How Do You Calculate the Initial Acceleration of a Rod's Center of Mass?

Click For Summary
SUMMARY

The initial acceleration of a uniform rod's center of mass (CM) can be calculated using the equation Rmg(sinθ) = Iα, where R is the distance from the pivot to the CM, m is the mass, g is the acceleration due to gravity, θ is the angle of release, I is the moment of inertia, and α is the angular acceleration. For a rod of length 1.15 m released from an angle of 21.0°, the moment of inertia is I = (1/3)mL². The correct calculation yields an angular acceleration α of 4.58 rad/s², leading to a linear acceleration a of 2.63 m/s² for the CM.

PREREQUISITES
  • Understanding of rotational dynamics
  • Familiarity with the moment of inertia for a uniform rod
  • Knowledge of trigonometric functions (sine and cosine)
  • Basic principles of angular and linear acceleration
NEXT STEPS
  • Study the derivation of the moment of inertia for various shapes
  • Learn about the relationship between angular and linear acceleration
  • Explore the effects of different pivot points on rotational motion
  • Investigate the role of friction in rotational dynamics
USEFUL FOR

Students and educators in physics, mechanical engineers, and anyone interested in understanding the dynamics of rotational motion and acceleration calculations.

WillP
Messages
8
Reaction score
0
Pivot point on a Uniform Rod and Acceleration

I'm stuck on this question, which seems like it should be fairly simple:

A uniform rod of length 1.15 m is attached to a frictionless pivot at one end. It is released from rest from an angle theta = 21.0° above the horizontal. Find the magnitude of the initial acceleration of the rod's CM.
there's a graphic of it here:
http://capaserv.physics.mun.ca/msuphysicslib/Graphics/Gtype20/prob28_1012rod.gif

ok so what I've done so far is:
Rmg(sinθ) = Iα
Rmg(sinθ) = (1/3)mL^2α

getting the expression I = (1/3)mL^2 from my textbook for a uniform rod with a pivot at its end.

working that out I get:
(0.575)(9.8)(sin21) = (1/3)(1.15)^2 α
α = 4.58 rad/s

then converting α to a with:
a = Rα
a = (.575)(4.58)
a = 2.63 m/s^2

but apparently this isn't right.
can anyone help me out?
 
Last edited by a moderator:
Physics news on Phys.org
nevermind... my stupid mistake should have used cos instead of sin :redface:
 


The rotational moment of inertia is a measure of an object's resistance to rotational motion, similar to how mass is a measure of an object's resistance to linear motion. It is dependent on the object's mass distribution and the distance of the mass from the axis of rotation. In this case, the uniform rod has a moment of inertia given by I = (1/3)mL^2, where m is the mass of the rod and L is its length.

To find the initial acceleration of the rod's center of mass, we can use the rotational dynamics equation Rmg(sinθ) = Iα, where R is the distance from the pivot point to the center of mass, g is the acceleration due to gravity, θ is the initial angle above the horizontal, I is the moment of inertia, and α is the angular acceleration.

Substituting in the known values, we get (0.575)(9.8)(sin21) = (1/3)(1.15)^2α. Solving for α, we get α = 4.58 rad/s^2.

To find the linear acceleration of the center of mass, we can use the relation a = Rα, where a is the linear acceleration and R is the distance from the pivot point to the center of mass. Substituting in the values, we get a = (0.575)(4.58) = 2.63 m/s^2.

Your calculations look correct, so it's possible that there may be a mistake in the given values or the problem statement. Double check the given values and make sure they are correct. If they are, then your solution is correct.
 

Similar threads

Replies
16
Views
3K
Replies
3
Views
2K
Replies
4
Views
2K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 7 ·
Replies
7
Views
6K
  • · Replies 18 ·
Replies
18
Views
7K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 3 ·
Replies
3
Views
3K
Replies
6
Views
4K
  • · Replies 11 ·
Replies
11
Views
3K