Circular motion vector question

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Homework Help Overview

The discussion revolves around a problem in circular motion involving a particle sliding inside a vertical smooth semi-circular ring. The problem requires the application of conservation of energy and Newton's Second Law to determine the reaction force at a specific angle.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants explore the relationship between energy conservation and forces acting on the particle, particularly focusing on the radial direction. There are attempts to derive expressions for acceleration and reaction forces, with some questioning the signs and directions of forces involved.

Discussion Status

The discussion is ongoing, with participants clarifying their understanding of the equations and the physical setup. There is a recognition of differing interpretations regarding the signs of forces and accelerations, leading to confusion about the calculations. Some participants suggest revisiting the calculations based on the correct definitions of acceleration.

Contextual Notes

There is a noted difficulty in using standard notation for vectors, which may affect clarity. Participants are also grappling with the implications of their definitions of the unit vectors and the directions of forces in the context of the problem.

joker_900
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Homework Statement


OK this involves vectors but I can't use the normal notation on the internet so I'm using u^ to mean the unit vector along the vector u - i hope you can help me!

A particle of mass m is constrained to slide on the inside of a vertical smooth semi-circular ring of radius r. The position of the particle is described by a polar coordinate system whose origin is at the centre of the circle with axes along the orthogonal unit vectors r^ and b^ where b is the angle between the radius vector r and the vertical line that passes through the origin.

Assuming the particla is released from rest at the top of the semi-circle, use conservation of energy and Newton's Second Law in the r^ direction to calculate the reaction force exerted by the surface at b=60 degrees.


Homework Equations



The first part of this equation led to finding the formula for acceleration:

[/b]a[/b] = r*b''b^ - (v*v/r)r^ where b'' is the second derivative of the angle


The Attempt at a Solution



For conservation of energy I had

2grcosb = v*v, at b=60 => gr = v*v

And for Newton in the r^ direction I had

ma = mgcosb - R , at b=60 => ma = 0.5mg - R where R is the reaction force

From the equation for acceleration in the section above, I took the acceleration in the r^ direction to be

v*v/r and I substituted this into the equation above, and then substituted the energy conservation equation to get

R=1.5mg

However the given answer is 0.5mg - where have I gone wrong?!?
 
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joker_900 said:

Homework Statement


OK this involves vectors but I can't use the normal notation on the internet so I'm using u^ to mean the unit vector along the vector u - i hope you can help me!

A particle of mass m is constrained to slide on the inside of a vertical smooth semi-circular ring of radius r. The position of the particle is described by a polar coordinate system whose origin is at the centre of the circle with axes along the orthogonal unit vectors r^ and b^ where b is the angle between the radius vector r and the vertical line that passes through the origin.

Assuming the particla is released from rest at the top of the semi-circle, use conservation of energy and Newton's Second Law in the r^ direction to calculate the reaction force exerted by the surface at b=60 degrees.


Homework Equations



The first part of this equation led to finding the formula for acceleration:

[/b]a[/b] = r*b''b^ - (v*v/r)r^ where b'' is the second derivative of the angle


The Attempt at a Solution



For conservation of energy I had

2grcosb = v*v, at b=60 => gr = v*v

And for Newton in the r^ direction I had

ma = mgcosb - R , at b=60 => ma = 0.5mg - R where R is the reaction force

From the equation for acceleration in the section above, I took the acceleration in the r^ direction to be

v*v/r and I substituted this into the equation above, and then substituted the energy conservation equation to get

R=1.5mg

However the given answer is 0.5mg - where have I gone wrong?!?


The radial acceleration is toward the center of the circle so th eequation should be
ma = - mgcosb + R
 
kdv said:
The radial acceleration is toward the center of the circle so th eequation should be
ma = - mgcosb + R

I've defined r^ as going from the centre to the circumference though, so surely the mgcosb bit is positive as it acts outwards, and as R acts in the opposite direction it should be negative?
 
joker_900 said:
I've defined r^ as going from the centre to the circumference though, so surely the mgcosb bit is positive as it acts outwards, and as R acts in the opposite direction it should be negative?

Ok, but then your acceleration will be a_r = - v^2/R !
 
kdv said:
Ok, but then your acceleration will be a_r = - v^2/R !

Oh sorry (you mean v^2/r ?) I did do that but I mistyped it. I took the acceleration in the r^ direction as -v*v/r
 
joker_900 said:
Oh sorry (you mean v^2/r ?) I did do that but I mistyped it. I took the acceleration in the r^ direction as -v*v/r

Yes, I meant -v^2/r.

using a= +v^2/r as yopu had posted I got your final answer of 0.5 mg.
when I redid it with the correct acceleration of a=-v^2/r, I get the correct 1.5 mg.
You are saying that you got 0.5 mg using a=-v^2/r? I am confused. Please check your calculation.
 

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