Jump to content

Slow Yoyo


encipher

Recommended Posts

Hi,

 

I am working with a couple of highschool students on a physics project their class is doing. They have to construct a yoyo that will fall a distance of 2 meters in the GREATEST amount of time. Mechanical friction cannot be used as a means of slowing the yoyo down.

 

The maximum allowed mass is 1000grams and the maximum diameter / length is 20cm.

 

We came up with a square shape and a thin rod in between. We acheived a time of about 3 minutes.

 

Now today one of the students talked to me about the 'competition'. Apparently a rivaling group claimed to have gotten the yoyo slowed down to 45 minutes over the 2 meter drop. I have thought about how this is possible without friction being a factor and within the guidlines of the rules, but have yet to come up with a workable idea. Any thoughts on the setup they might have used? Also,it cannot be lighter than air.

 

Thank you

Link to comment
Share on other sites

Hi,

 

I am working with a couple of highschool students on a physics project their class is doing. They have to construct a yoyo that will fall a distance of 2 meters in the GREATEST amount of time. Mechanical friction cannot be used as a means of slowing the yoyo down.

 

The maximum allowed mass is 1000grams and the maximum diameter / length is 20cm.

 

We came up with a square shape and a thin rod in between. We acheived a time of about 3 minutes.

 

Now today one of the students talked to me about the 'competition'. Apparently a rivaling group claimed to have gotten the yoyo slowed down to 45 minutes over the 2 meter drop. I have thought about how this is possible without friction being a factor and within the guidlines of the rules, but have yet to come up with a workable idea. Any thoughts on the setup they might have used? Also,it cannot be lighter than air.

 

Thank you

 

Ah, but can it be as light as air?

 

Is air resistance counted as mechanical friction? If not, cross-vanes (making it look like a water-wheel) will help slow it down and dissipate energy.

 

You want to maximize the moment of inertia, so that it takes up the maximum energy with minimal rotation speed. You also want to choose your axle to maximize rotation at the expense of linear motion.

Link to comment
Share on other sites

Hi,

 

Well, their paper says it must be heavier than air, and no, air resistance cannot be a factor.

 

What we went with was a Square, with the insides cut out, except for rods to connect the axle to (which is very thin) that way we have a large moment of inertia. Now with that design, I mathematically calculated it to be something around 147 seconds (using conservation of energy) and the test was pretty close.

 

Now I don't know what could possibly give 45 minutes.

Link to comment
Share on other sites

Why a square and not a circle?

 

 

The only thing I can think of to extend the time is to come up with some kind of winding scheme to make the yo-yo partly rewind itself before the two meters have been reached.

 

Because the moment of inertia of a square is greater than that of a circle (within the given dimentions)

 

 

I calculated the moment of inertia of the square to be [math]\frac{1}{3}MA^2[/math]

 

Where A is the length of one side.

 

As opposed to that of a hoop which would be:

 

[math]MR^2[/math]

 

where R is the radius of the hoop.

 

Since the maximum length of the side or radius can be 20cm.. and the mass doesnt matter (sine according to conservation of energy it cancels out).. We figured the square shape would be the shape with the largest moment of inertia.

Link to comment
Share on other sites

does the yoyo need to come back up?

 

i think you're getting stuck on linear inertia, radial intertia is more along the lines of levers.

 

if the mass is concentrated around the rim and the spindle is 1 cm radius, the mass will need to travel 20x faster than the centre of the yoyo.

so you then divide G by 20 to get your final acceleration, roughly 0.5 m/s.

 

if the mass were closer in, the ratio is proportionally less so the mass needn't accelerate as much so the yoyo accelerates faster.

 

mechanical dampenning is out... how about electrical dampenning...

use an inductive load on a counter-rotating wheel. kinetic energy is turned into heat via ohmic heating so it's not "mechanical friction"

Link to comment
Share on other sites

no, the yoyo does not need to go back up.

 

Yeah, concentrating mass on the edge is key, but really making the yoyo heavier will not matter, since mass cancels out according to the following equation:

 

 

[math]mgh = \frac{1}{2}mv^2 + \frac{1}{2}I\omega^2[/math]

 

therefore what really matters is what the radius of the object is (for its moment of inertia). Or maybe I am wrong, any thoughts?

