Dynamics and Friction: Solving for Maximum Angle on a Ramp with μ_{s}=0.25

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Homework Help Overview

The problem involves determining the maximum angle θ at which a box can rest on a ramp without slipping, given a static friction coefficient μ_{s}=0.25. The context is within the subject area of dynamics and friction.

Discussion Character

  • Exploratory, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to analyze the forces acting on the box using a free body diagram and applies Newton's second law. Some participants question whether the box is accelerating at the point of slipping, leading to a discussion about setting the net force to zero.

Discussion Status

Participants are exploring the relationship between the forces acting on the box and the conditions for slipping. There is a suggestion that the static friction condition leads to a relationship involving the tangent of the angle, and some guidance has been provided regarding the significance of units and significant figures.

Contextual Notes

There is an implicit assumption that the box is on the verge of slipping, and the discussion reflects on the conditions under which this occurs. The original poster's approach and subsequent confirmations indicate a focus on the theoretical understanding of the problem rather than a definitive solution.

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Homework Statement



A box is halfway up a ramp. The ramp makes an angle, θ with the ground. What is the maximum value of θ before the mass will slip? μ[itex]_{s}[/itex]=0.25

Homework Equations



F[itex]_{x}[/itex]=ma[itex]_{x}[/itex]

The Attempt at a Solution


I drew a free body diagram to show the forces affecting the box

η-mgcos=0
η=mgcosθ (eq'n 1)


F[itex]_{x}[/itex]=ma[itex]_{x}[/itex]
μ[itex]_{s}[/itex]η-mgsinθ=ma[itex]_{x}[/itex] (sub eq'n 1 in)
μ[itex]_{s}[/itex](mgcosθ)-mgsinθ=ma[itex]_{x}[/itex]
mg(μ[itex]_{s}[/itex]cosθ-sinθ)=ma[itex]_{x}[/itex]


I'm not sure where to go from here, or even if this is the correct path for me to take
 
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You have correctly identified the forces acting, but just as the box is on the verge of slipping, is it accelerating?
 
the box wouldn't be accelerating, so would it be

mg(μ[itex]_{s}[/itex]cosθ-sinθ)=0
mgμ[itex]_{s}[/itex]cosθ=mgsinθ
μ[itex]_{s}[/itex]cosθ=sinθ
μ[itex]_{s}[/itex]=tanθ
θ=14.036
 
hsphysics2 said:
the box wouldn't be accelerating, so would it be

mg(μ[itex]_{s}[/itex]cosθ-sinθ)=0
mgμ[itex]_{s}[/itex]cosθ=mgsinθ
μ[itex]_{s}[/itex]cosθ=sinθ
μ[itex]_{s}[/itex]=tanθ
θ=14.036
Yes, good, in degrees (don't forget units), but you should round your answer to 14 degrees ( 2 significant figures).
 

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