Question #39297

1)an object is placed on the surface of a smooth inclined plane of inclination θ.it takes time t to reach the bottom. if the same object is allowed to slide down inclined plane on inclination θ,it takes time nt to reach the bottom where n is a number greater than 1. what is coefficient?
2)The force required to just move a body up the inclined plane is doublethe force required to justprevent the body from sliding down the plane.the coefficient of friction is μ.find the inclination θ of the plane
3)a particle inside a hollow sphere of radius r, having coeffient of friction(1/√3), upto what height can particle be at rest?

Expert's answer

Answer on Question #39297, Physics - Mechanics | Kinematics | Dynamics

Question:

1) An object is placed on the surface of a smooth inclined plane of inclination θ\theta. It takes time tt to reach the bottom. If the same object is allowed to slide down inclined plane on inclination θ\theta, it takes time ntnt to reach the bottom where nn is a number greater than 1. What is coefficient?

2) The force required to just move a body up the inclined plane is double the force required to just prevent the body from sliding down the plane. The coefficient of friction is μ\mu. Find the inclination θ\theta of the plane

3) A particle inside a hollow sphere of radius rr, having coefficient of friction(1/V3), up to what height can particle be at rest?

Answer:

1) The first question is confusing, so we assume that objects are placed on the same height hh and the second included plane has the inclination θ1\theta_{1}. Let us consider the first case. Objects has the acceleration a=gsinθa = g \sin \theta and moves on the distance =htanθ\ell = h \tan \theta. So,


=at22=gsinθt22t=2hgcosθ.\ell = \frac{a t^{2}}{2} = \frac{g \sin \theta t^{2}}{2} \Rightarrow t = \sqrt{\frac{2 h}{g \cos \theta}}.


In the same way one can obtain


nt=2hgcosθ1.n t = \sqrt{\frac{2 h}{g \cos \theta_{1}}}.


Whence


ntt=2hgcosθ1/2hgcosθn=cosθcosθ1.\frac{n t}{t} = \sqrt{\frac{2 h}{g \cos \theta_{1}}} \Bigg/ \sqrt{\frac{2 h}{g \cos \theta}} \Rightarrow n = \sqrt{\frac{\cos \theta}{\cos \theta_{1}}}.


2) The friction force is


Ff=μmgcosθ.F_{f} = \mu m g \cos \theta.


The force required to move a body up equals


F1=μmgsinθ+Ff.F _ {1} = \mu m g \sin \theta + F _ {f}.


The force required to prevent a body from sliding down equals


F2=μmgsinθFf.F _ {2} = \mu m g \sin \theta - F _ {f}.


By conditions,


F1F2=2=μmgsinθ+μmgcosθμmgsinθμmgcosθ\frac {F _ {1}}{F _ {2}} = 2 = \frac {\mu m g \sin \theta + \mu m g \cos \theta}{\mu m g \sin \theta - \mu m g \cos \theta}sinθ=3cosθθ=arctan3.\sin \theta = 3 \cos \theta \Rightarrow \theta = \arctan 3.


3) The friction force equals


Ff=μmgcosθ,F _ {f} = \mu m g \cos \theta,


where μ=1/3\mu = 1 / \sqrt{3}, cosθ=rhr\cos \theta = \frac{r - h}{r}, hh is a height needs to be found. The friction force prevents a particle to slide down under the action of the component of the gravitational force


F1=mgsinθ.F _ {1} = m g \sin \theta.


So,


Ff=F1μmgcosθ=mgsinθF _ {f} = F _ {1} \Rightarrow \mu m g \cos \theta = m g \sin \thetatanθ=μθ=30.\tan \theta = \mu \Rightarrow \theta = 30{}^{\circ}.cosθ=32=rhrh=232r.\cos \theta = \frac {\sqrt {3}}{2} = \frac {r - h}{r} \Rightarrow h = \frac {2 - \sqrt {3}}{2} r.

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