Why Is Sin(theta) Squared in This Mechanical Engineering Problem?

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Homework Help Overview

The discussion revolves around a mechanical engineering problem involving the dynamics of a particle on a wedge, specifically focusing on the appearance of sin(theta) squared in a derived equation. Participants are exploring the underlying physics and mathematical relationships involved in the problem.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants are attempting to understand the derivation of the equation and the role of sin(theta) squared. They are discussing the forces acting on the particle and the wedge, including references to free body diagrams (FBD) and the implications of frictionless surfaces.

Discussion Status

The discussion is ongoing, with participants sharing their understanding and asking clarifying questions. Some guidance has been offered regarding the forces involved, but there is no explicit consensus on the role of sin(theta) squared yet.

Contextual Notes

Participants have noted the need for a clear understanding of the forces acting on the system, particularly in relation to the acceleration of the wedge and the normal reaction forces. There is an emphasis on the assumptions made in the problem setup, such as the frictionless nature of the surfaces.

Turborrado
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Hi! New to this forum and signed up because I've just started a foundation degree in mechanical engineering, and having been out of education for a very long time beforehand, getting back to grips with mathematics and the like!

Anyway, I would like to ask for some advice on this problem, I know how the top part of the fraction come about, as well as the lower case and upper case m in the lower part of the fraction, but still unsure as to why sin(theta) is squared? Thanks in advance!

IMAG0404.jpg
 

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We need to work the whole solution out to tell where does that ##\sin^2 \theta## came from.
So a better way would be that you let us, how you worked out the question and we try to solve your confusion.
 
Hi and thanks for your reply, I have got as far as identifying that the equation shown for a1 is a rearranged F=ma, to a=F/m , the F being mgsin0cos0 and the m being m the lower part of the fraction.

I know m is the mass of the particle on the wedge and M is the mass of the wedge but fail to see how sin0^2 fits in, I would imagine it would be to so with calculating the mass.
 
Turborrado said:
Hi and thanks for your reply, I have got as far as identifying that the equation shown for a1 is a rearranged F=ma, to a=F/m , the F being mgsin0cos0 and the m being m the lower part of the fraction.

I know m is the mass of the particle on the wedge and M is the mass of the wedge but fail to see how sin0^2 fits in, I would imagine it would be to so with calculating the mass.
Did you draw a FBD ?
 
Buffu said:
Did you draw a FBD ?

Here is what I drew, and how far I got. As I understand the surfaces are frictionless so the round particle will fall straight down and the wedge will move to the right.
 

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Turborrado said:
Here is what I drew, and how far I got. As I understand the surfaces are frictionless so the round particle will fall straight down and the wedge will move to the right.
Normal reaction of sphere on the block is not ##mg\cos\theta##, It is so because the big block is accelerating.

Equate the forces perpendicular to the incline acting on the sphere, from there you will get the correct value of normal reaction. Substitute it in your last equation and you will get the answer.
 
Turborrado said:
Here is what I drew
Is a2 relative to the ground or relative to the wedge?
 

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