Link to comment
Share on other sites

Because the moment of inertia of a square is greater than that of a circle (within the given dimentions)

 

 

I calculated the moment of inertia of the square to be [math]\frac{1}{3}MA^2[/math]

 

Where A is the length of one side.

 

As opposed to that of a hoop which would be:

 

[math]MR^2[/math]

 

where R is the radius of the hoop.

 

Since the maximum length of the side or radius can be 20cm.. and the mass doesnt matter (sine according to conservation of energy it cancels out).. We figured the square shape would be the shape with the largest moment of inertia.

 

 

Ok. I had interpreted maximum dimension to be the diagonal, in which case the circle wins, but if it's the side length then you are indeed correct.

 

The mass does matter in the limit of low density, where you can't ignore the bouyant force of the air.

Link to comment
Share on other sites

I calculated the moment of inertia of the square to be

[math]\frac{1}{3}MA^2[/math]

Where A is the length of one side.

How did you found that ?

I google "moment of inertia and I found [math]\frac{1}{6}MA^2[/math] on that site

http://www.physics.uoguelph.ca/tutorials/torque/Q.torque.inertia.html

 

If you bring A to R you have [math]\frac{2}{3}MR^2[/math]

 

I am not very good in math but I would like to know theorically how long it will take the yoyo if we use a 2 mm radius axel with the cylinder geometry [math]MR^2[/math]

Thanks

Link to comment
Share on other sites

Ok I will give it a try

using g=10m/s^2

the force is mg = 1kg*10m/s^2 = 10 Newton

the torque t on the axel of 1mm radius = F * r = 10 N * .001 m = .01 N.m

the moment of inertia for a 10 cm radius cylinder is MR^2 = 1kg * (.1m)^2 = .01

angular acceleration = torque / moment of inertia = .01/.01= 1 rad/sec^2

on the axel 1mm = 1 radian then 2m = 2000 radian

2000 radian = 1/2 angular acceleration * time^2

sqrt 4000 = time = 62sec

It look like a short time...

What do you think of it ?

Link to comment
Share on other sites

Well, its kinda messy, but it looks ok.

 

Yes the moment of inertia of a square is 1/6 MA^2.

 

But I mentioned earlier that I had cut out the inside of the square, making it like a hoop. But square. and according to the general formula: [math]I = \int r^2 dm[/math]

 

I derived that moment of inertia (if you would like to see me work i would be glad to post it. ) Now it would actually be that + [math] 4 (\frac{1}{3}ML^2)[/math] for the 4 spokes that connect it to the axle.

 

 

I talked to a few of the students, and they mentioned that their friends said something about a counterweight being used to achieve the slow speed. Anyone have any thoughts on that?

Link to comment
Share on other sites

sorry, i thought you meant 20cm max radius, a square has a max width of ~28cm, so the optimum would be to concentrate the mass at the corners of a square of side length 20cm.

try to get as close as possible to the 1kg, the more the mass is concentrated, the less the mass of the spindle effects the descent. if you had a winding arrangement with a pin such that it moves down a distance, then back up over and over again, unavoidable natural losses can be utilised.

 

a counter weight can be used to lock a gearing system to vertical, the spindle turns relative to the counter weight, transferring the torque through the gears to spin the yoyo X times faster than normal dividing the descent rate by the gearing ratio.

Link to comment
Share on other sites

Why not use a counterweight? As the yoyo moves down. spinning out on its string, have another string attached to the axle pulling a counterweight up. The balance between the weights will determine how fast the yoyo goes. If they are nearly equivalent, the yoyo will move very slowly.

 

You might need to use a long weight on two strings that attach each side of the main yoyo string to keep it balanced, but that's easy enough. As long as the yoyo is slightly heavier than the counterweight, it will move down and wind the counterweight up. You'd just have to play with the different weights a bit.

 

Just a thought.

Link to comment
Share on other sites

So if my calculations are good, 62 sec is far less than what encipher did and by a factor that is more than any improvement only by work on the geometry.

If you do the calculation with the square geometry, you will still have less than the 3 minutes you achive and by the others result. Some other factor made the difference between the theory and the experiment.

