Mastering Physics 10.85 - Dynamics of Rotational Motion

In summary, a 5.30 kg ball is dropped from a height of 11.5 m above one end of a uniform bar that pivots at its center. The bar has mass 8.50 kg and is 9.00 m in length. At the other end of the bar sits another 5.40 kg ball, unattached to the bar. The dropped ball sticks to the bar after the collision. The 1st ball has a velocity of 15 \frac{m}{s} and hits the bar at an angle of 2.48 degrees.
  • #1
youvecaughtme
6
0
This is my first post on here; I hope it will be worth it. I haven't been able to find an adequate solution to this elsewhere.

Homework Statement



A 5.30 kg ball is dropped from a height of 11.5 m above one end of a uniform bar that pivots at its center. The bar has mass 8.50 kg and is 9.00 m in length. At the other end of the bar sits another 5.40 kg ball, unattached to the bar. The dropped ball sticks to the bar after the collision.

Homework Equations



[itex]W_t=K_t[/itex]
[itex]L_i=L_f[/itex]
[itex]L=mvr[/itex]
[itex]v=r\omega[/itex]

The Attempt at a Solution



First, I defined the data given as following:
[itex]m_1 = 5.3kg, h_1 = 11.5 m, m_b = 8.5 kg, \ell = 9.00m, m_2 = 5.4kg[/itex]

Then, I looked up the moments of inertia for the bar and balls relative to the center of the bar, then found the total of these:

[itex]I_b=\frac{1}{12}m_b(\frac{\ell}{2})^2=8.94 kg \, m^2[/itex]
[itex]I_1=m_1(\frac{\ell}{2})^2=107 kg \, m^2[/itex]
[itex]I_2=m_2(\frac{\ell}{2})^2=109 kg \, m^2[/itex]
[itex]I_t=\sum I = 225.6 kg \, m^2[/itex]

Then, I found the resulting velocity of the 1st ball when it hits the bar:
[itex]m_1h_1g = I_2\omega_2^2 \implies v = \sqrt{2h_1g} \implies v = 15 \frac{m}{s}[/itex]

Then I used the conservation of angular momentum to find the final angular velocity after the bar has rotated:
[itex]L_1 = m_1v_1\frac{\ell}{2}=357.75Nms[/itex]
[itex]L_2=I_t\omega[/itex]
[itex]L_1=L_2 \implies I_t\omega = L_1 \implies \omega = \frac{L_1}{I_t} = 1.59 \frac{rad}{sec}[/itex]

Then I found the initial velocity of the ball moving upwards from the angular velocity and used the work energy theorem to find the final height of the ball.
[itex]v=\frac{\ell}{2} \omega \implies v=7.14 \frac{m}{s}[/itex]
[itex]\frac{1}{2}m_2v^2=m_2gh_2 \implies h_2=\frac{v^2}{2g} \implies h_2 = 2.60 m[/itex]

However, this is the incorrect value for [itex]h_2[/itex]. Any ideas?
 
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  • #2
youvecaughtme said:
[itex]I_b=\frac{1}{12}m_b(\frac{\ell}{2})^2=8.94 kg \, m^2[/itex]
Double check that value.
 
  • #3
Doc Al said:
Double check that value.

That's embarrassing; nice catch! I tried it with this updated value and still got the wrong answer:


[itex]I_b=\frac{1}{12}m_b(\frac{\ell}{2})^2=14.3 kg \, m^2[/itex]
[itex]I_1=m_1(\frac{\ell}{2})^2=107 kg \, m^2[/itex]
[itex]I_2=m_2(\frac{\ell}{2})^2=109 kg \, m^2[/itex]
[itex]I_t=\sum I = 230 kg \, m^2[/itex]

Then, I found the resulting velocity of the 1st ball when it hits the bar:
[itex]m_1h_1g = I_2\omega_2^2 \implies v = \sqrt{2h_1g} \implies v = 15 \frac{m}{s}[/itex]

Then I used the conservation of angular momentum to find the final angular velocity after the bar has rotated:
[itex]L_1 = m_1v_1\frac{\ell}{2}=357.75Nms[/itex]
[itex]L_2=I_t\omega[/itex]
[itex]L_1=L_2 \implies I_t\omega = L_1 \implies \omega = \frac{L_1}{I_t} = 1.55 \frac{rad}{sec}[/itex]

Then I found the initial velocity of the ball moving upwards from the angular velocity and used the work energy theorem to find the final height of the ball.
[itex]v=\frac{\ell}{2} \omega \implies v=7.00 \frac{m}{s}[/itex]
[itex]\frac{1}{2}m_2v^2=m_2gh_2 \implies h_2=\frac{v^2}{2g} \implies h_2 = 2.50 m[/itex]
 
  • #4
Just curious: What's the initial angle of the bar? Horizontal?
 
  • #5
Doc Al said:
Just curious: What's the initial angle of the bar? Horizontal?

I assumed it was; the question statement that I posted is all of the information that I have.
 
  • #6
Your work looks OK to me. My only suggestion, if it's an online system that may be fussy about numeric values, is to redo the calculation without round off intermediate steps. (In case that's what you did.) That may affect the answer a bit.

What book is this from?
 
  • #7
Doc Al said:
Your work looks OK to me. My only suggestion, if it's an online system that may be fussy about numeric values, is to redo the calculation without round off intermediate steps. (In case that's what you did.) That may affect the answer a bit.

What book is this from?

Hm, I just tried the calculation again without any rounding and I got 2.48 m and the online system still rejected it. Thanks for taking a look at this, though!

It's from Sears & Zemansky's University Physics 13e.

Edit:
Somebody pointed out (on Facebook) that I shoudn't be using [itex]\frac{\ell}{2}[/itex] for the calculation of the moment of inertia of the bar and I realized that I didn't notice that when you pointed it out. This made my answer come out right.
 
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  • #8
youvecaughtme said:
Edit:
Somebody pointed out (on Facebook) that I shoudn't be using [itex]\frac{\ell}{2}[/itex] for the calculation of the moment of inertia of the bar and I realized that I didn't notice that when you pointed it out. This made my answer come out right.
Good!

(I should have checked to make sure that you corrected it.)
 

FAQ: Mastering Physics 10.85 - Dynamics of Rotational Motion

1. What is rotational motion?

Rotational motion is the movement of an object around a fixed point, also known as the axis of rotation. This type of motion can be seen in objects such as wheels, gears, and planets.

2. What is the difference between linear and rotational motion?

Linear motion is the movement of an object in a straight line, while rotational motion involves movement around an axis. Linear motion can also be described by its speed and velocity, while rotational motion is described by its angular speed and angular velocity.

3. How is torque related to rotational motion?

Torque is a measure of the force that causes an object to rotate around an axis. It is directly related to the angular acceleration of an object in rotational motion, with a larger torque resulting in a greater angular acceleration.

4. Can an object have both linear and rotational motion?

Yes, an object can have both linear and rotational motion. For example, a rolling ball has both linear motion as it moves forward, and rotational motion as it rotates around its center point.

5. How is centripetal force related to rotational motion?

Centripetal force is the force that keeps an object moving in a circular path. In rotational motion, this force acts towards the center of the rotation, causing the object to continue its circular motion. Without centripetal force, the object would move in a straight line tangential to the circular path.

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