Find the magnitude of the initial acceleration of the rod's center of mass

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SUMMARY

The discussion centers on calculating the initial acceleration of a uniform rod's center of mass when released from a 17-degree angle above the horizontal. The correct approach involves using torque and moment of inertia equations, specifically torque = moment of inertia * angular acceleration and I = 1/3 ML². The key correction identified was replacing cosine with sine in the torque equation, leading to the correct angular acceleration calculation. Ultimately, the linear acceleration of the center of mass is determined using the formula a = α(L/2), yielding the correct answer.

PREREQUISITES
  • Understanding of rotational dynamics and torque
  • Familiarity with moment of inertia calculations, specifically I = 1/3 ML²
  • Knowledge of angular acceleration and its relationship to linear acceleration
  • Basic trigonometry, particularly the sine and cosine functions
NEXT STEPS
  • Study the derivation and application of torque in rotational motion
  • Learn about the moment of inertia for various shapes and its implications in dynamics
  • Explore the relationship between angular and linear acceleration in rigid body motion
  • Investigate common mistakes in applying trigonometric functions in physics problems
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Students studying physics, particularly those focusing on mechanics and rotational dynamics, as well as educators seeking to clarify concepts related to torque and angular motion.

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Homework Statement



A uniform rod of length 1.15m is attached to a frictionless pivot at one end. It is released from rest an angle theta=17.0 degrees above the horizontal.

Find the magnitude of the initial acceleration of the rod's center of mass

Homework Equations



torque=moment of inertia*angular acceleration
torque=length*force(perpendicular)

I=1/3 ML^2

The Attempt at a Solution



I set the torque about pivot equal to the moment of inertia about pivot times the angular acceleration to find the angular acceleration. Then I found the linear acceleration by multiplying the found angular acceleration by the length of rod. So my work was...

L/2*(Mg)cos17=1/3*ML^2*(angular acceleration)
3/2*(g/L)*cos17=(angular acceleration)
12.22 rad/s^2= (angular acceleration)

a=(angular acceleration)*L= 14.05 m/s^2

However the answer I got is wrong. (Unfortunately, I do not have access to the correct answer) What step did I miss?
 
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... L/2*(Mg)cos17=1/3*ML^2*(angular acceleration)

This should be the sin not the cos.

The com will then experience only a tangential acceleration:

a_t = r \alpha
 
I replaced the cos with the sin17 in my equation and I just tried to solve but I was told my answer was wrong. And I did exactly what you suggested. I wonder why that was wrong? Did I need to do something else?
 
Have you used the correct angle ? 17 deg above the horizontal is 90 + 17 from the vertical.
 
If you are trying to find the tangential acceleration of the centre of mass, wouldn't it be a_t = \alpha(L/2), since the centre of mass will be at half the length of a uniform rod? Just a thought.
 
Mentz114, thank you for mentioning that! I looked through some notes and saw I need to add 90 degrees. However, I just redid the problem, using the info you told me and what andrevdh told me, and oddly enough, I got the same answer!

hage567, I will try to find the initial acceleration with L/2 instead of L.
 
Thanks everyone, I got the right answer now.
 

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