Rotational Motion of the Yo-Yo

In summary: I think it is easier to use the axis through the center of mass. In which case you need to use the parallel axis theorem to find the moment of inertia. You also need to remember that the different parts of the yoyo will have different angular accelerations. Can you follow the steps in post #6 to get the acceleration of the center of mass, angular acceleration and tension force?In summary, a yo-yo is made up of two larger discs with radius R = 4.00 cm and mass M = 30.0 g each, and a smaller disc with radius r = 0.700 cm and mass m = 5.00 g in the middle. The string is considered massless and
  • #1
Haveagoodday
43
1
Skjermbilde 2015-10-29 kl. 21.45.07.png


1. Homework Statement

A yo-yo roughly speaking consists of two round, uniform discs, sandwiched

around a third smaller disc. A string is wound around the middle disc, and so

the yo-yo may roll up and down as the string winds and unwinds. Consider

such a yo-yo, with the two bigger discs having radius R = 4.00 cm and mass

M = 30.0 g each; and the smaller disc in the middle having radius r = 0.700

cm and mass m = 5.00 g. The string is taken to be massless, and infinitely

thin.

a) What is the total moment of inertia of the yo-yo, around an axis going

through the centre of the discs? Indicate both the algebraic expression and

a number.

b) The end of the string is now fastened to something at a fixed position

(like a finger), and the yo-yo is let drop towards the floor. Identify the forces

acting on the yo-yo, and for each, indicate whether they provide torque, work,

impulse and/or acceleration to the yo-yo.

c) What is the acceleration of the yo-yo downwards; what is its angular

acceleration? How large is the string force?

d) How big a fraction of the total kinetic energy goes into the rotating motion?

The Attempt at a Solution


Can somebody check my solutions?
a)
ΣI= 1/2mr^2 + MR^2=4.812 kg*m^2
b)
There are forces like force of gravity and string force
gravity provides Work and acceleration
string provides torque and impulse

c) a=g= 9.80 m/s^2
Fg=2Mg=0.588 N
Fg=mg=0.049 N
τ=RFg=0.02352
τ=rFg=3.43*10^-4
α=Στ/ΣI=5.6 rad/s^2
Fs=mg/1-(mR^2/ΣI)= 0.388 N

d) haven't solved this one yet, does anybody have an idea for how to solve this one?
 
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  • #2
Haveagoodday said:
View attachment 91041

1. Homework Statement

A yo-yo roughly speaking consists of two round, uniform discs, sandwiched

around a third smaller disc. A string is wound around the middle disc, and so

the yo-yo may roll up and down as the string winds and unwinds. Consider

such a yo-yo, with the two bigger discs having radius R = 4.00 cm and mass

M = 30.0 g each; and the smaller disc in the middle having radius r = 0.700

cm and mass m = 5.00 g. The string is taken to be massless, and infinitely

thin.

a) What is the total moment of inertia of the yo-yo, around an axis going

through the centre of the discs? Indicate both the algebraic expression and

a number.

b) The end of the string is now fastened to something at a fixed position

(like a finger), and the yo-yo is let drop towards the floor. Identify the forces

acting on the yo-yo, and for each, indicate whether they provide torque, work,

impulse and/or acceleration to the yo-yo.

c) What is the acceleration of the yo-yo downwards; what is its angular

acceleration? How large is the string force?

d) How big a fraction of the total kinetic energy goes into the rotating motion?

The Attempt at a Solution


Can somebody check my solutions?
a)
ΣI= 1/2mr^2 + MR^2=4.812 kg*m^2

Are you sure about the units of I here? 1 kg-m2 represents a relatively healthy inertia. I'm not sure a person could handle a yo-yo with this much inertia.

In the problem statement, the masses of the yo-yo parts are given in grams, not kilograms, and the radii of the various parts are given in centimeters, not meters.

b)
There are forces like force of gravity and string force
gravity provides Work and acceleration
string provides torque and impulse

c) a=g= 9.80 m/s^2
Fg=2Mg=0.588 N
Fg=mg=0.049 N
τ=RFg=0.02352
τ=rFg=3.43*10^-4

You're showing two different values of τ here. What are the units of τ? Why do you have two different values?

α=Στ/ΣI=5.6 rad/s^2
Fs=mg/1-(mR^2/ΣI)= 0.388 N

d) haven't solved this one yet, does anybody have an idea for how to solve this one?
 
  • #3
SteamKing said:
Are you sure about the units of I here? 1 kg-m2 represents a relatively healthy inertia. I'm not sure a person could handle a yo-yo with this much inertia.

In the problem statement, the masses of the yo-yo parts are given in grams, not kilograms, and the radii of the various parts are given in centimeters, not meters.
You're showing two different values of τ here. What are the units of τ? Why do you have two different values?
Sorry i ment to write 4.812*10^-5 kg*m^2 in a
 
  • #4
SteamKing said:
Are you sure about the units of I here? 1 kg-m2 represents a relatively healthy inertia. I'm not sure a person could handle a yo-yo with this much inertia.

