Is the tension of the string in a yoyo the same when descending and ascending?

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Homework Help Overview

The discussion revolves around the tension in the string of a yoyo during its ascending and descending motions. The yoyo consists of two uniform discs and is analyzed under the assumption of energy conservation.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants explore the relationship between tension and motion direction, with some suggesting that the tension remains constant while others argue it differs due to rotational effects. Various equations of motion and forces are discussed, including net force and angular acceleration.

Discussion Status

There is an active exploration of the problem, with participants offering differing views on the tension in the string. Some have provided calculations for the descending motion, while questions remain about the ascending motion. Guidance has been offered regarding the relationship between linear and rotational dynamics.

Contextual Notes

Assumptions about energy conservation and the fixed nature of the yoyo string are under discussion. The impact of rotational dynamics on tension is also a point of contention.

weesiang_loke
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Homework Statement


For a yoyo made of two uniform discs of radius R and each has mass M/2. A short shaft connecting the discs has a very small radius of r. A string is wrapped around the shaft and the yoyo is released with initial speed of zero. Assume that the string is vertical all times and energy in the system is conserved

My question is whether the tension of the string when the yoyo is descending and the tension of string when it is ascending is the same.

Homework Equations


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The Attempt at a Solution


I think that the tension is the same for both cases as the net force acting downwards should be the same if we want the yoyo to accelerate when it moves downwards and decelerate when it moves up again. So in this case the energy is conserved. Is this the correct explanation?
 
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The tension will not be the same. This is because when the yoyo is going down, say it rotates in the clockwise direction. What this does is change the direction of the frictional force acting on the string as it's wrapped around the smaller metal rod. When the yoyo is coming up, it's spinning the in the anticlockwise direction and the tension is in the opposite direction. Thus, the tension in both the cases will be different.
 
so what i get for descending motion:
assuming the tension in the string is T and the mass of the whole yoyo is M. so the net force acting in downwards direction:
we have M*g - T = M*a -----> force equation
T*r = I*\alpha where I is the moment of inertia and \alpha is the angular acceleration.

and \alpha = \frac{<i>a</i><sub>tangetial</sub>}{<i>r</i>}
I = 2* (0.5*(M/2)*R2
so by substition of T, we will get
atangential = \frac{2<i>g</i>}{2 + \frac{<i>R</i><sup>2</sup>}{<i>r</i><sup>2</sup>}}

and so the tension in string during the descending of the yoyo is \frac{<i>M*g*R</i><sup>2</sup>}{2<i>r</i><sup>2</sup> + R<sup>2</sup>}.


but i don't know how to determine the tension in the ascending motion. any hint?
 
hi weesiang_loke! :smile:
weesiang_loke said:
For a yoyo made of two uniform discs of radius R and each has mass M/2. A short shaft connecting the discs has a very small radius of r. A string is wrapped around the shaft and the yoyo is released with initial speed of zero. Assume that the string is vertical all times and energy in the system is conserved

My question is whether the tension of the string when the yoyo is descending and the tension of string when it is ascending is the same.

F = ma (using linear forces) takes no notice of rotation …

T will always equal mg - a, irrespective of the rotation

for an ordinary hand-held yoyo, i don't see how energy could possibly be conserved … the wrist muscles supply energy that keeps the yoyo going

however, if the top of the yoyo string is fixed, with the yoyo rolling-and-falling down the string only under gravity, bouncing off something, and then rolling up again, then the acceleration should be equal at each height on both trips, and so T will be equal also

(and of course work done, = ∫ T dh, will be the same)

(and the angular velocity and acceleration, ω and α, will be determined by the rolling constraints v = ωr and a = αr and by the conservation of energy equation :wink:)​
 
ok. got it. thanks.
 

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