Continuously Variable Transmission Idea
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Then present a set of simple equations that describes your model.A.T. said:I have the real physical thing, and reality says your analysis is wrong.
There needs to be two components with specified angular velocity to constrain the mechanical system.
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The equations governing this gear set seem pretty simple to me. There are four of them:
The gear ratio of the left gear set (##GR_L##), relating angular velocities (##\omega##) of the input (##i##) and output (##o##) shafts:
$$GR_L = \frac{\omega_{oL}}{\omega_{iL}}$$
The gear ratio of the right gear set (##GR_R##), relating angular velocities of the input (##i##) and output (##o##) shafts:
$$GR_R = \frac{\omega_{oR}}{\omega_{iR}}$$
The relationship between the angular velocities of the input differential:
$$\omega_{in} = \frac{\omega_{iL} + \omega_{iR}}{2}$$
The relationship between the angular velocities of the output differential:
$$\omega_{out} = \frac{\omega_{oL} + \omega_{oR}}{2}$$
Already, we can tell we have a problem because we have 4 equations and 5 unknowns (##\omega_{iL}##, ##\omega_{iR}##, ##\omega_{oL}##, ##\omega_{oR}##, ##\omega_{out}##).
For the overall gear ratio (##GR##), it is defined as:
$$GR = \frac{\omega_{out}}{\omega_{in}} = \frac{\omega_{oL} + \omega_{oR}}{\omega_{iL} + \omega_{iR}}=\frac{\omega_{iL}GR_L + \omega_{iR}GR_R}{\omega_{iL} + \omega_{iR}}$$
From that simple equation, we can already define simple - and very intuitive - solutions:
We can define a new constraint, for example ##\frac{\omega_{iR}}{\omega_{in}}##, and the overall gear ratio becomes:
$$GR = \left(1-\frac{1}{2}\frac{\omega_{iR}}{\omega_{in}}\right)GR_L + \frac{1}{2}\frac{\omega_{iR}}{\omega_{in}}GR_R$$
The previous simple solutions become:
The gear ratio of the left gear set (##GR_L##), relating angular velocities (##\omega##) of the input (##i##) and output (##o##) shafts:
$$GR_L = \frac{\omega_{oL}}{\omega_{iL}}$$
The gear ratio of the right gear set (##GR_R##), relating angular velocities of the input (##i##) and output (##o##) shafts:
$$GR_R = \frac{\omega_{oR}}{\omega_{iR}}$$
The relationship between the angular velocities of the input differential:
$$\omega_{in} = \frac{\omega_{iL} + \omega_{iR}}{2}$$
The relationship between the angular velocities of the output differential:
$$\omega_{out} = \frac{\omega_{oL} + \omega_{oR}}{2}$$
Already, we can tell we have a problem because we have 4 equations and 5 unknowns (##\omega_{iL}##, ##\omega_{iR}##, ##\omega_{oL}##, ##\omega_{oR}##, ##\omega_{out}##).
For the overall gear ratio (##GR##), it is defined as:
$$GR = \frac{\omega_{out}}{\omega_{in}} = \frac{\omega_{oL} + \omega_{oR}}{\omega_{iL} + \omega_{iR}}=\frac{\omega_{iL}GR_L + \omega_{iR}GR_R}{\omega_{iL} + \omega_{iR}}$$
From that simple equation, we can already define simple - and very intuitive - solutions:
- if ##\omega_{iR} = 0##, then ##GR = GR_L##;
- if ##\omega_{iL} = \omega_{iR}##, then ##GR = \frac{GR_L + GR_R}{2}##
- if ##\omega_{iL} = 0##, then ##GR = GR_R##;
We can define a new constraint, for example ##\frac{\omega_{iR}}{\omega_{in}}##, and the overall gear ratio becomes:
$$GR = \left(1-\frac{1}{2}\frac{\omega_{iR}}{\omega_{in}}\right)GR_L + \frac{1}{2}\frac{\omega_{iR}}{\omega_{in}}GR_R$$
The previous simple solutions become:
- if ##\frac{\omega_{iR}}{\omega_{in}}= 0##, then ##GR = GR_L##;
- if ##\frac{\omega_{iR}}{\omega_{in}} = 1##, then ##GR = \frac{GR_L + GR_R}{2}##
- if ##\frac{\omega_{iR}}{\omega_{in}} = 2##, then ##GR = GR_R##;
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Seems like I gave up too early. But the insistence of @Baluncore made me more do more careful testing. And it looks like ratios other then 1:1 are indeed possible. Thanks and apologies to @Baluncore.A.T. said:![]()
Disappointingly it was exactly what I initially expected: A boring 1:1 transmission that merely reverses the direction (the yellow crosses rotate opposite to each other).
This part however is correct, and consistent with the formulas posted above by @jack action :
It was referring to this idea:A.T. said:Contrary to some claims in this thread, it is not possible to hold the output static, while turning the input continuously.
As @jack action derived above, one can fix the left or right side gears to switch the total gear ratio between minimum and maximum, given by the opposite side gears respectively. But you cannot hold the output static, while the input rotates, because the the total gear ratio can only be varied within a finite range.Halc said:One can for instance bolt the output to a wall, preventing any rotation. The input can still turn freely.
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Here is a table that gives the speed of the shafts, all referenced to an input of 100. A and B are the input shaft gears, the average of A and B is X, the input. C and D are the output gears, the average of C and D is Y, the output. These definitions are compliant with those of jack action.
Here is the graph that shows gear ratio. The input X remains at 100%, the output is Y, the bright white trace, that can be read off as % gear ratio.