In the problem statement, the masses of the yo-yo parts are given in grams, not kilograms, and the radii of the various parts are given in centimeters, not meters.
You're showing two different values of τ here. What are the units of τ? Why do you have two different values?
In c i calculated the torque for gravitational force for the outer parts and the inner part.
 
  • #5
Haveagoodday said:
gravity provides Work and acceleration
Does it also provide impulse or torque?
(The torque question is a bit unclear. The torque of a force depends on the axis you choose. Is it right to assume mass centre?)
Haveagoodday said:
c) a=g= 9.80 m/s^2
Fg=2Mg=0.588 N
Fg=mg=0.049 N
As with part a), it would be better to keep everything algebraic as long as possible, only plugging in numbers at the end. Makes it easier for others to follow your working. But you do need to use distinct variables, not keep reusing a, m, F etc. with different meanings.
Haveagoodday said:
τ=rFg=3.43*10^-4
I see you now consider Fg to be generating torque, but about which axis? Is that the axis you used for calculating I?
 
  • #6
I have a question about the situation in b), wouldn't the string force also provide acceleration? and the acceleration of the yoyo isn't the same as g (9.80) ,some of the energy is transferred to the spinning motion, right?
 
  • #7
hooolahooop said:
I have a question about the situation in b), wouldn't the string force also provide acceleration? and the acceleration of the yoyo isn't the same as g (9.80) ,some of the energy is transferred to the spinning motion, right?
The linear acceleration is determined by the net force. I don't much like the question of whether the tension provides acceleration. It doesn't do any work, but does influence the acceleration. Yes, some of the energy goes into spinning the yoyo.

Let's try to get the rotational acceleration right. What axis do you want to use? You can use either mass centre of the yoyo or any point fixed in space. Having chosen it, what is the net torque about that axis and what is the yoyo's moment of inertia about it?
 
  • #8
haruspex said:
The linear acceleration is determined by the net force. I don't much like the question of whether the tension provides acceleration. It doesn't do any work, but does influence the acceleration. Yes, some of the energy goes into spinning the yoyo.

Let's try to get the rotational acceleration right. What axis do you want to use? You can use either mass centre of the yoyo or any point fixed in space. Having chosen it, wad is the net torque about that axis and what is the yoyo's moment of inertia about it?

The question are asking for acceleration of the yoyo downwards i used different equations and calculated the total moment of inertia, where i got that

T(torque) = r * Fs(spring force)

T (torque) = I * alpha --> I * alpha = r*Fs ----> alpha = a/r

Ma = Mg - Fs

Fs = [I (total) *(a/r)]/r ----> Ma = Mg - (I*a/r^2)

solve for a -- > a = (M*g*r ^2) /[ r^2*M + I(total)] where r is the radius of the small disc because the string is around this disci used an axis through the middle( center of mass)
 
  • #9
What do you use as unit for radius and mass? (m and kg?) Also what did you get as total inertia?
 
  • #10
hooolahooop said:
The question are asking for acceleration of the yoyo downwards i used different equations and calculated the total moment of inertia, where i got that

T(torque) = r * Fs(spring force)

T (torque) = I * alpha --> I * alpha = r*Fs ----> alpha = a/r

Ma = Mg - Fs

Fs = [I (total) *(a/r)]/r ----> Ma = Mg - (I*a/r^2)

solve for a -- > a = (M*g*r ^2) /[ r^2*M + I(total)] where r is the radius of the small disc because the string is around this disci used an axis through the middle( center of mass)
Yes, that all looks right.
 
  • #11
For angular acceleration, i got a(alpha)=g/(R+I/(mR))
 

1. What is rotational motion of a yo-yo?

The rotational motion of a yo-yo refers to the spinning or rolling motion of the yo-yo around its central axis.

2. How does the yo-yo maintain its rotational motion?

The yo-yo maintains its rotational motion through the conservation of angular momentum, which means that the angular momentum of the yo-yo remains constant unless an external torque is applied.

3. How does the string affect the rotational motion of the yo-yo?

The string affects the rotational motion of the yo-yo by providing the necessary tension and torque to keep the yo-yo spinning. As the string unwinds, it increases the yo-yo's moment of inertia, slowing down its rotation. When the string is wound back up, it decreases the moment of inertia, increasing the yo-yo's rotational speed.

4. What factors affect the rotational motion of a yo-yo?

The rotational motion of a yo-yo can be affected by factors such as the length and weight of the string, the shape and weight distribution of the yo-yo, and the surface it is spinning on.

5. How is the rotational motion of a yo-yo related to its linear motion?

The rotational motion of a yo-yo is closely related to its linear motion. As the yo-yo spins, it also moves up and down the string in a linear motion. The speed and direction of the yo-yo's rotation directly affect its linear motion, and vice versa.

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