Frictional Forces Physics 1 Problem

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Homework Help Overview

The problem involves a crate on an inclined ramp, requiring analysis of forces including friction, tension, and weight. The context is within the subject area of mechanics, specifically dealing with frictional forces and equilibrium conditions.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • Participants discuss mapping forces in the x and y directions and the importance of free-body diagrams. There is an exploration of the relationship between tension in the rope and the weight of the mass on the other end. Questions arise regarding the equality of tension despite different angles and the implications of the setup.

Discussion Status

The discussion is ongoing, with participants seeking clarification on their approaches and reasoning. Some guidance has been offered regarding the need for multiple free-body diagrams and the importance of algebraic manipulation before substituting values. There is no explicit consensus yet on the correctness of the initial attempts.

Contextual Notes

Participants are working within the constraints of a homework problem, which may limit the information available and the assumptions that can be made. The discussion reflects uncertainty about the setup and the relationships between forces involved.

Almost935
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Homework Statement



7.) A 1520-N crate is to be held in place on a ramp that rises at 30.0° above the horizontal (see figure). The massless rope attached to the crate makes a 22.0° angle above the surface of the ramp. The coefficients of friction between the crate and the surface of the ramp are µk = 0.450 and μs = 0.650. The pulley has no appreciable mass or friction. What is the MAXIMUM weight w that can be used to hold this crate stationary on the ramp?

Picture of problem:
attachment.php?attachmentid=67399&stc=1&d=1394245127.png


Homework Equations



Fs = μsFn

F = ma

The Attempt at a Solution



I attempted by first mapping out the forces for Fx and Fy. I then solved for the normal force in order to replace it in the static friction force equation so as to be able to solve for the tension in the rope which I then found to be 1380 N. I am unsure whether this is the answer. Logically it somewhat makes sense that the tension in the rope must be equal to the weight of the mass on the other end to be completely still. Looking for some analysis of my answer and some pointers in the correct direction
 

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Almost935 said:
I attempted by first mapping out the forces for Fx and Fy.
Guessing that you placed the axes to that +x direction points "up along the ramp"?

I then solved for the normal force in order to replace it in the static friction force equation so as to be able to solve for the tension in the rope which I then found to be 1380 N. I am unsure whether this is the answer. Logically it somewhat makes sense that the tension in the rope must be equal to the weight of the mass on the other end to be completely still.
Best practice is to do all the algebra before you put numbers in - it can avoid the sort of confusion you ended up in.

Looking for some analysis of my answer and some pointers in the correct direction
You need two free-body diagrams to be sure to get this answer correct, one for the mass on the slope - which you have basically done, and the other for the hanging mass.

This gives you two equations - which is good, because you have two unknowns: the tension in the rope and the weight that hangs off the pulley.

So repeat the process for the hanging mass and see if you are right.
 
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So you are saying that the Tension is equal throughout despite the angle on the first mass?
 
The tension points along the rope doesn't it? Why would the rope care about what angle stuff is attached to it?
 

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