Rotational Motion of a thin rod

In summary: The kinetic energy and net forces remain the same, but the moments of inertia change and are calculated using the parallel axis theorem. The new CM is also used in the calculation of the moments of inertia.
  • #1
Bones
108
0

Homework Statement


A 4.00 kg mass and a 3.00 kg mass are attached to opposite ends of a thin 44 cm long horizontal rod (see figure). The system is rotating at angular speed ω = 6 rad/s about a vertical axle at the center of the rod.

(a) Determine the kinetic energy K of the system.


(b) Determine the net force on each mass.


(c) Repeat parts (a) and (b) assuming that the axle passes through the CM of the system.



Homework Equations





The Attempt at a Solution


KE=1/2(0.3388m*N)(6rad/s)^2=6.10 J
F1=(4kg)(6rad/s)^2(0.22m)=31.7 N
F2=(3kg)(6rad/s)^2(0.22m)=23.8 N
CM=(4kg)(0.22m)+(3kg)(0.22m)/4kg+3kg=0.22m

How does the CM change the problem? I am having trouble figuring out the second set of answers.
 
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  • #2
The moment of inertia of a system is given by the sum of the moments of intertia of each of the system's components, the spheres and the rod. Remember the parallel axis theorem when solving for the moments of inertia when the axis is moved to the center of mass.
 
  • #3
Bones said:
KE=1/2(0.3388m*N)(6rad/s)^2=6.10 J
F1=(4kg)(6rad/s)^2(0.22m)=31.7 N
F2=(3kg)(6rad/s)^2(0.22m)=23.8 N
CM=(4kg)(0.22m)+(3kg)(0.22m)/4kg+3kg=0.22m

How does the CM change the problem? I am having trouble figuring out the second set of answers.

What are you doing with the Center of mass equation? What lengths to the 2 masses do you get?
And aren't they supposed to add to .44 m?
 
  • #4
Center of mass = [tex]\frac{\sum{(distance)(mass)}}{\sum{mass}}[/tex]

make sure to define your co-ordinate system

remember the CM is not changing, the rod is only at [tex]\frac{d}{2}[/tex] of the masses not at the center of mass

I just read your CM equation, you are using [tex]\frac{d}{2}[/tex] as your starting point, so wouldn't right be positive and left be negative?
 
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  • #5
LowlyPion said:
What are you doing with the Center of mass equation? What lengths to the 2 masses do you get?
And aren't they supposed to add to .44 m?

I am confused.
 
  • #6
Bones said:
I am confused.

What is the distance of each mass from the center of mass?

Can't you figure where the center of mass is and what those distances to each mass are?
 
  • #7
Bones said:
I am confused.

Hey set your co-ordinates correctly, if your center point is 0, then to the right 0.22 m is positive to the left 0.22 is negative...---->THINK X AXIS <----- So you have [tex]\frac{(4)(-0.22)+(3)(+0.22)}{3+2}[/tex]

Your displacements are vectors, they have direction!
Its pretty straight forward

Untitled.jpg
 
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  • #8
So the center of mass is -.03143m

Thanks!
 
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  • #9
Bones said:
So the center of mass is -.03143m

Yes, or 0.0314 meters to the left.
 
  • #10
More accurately CM is defined as [tex]\sum{\frac{m_{1}\vec{r_{1}}+m_{2}\vec{r_{2}}+...+m_{n}\vec{r_{n}}}{m_{1}+m_{2}+...+m_{n}}}[/tex]
 
  • #11
It changes now because the axle is at the CM instead of [tex]\frac{d}{2}[/tex]
 

What is rotational motion?

Rotational motion refers to the movement of an object around a fixed axis or point. This type of motion is circular or curvilinear in nature and can occur in both natural and man-made systems.

How is rotational motion different from linear motion?

Rotational motion involves the movement of an object around an axis, while linear motion involves the movement of an object in a straight line. In rotational motion, the object's position and orientation change continuously, while in linear motion, the object's position changes linearly with time.

What is a thin rod?

A thin rod is a long, slender object with a uniform cross-section. It can be made of various materials such as metal, wood, or plastic and is often used in engineering and physics experiments to study rotational motion.

What factors affect the rotational motion of a thin rod?

The rotational motion of a thin rod is affected by factors such as its length, mass, distribution of mass, and the force applied to it. The shape of the object and the surface it is rotating on can also impact its motion.

How is rotational motion of a thin rod measured?

The rotational motion of a thin rod is typically measured in terms of its angular displacement, velocity, and acceleration. These values can be calculated using equations such as angular displacement = θ, angular velocity = ω, and angular acceleration = α.

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