Code:
X A B C D Y
100.000 -50.000 250.000 -25.000 500.000 237.500
100.000 -33.333 233.333 -16.667 466.667 225.000
100.000 -16.667 216.667 -8.333 433.333 212.500
100.000 0.000 200.000 0.000 400.000 200.000
100.000 16.667 183.333 8.333 366.667 187.500
100.000 33.333 166.667 16.667 333.333 175.000
100.000 50.000 150.000 25.000 300.000 162.500
100.000 66.667 133.333 33.333 266.667 150.000
100.000 83.333 116.667 41.667 233.333 137.500
100.000 100.000 100.000 50.000 200.000 125.000
100.000 116.667 83.333 58.333 166.667 112.500
100.000 133.333 66.667 66.667 133.333 100.000
100.000 150.000 50.000 75.000 100.000 87.500
100.000 166.667 33.333 83.333 66.667 75.000
100.000 183.333 16.667 91.667 33.333 62.500
100.000 200.000 0.000 100.000 0.000 50.000
100.000 216.667 -16.667 108.333 -33.333 37.500
100.000 233.333 -33.333 116.667 -66.667 25.000
100.000 250.000 -50.000 125.000 -100.000 12.500
100.000 266.667 -66.667 133.333 -133.333 0.000
100.000 283.333 -83.333 141.667 -166.667 -12.500
100.000 300.000 -100.000 150.000 -200.000 -25.000
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Look at the graph, or the table. The output, Y, crosses zero when;A.T. said:But you cannot hold the output static, while the input rotates, because the the total gear ratio can only be varied within a finite range.
X=100.0; A=266.7; B=-66.667; C=133.3; D=-133.3; Y=0.000
You can do that by clamping the output while turning the input. It is not however possible to brake gears to achieve Y≤0, since the speed of A must be accelerated, while the direction of gear B must be reversed. Reversal is not possible with a brake. Only ratios by a factor of two, between 200% and 50% are possible using brakes.
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Is is possible to achieve Y=0 with a single (non zero) input X (all side axles spin freely) just by changing/reversing the gear ratios (AC and BD)? Or do you have to drive some side axles at a given speed for that?Baluncore said:Look at the graph, or the table. The output, Y, crosses zero when;
X=100.0; A=266.7; B=-66.667; C=133.3; D=-133.3; Y=0.000
You can do that by clamping the output while turning the input. It is not however possible to brake gears to achieve Y≤0, since the speed of A must be accelerated, while the direction of gear B must be reversed. Reversal is not possible with a brake. Only ratios by a factor of two, between 200% and 50% are possible using brakes.
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It is not possible to drive Y to zero, unless you brake Y itself. No matter how I juggle the ratios, one of the input gears must be driven negative to have Y = 0.
However, it can be achieved with a reversal, by inserting an idler gear into one, or the other gear train. It is then possible using a brake to have a bidirectional output that can be zero.
Here is a plot with one negative ratio coefficient.
Notice how A and B are positive, while Y can be negative.
However, it can be achieved with a reversal, by inserting an idler gear into one, or the other gear train. It is then possible using a brake to have a bidirectional output that can be zero.
Here is a plot with one negative ratio coefficient.
Notice how A and B are positive, while Y can be negative.
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You can hold the output static by setting ##GR=0##:
$$0 = \left(1-\frac{1}{2}\frac{\omega_{iR}}{\omega_{in}}\right)GR_L + \frac{1}{2}\frac{\omega_{iR}}{\omega_{in}}GR_R$$
$$\frac{1}{2}\frac{\omega_{iR}}{\omega_{in}}GR_L - GR_L = \frac{1}{2}\frac{\omega_{iR}}{\omega_{in}}GR_R$$
$$\frac{1}{2}\frac{\omega_{iR}}{\omega_{in}}(GR_L - GR_R) = GR_L$$
Or:
$$\frac{\omega_{iR}}{\omega_{in}} = \frac{2GR_L}{GR_L - GR_R}$$
Using the other equation:
$$0 = \frac{\omega_{iL}GR_L + \omega_{iR}GR_R}{\omega_{iL} + \omega_{iR}}$$
$$\omega_{iL}GR_L = - \omega_{iR}GR_R$$
$$\frac{\omega_{iL}}{\omega_{iR}} = - \frac{GR_R}{GR_L}$$
So whatever direction you end up on one side, the other side will rotate in reverse.
Also, since power has to be conserved, at least one of the shafts becomes the output if the friction is not enough.
$$0 = \left(1-\frac{1}{2}\frac{\omega_{iR}}{\omega_{in}}\right)GR_L + \frac{1}{2}\frac{\omega_{iR}}{\omega_{in}}GR_R$$
$$\frac{1}{2}\frac{\omega_{iR}}{\omega_{in}}GR_L - GR_L = \frac{1}{2}\frac{\omega_{iR}}{\omega_{in}}GR_R$$
$$\frac{1}{2}\frac{\omega_{iR}}{\omega_{in}}(GR_L - GR_R) = GR_L$$
Or:
$$\frac{\omega_{iR}}{\omega_{in}} = \frac{2GR_L}{GR_L - GR_R}$$
Using the other equation:
$$0 = \frac{\omega_{iL}GR_L + \omega_{iR}GR_R}{\omega_{iL} + \omega_{iR}}$$
$$\omega_{iL}GR_L = - \omega_{iR}GR_R$$
$$\frac{\omega_{iL}}{\omega_{iR}} = - \frac{GR_R}{GR_L}$$
So whatever direction you end up on one side, the other side will rotate in reverse.
Also, since power has to be conserved, at least one of the shafts becomes the output if the friction is not enough.
rajava007
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Thank you everyone for helping me with this question. It originally started with the fantasy of discovering a new CVT concept, however along the way I learned many new things! Once again I thank you all!
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