Rotation : When will the rod slide off?

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Homework Help Overview

The discussion revolves around a problem involving the dynamics of a uniform rod partially resting on a rough horizontal surface. The scenario describes the rod being held stationary and then released, leading to its rotation about an edge. Participants are tasked with determining the angle at which the rod will begin to slide, considering the coefficient of friction.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the application of conservation of energy to relate angular motion and forces acting on the rod. There are attempts to derive expressions for angular velocity and energy loss, as well as considerations of forces acting on the rod during its motion.

Discussion Status

The discussion is active, with various approaches being explored. Some participants are providing insights into the relationships between forces and motion, while others are questioning the assumptions made regarding the forces acting on the rod. There is no explicit consensus, but multiple interpretations and lines of reasoning are being examined.

Contextual Notes

Participants are navigating through the complexities of the problem, including the effects of friction and the dynamics of rotational motion. There are indications of confusion regarding the forces involved, particularly the normal and frictional forces, and how they relate to the acceleration of the center of mass of the rod.

AlchemistK
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Homework Statement


one fourth length of a uniform rod of mass "m" and length "l" is placed on a rough horizontal surface and it is held stationary in horizontal position by means of a light thread. The thread is then burnt and the rod starts rotating about the edge. Find the angle between the rod and the horizontal when it is about to slide on the edge. The coefficient of friction between the rod and the surface is "μ"

Homework Equations


The Attempt at a Solution



I have a few more questions in a similar format, and I can't find the right way to tackle them. Could someone please point me in the right direction?

The answer as given in the book is θ= tan^-1 (4μ/13)
 
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Hi AlchemistK! :smile:

Start by using conservation of energy to find how dθ/dt depends on θ (before it slips). :wink:
 
Ok, after conserving energy, I got:
ω^2 = (24 g sinθ)/(7L)

where θ is the angle made by the rod with the horizontal.

On integrating, there comes a term of sinθ in the denominator and by applying the limits of θ from 0 to some angle θ, infinity comes up.

The loss in PE came out to be m*g*L*sinθ/4
The kinetic energy at any angle θ will be 1/2* I * ω^2
where I is m*(L^2)/48.
 
Last edited:
ok, now do the equation for:

Ftotal = mac.o.m

(sum of the forces on the rod = mass times acceleration of the centre of mass)​
 
In the direction of the rod,
ma = mgsinθ - μmgcosθ
 
no

you need to find the reaction force (call it R) at the table, from the acceleration

then you check to see whether µ is capable of producing R

(when it isn't, that's the answer)​
 
tiny-tim said:
from the acceleration

Do you mean the frictional force on the table due to the rode? (μmgcosθ)

Or the normal reaction due to the component of the weight of the rod? (mgcosθ)
 
are you sure that it's mgcosθ ?

use the previous equation to find the total reaction force R (including its direction)
 
Would that be the vector sum of mgcosθ and μmgcosθ? I can't see any more forces here.
 
  • #10
AlchemistK said:
Would that be the vector sum of mgcosθ and μmgcosθ?

No, it's the difference of ma and mg
 
  • #11
AlchemistK said:
Would that be the vector sum of mgcosθ and μmgcosθ? I can't see any more forces here.
tiny-tim said:
No, it's the difference of ma and mg


Aren't they numerically the same? ma - mg is equal and opposite to mgcosθ + μmgcosθ
 
  • #12
@tiny tim why did we find the relation b/w omega and theta
 

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