I came up with the concept of a yoyo that will take more than an infinite time to travel the 2 meter :) But it is agains the defenition of a yoyo. A yoyo must rotate.

I thought that an inbalance in the real yoyo made the difference.

A small imbalance will displace the center of mass from the geometric center. The torque will vary like an offset sine.

Chirstmass diner is waiting will continue later....

Link to comment
Share on other sites

Actually, my calculation came up to be pretty close to what I got in real life.

 

 

i started off with the folowing:

 

[math]mgh = \frac{1}{2}mv^2 + \frac{1}{2}I\omega^2[/math]

 

by subsituting in [math]\frac{v}{r}[/math] for omega, where V is the linear velocity of the yoyo and r is the radius of the AXLE. and subsituting in

[math]\frac{1}{3}MA^2[/math] for the moment of inertia (I)

 

the Mass cancels out, and A is the length of one side of the square.

 

Re-arranging the equation for the velocity will give you the following:

 

[math]\large v^2 = \frac{gh}{\frac{1}{2} + \frac{A^2}{6r^2}}[/math]

 

then using kinematics, the general formula [math] v_f^2 = v_i^2 + 2ax[/math]

 

We know that the initial velocity is zero so that cancels out

 

Solving for a and plugging in the above equation gives:

[math]\large{a = \frac{gh}{2h(\frac{1}{2} + \frac{A^2}{6r^2})}}[/math]

 

 

Then Plugging in all the numeical values:

g = 9.81 meters/s/s

h = 2 meters

A = 20 centimeters = .2 meters

r = .5 millimeters = .0005 meters

 

The acceleration is: .000184 meters/s/s (Yes, I hate sig figs)

 

Then, using the equation [math] x = v_it + \frac{1}{2}at^2[/math]

subtituting in the above value for a, and 2 for x, and solving for t

 

I get the following: 147.47 seconds.. divide by 60 find remainder, i get:

 

2 minutes and 27 seconds. Very close the the experimental value acheived.

 

I will be attempting to setup a counterweight yoyo and will post my results.

Link to comment
Share on other sites

Ok one big difference is that you use a 1mm diameter axel and in my setup I used a 2mm axel.

My idea of moving the center of mass out of the axel will create a two time cycle:

The first half of the cycle begin when the center of mass is just pass over the axel, the torque is in the direction to unwind the yoyo. The rotation speed increase and also the linear speed. When the center of mass is at the lowess point in the rotation the torque is zero and the rotation bring the center of mass on the other side of the axel. The torque is in the opposite direction slowing the rotation until the center of mass pass over the axel again. Hope you understand the idea :)

The first half cycle convert potential energy to angular momentum and the second half of the cycle convert back some angular momentum back to potential energy.

I think that by fine tunning the unbalance you can achive any speed. If to much unbalance the yoyo won't go down so there is a limit to the unbalance.

I would use a perfectly balance yoyo an used some putty to unbalance it and do some experiment to see how much putty to add and where to add it. Important to keep it balanced horizontally :)

Link to comment
Share on other sites

The first half cycle convert potential energy to angular momentum and the second half of the cycle convert back some angular momentum back to potential energy.

 

Careful, you're mixing terms here. You can convert potential energy into rotational and translational kinetic energy in this system, but you only change angular momentum by exerting a torque.

Link to comment
Share on other sites

  • 2 weeks later...

Yes actually, I spoke to them after I came back from my vacation. The design they were talking about was an axle, and two cylinders on each end. Inside the cylinders on each end was water, and a series of segments. (imagine a waterwheel, but closed and there is water in one of the sections.) as the yoyo rotates, there are tiny holes in each flaps that allows water to flow slowly from one section to the other. That is how it took a very long time to reach its destination.

Link to comment
Share on other sites

Create an account or sign in to comment

You need to be a member in order to leave a comment

Create an account

Sign up for a new account in our community. It's easy!

Register a new account

Sign in

Already have an account? Sign in here.

Sign In Now
×
×
  • Create New...

Important Information

We have placed cookies on your device to help make this website better. You can adjust your cookie settings, otherwise we'll assume you're okay to continue.