which gives: rin dqin = rout dqout If we divide the angle of rotation by time, dt, then we get the ratios of angular velocities in radians per second wout/ win = rin / rout An alternative interpretation is that the angular velocity at the mesh point is the same for both gears. Since velocity of a point on a rotating object is given by rw. The velocity equality at the mesh point is given by: rin win = rout wout And we see that the two previous equations are identical. Since the radius of a gear is proportional to the number of teeth, the velocity relationship can be given in terms on numbers of teeth on the input and output gears. Simply substitute into the above equation that nPd=2pr for both gears, to give: wout/ win = nin / nout We can now combine the power equation with the velocity equation to get the ratio of input and output torques: tin win = tout wout (power equation) tout / tin = win / wout tout / tin = rout / rin (substituting in velocity relationship) Thus when the input gear is smaller than the output gear:
The fundamental equations for a gear pair are: tin win = tout wout (power equality) wout/ win = rin / rout (velocity relationship in terms of radiuses) wout/ win = nin / nout (velocity relationship in terms of number of teeth) tout / tin = rout / rin (torque relationship in terms of radiuses) tout / tin = nout / nin (torque relationship in terms of number of teeth) The Gear Ratio is defined as the input speed relative to the output speed. It is typically written as: Gear Ratio = win : wout
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Racecar spelled backwards is Racecar, because Racecar.
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#72 |
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This kind of reminds me of the time that CJ guy started talking to himself.
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#73 | |
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not playing cards
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#74 |
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not playing cards
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Everybody wants to race me.
Everybody fucks with my car even when I'm parked out in the back 40. <other model car> owners are all dooshbags.
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#75 |
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Good ones!!!!!!
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Racecar spelled backwards is Racecar, because Racecar.
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#76 |
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Banned
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#77 |
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All you have to do is mention how AWD has great traction from a dig, he'll come.
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#78 |
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Banned
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#79 | |
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Racecar spelled backwards is Racecar, because Racecar.
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#80 |
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I was thinking more the Ubersuber, Stonenewt, Wparsons (or Wbradley don't remember which and too lazy to go look so sorry one of you guys) debates really.
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#82 | ||
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not playing cards
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Quote:
Yeah, but that whole ebola catastrophuck...
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#83 | |
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You probably didn't think I'd get that reference, but I did. And a laughed for a solid minute.
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#84 |
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Because race car
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