Newton’s Second Law of Motion — Collar sliding on a rotating rod

Click For Summary
SUMMARY

The discussion centers on the application of Newton's Second Law of Motion in the context of a collar sliding on a rotating rod, utilizing polar coordinates. It establishes that the acceleration of the collar relative to the rod consists solely of the radial component, as the transverse component is effectively zero due to the collar being constrained to the rod's motion. This conclusion is supported by the understanding that the rod applies the necessary torque to the collar, ensuring that its transverse acceleration matches that of the rod.

PREREQUISITES
  • Understanding of Newton's Second Law of Motion
  • Familiarity with polar coordinates and their components
  • Basic knowledge of rotational dynamics
  • Concept of torque and its application in mechanics
NEXT STEPS
  • Study the derivation of acceleration components in polar coordinates
  • Explore the implications of torque in rotational motion
  • Investigate examples of constrained motion in mechanics
  • Learn about the applications of Newton's laws in complex systems
USEFUL FOR

Students of physics, mechanical engineers, and anyone interested in the dynamics of rotating systems and the application of Newton's laws in real-world scenarios.

mingyz0403
Messages
12
Reaction score
1
Homework Statement
The horizontal rod OA rotates about a vertical shaft according to the relation dθ/dt=10t, where
dθ/dt and t are expressed in rad/s and seconds, respectively. A 250 g collar B is held by a cord with a breaking strength of 18 N. Neglecting friction, determine,immediately after the cord breaks, (a) the relative acceleration of the collar with respect to the rod, (b) the magnitude of the horizontal force exerted on the collar by the rod.
Relevant Equations
Newton's Second Law
The soultion used polar corrdinates. Acceleration in polar corrdinates have radial and transeverse components.When calculating the acceleration of collar respect to the rod, the solution only calculates the radial component of acceleration. Is it because the collar is on the rod, so the transeverse acceleration component of the collar is the same as the rod. Acceleration of collar respect to rod=Acceleration of collar-Acceleration of Rod. Therefore, the transeverse component of acceleration of collar respect to the rod is 0?
 

Attachments

  • 1.png
    1.png
    45.7 KB · Views: 320
  • 2.png
    2.png
    53.5 KB · Views: 287
Physics news on Phys.org
mingyz0403 said:
Therefore, the transeverse component of acceleration of collar respect to the rod is 0?
Correct. The rod forces the collar with whatever torque is necessary.
 
  • Like
Likes   Reactions: mingyz0403
BvU said:
Correct. The rod forces the collar with whatever torque is necessary.
Ok, Thank you.
 

Similar threads

  • · Replies 2 ·
Replies
2
Views
3K
Replies
3
Views
9K
  • · Replies 8 ·
Replies
8
Views
2K
  • · Replies 6 ·
Replies
6
Views
5K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 3 ·
Replies
3
Views
3K
Replies
2
Views
7K
Replies
1
Views
2K
Replies
7
Views
2K
  • · Replies 23 ·
Replies
23
Views
3K