Problem 1.136 from Irodov's book

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Homework Help Overview

The discussion revolves around a problem from Irodov's book concerning the motion of a particle along a trajectory, specifically focusing on the conditions under which the particle breaks off from a groove and its subsequent velocity. The subject area includes concepts from mechanics, energy conservation, and projectile motion.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the assumptions regarding the particle's motion, questioning whether it maintains contact with the trajectory throughout its path. There is also discussion on the implications of starting from rest and the relevance of kinetic energy at different points in the motion. The necessity of considering horizontal components of velocity is debated, particularly in relation to the problem's requirements.

Discussion Status

The conversation is active, with participants clarifying their understanding of the equations involved and the conditions at the point of breaking off from the groove. Some guidance has been provided regarding the treatment of horizontal and vertical components of motion, but there remains a lack of consensus on specific values and interpretations of the velocity at different points.

Contextual Notes

Participants note that the problem does not specify certain initial conditions, such as whether the body starts rolling from rest, which may affect the analysis. There is also mention of differing interpretations of the velocity values provided in the book and the solution link shared.

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Hello

I am attaching a problem from Irodov's book "Problems in general physics". There is also a website where the solutions are given. I am just trying to understand the solution. Solution is given at http://irodovsolutionsmechanics.blogspot.com/2008_05_03_archive.html

Now in the problem I assumed that the particle keeps in touch with the trajectory for all the half circle. I think its a wrong assumption. Also the problem doesn't mention if the body starts rolling from the rest. does it matter ? In the solution given I have not understood how he got equation 1. If we use conservation of energy , then we will need to take care of the kinetic energy at the bottom. He doesn't use that kinetic energy at all. Also the problem just asks for the velocity of the body after breaking off the groove but this guy calculates the horizontal component of the velocity. Even at the back of the book, the horizontal component of the velocity is given. can somebody clarify ?

Issac N
 

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  • 1.136.jpg
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The body does break off the groove. It has to have a certain minimum velocity at the base to complete a circle. Assuming a complete circle is incorrect.
The eqn.1 does use k.e at the bottom but that is also equal to g.p.e at the top of the hill.
They also have mentioned zero velocity at the top - look what they say-"starts sliding".
And they use the horizontal velocity because they are originally asking for velocity at the highest point of trajectory.
 
ok the equation 1 now makes sense. but why do we need to take horizontal component
of the velocity. that's the answer at the end of the book too. at the time of breaking from the groove, v = sqrt(gh/3) but the book gives v= (2/3) sqrt(gh/3)... as given in the above solution.

Issac n
 
IssacNewton said:
but why do we need to take horizontal component
of the velocity.
Because at the highest point of the trajectory the vertical component will be zero.
at the time of breaking from the groove, v = sqrt(gh/3)
How did you derive that?
 
IssacNewton said:
ok the equation 1 now makes sense. but why do we need to take horizontal component
of the velocity. that's the answer at the end of the book too. at the time of breaking from the groove, v = sqrt(gh/3) but the book gives v= (2/3) sqrt(gh/3)... as given in the above solution.

Issac n
In the solution of problem, they have found the velocity of the ball in the position where the line joining the ball and the center makes an angle θ with the horizontal.
In your attachment, the velocity at the highest point of the semicircle is asked.
 
Doc Al said:
Because at the highest point of the trajectory the vertical component will be zero.

How did you derive that?

Doc Al

if you see the solution provided at the link, when the object breaks off the groove, the normal reaction N becomes zero .so plugging N=0 in eq. 2 we can solve for sin(theta). also the problem asks to find the velocity at the highest point of the trajectory of the object, not the highest point of the half-circle. please see the solution link given by me. i didn't understand the last part where he says v= (2/3) sqrt(gh/3)

Issac N
 
IssacNewton said:
Doc Al

if you see the solution provided at the link, when the object breaks off the groove, the normal reaction N becomes zero .so plugging N=0 in eq. 2 we can solve for sin(theta). also the problem asks to find the velocity at the highest point of the trajectory of the object, not the highest point of the half-circle. please see the solution link given by me.
My bad. I misread what you wrote.

i didn't understand the last part where he says v= (2/3) sqrt(gh/3)
You have the velocity at the break point. Find its horizontal component. That won't change as the object reaches its highest point.

Once the object leaves the surface, it's a free projectile under gravity. For a projectile, treat horizontal and vertical motion separately. Only the vertical speed changes as the object rises; the horizontal speed is constant. At the top, the vertical component is zero.
 
Last edited:
Will you please post the full text of the problem?
 
rl.bhat said:
Will you please post the full text of the problem?
See the attachment in post #1.
 
  • #10
Doc Al said:
See the attachment in post #1.
OK. Got it.
 
  • #11
Doc Al said:
My bad. I misread what you wrote.


You have the velocity at the break point. Find its horizontal component. That won't change as the object reaches its highest point.

Once the object leaves the surface, it's a free projectile under gravity. For a projectile, treat horizontal and vertical motion separately. Only the vertical speed changes as the object rises; the horizontal speed is constant. At the top, the vertical component is zero.

thanks... makes sense now
 

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