Balance the Ball

A ball is held up by a string, as shown in the figure above with the string tangent to the ball. If the angle between the string and the wall is θ \theta , what is the minimum coefficient of static friction between the ball and the wall, if the ball is not to fall?

csc θ \csc \theta cos θ \cos \theta tan θ \tan \theta sin θ \sin \theta

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2 solutions

Satvik Pandey
May 23, 2015

From the figure

As the ball is at rest so net force acting on it is zero.

T s i n θ = N Tsin\theta=N .................(1)

Net torque about CoM should be zero.

So T R = f s R TR=f_{s}R .....................................(2) Here 'R' is the radius of the ball.

As we have to find the minimum value of μ s \mu_{s} i.e limiting value of static friction. So

f s = μ s N f_{s}= \mu_{s}N .............(3)

On solving these equations we get μ s = c o s e c ( θ ) \mu_{s}=cosec(\theta) .

Perfect..!!

Rohit Gupta - 6 years ago

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Thank you sir! :)

satvik pandey - 6 years ago

Sir If we solve this using Forces balancing then we get μ = tan θ \mu = \tan{\theta} . So there will be 2 answers. Please explain ?

Rajdeep Dhingra - 6 years ago

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@Rajdeep Dhingra post your solution and then we will see where is the mistake as the answer must be unique.!!

Rohit Gupta - 6 years ago

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@Rohit Gupta Tcos(theta) *2R=mgR ......balancing moments about point of contact......

and substituting in eq. Tcos(theta) + f = mg.......

we finally obtain u = cot(theta)

Plz explain

Ravi Singh - 5 years, 11 months ago

How can you balance the forces without calculating the torques (as the ball cannot be considered a particle like object , i.e. the ball cannot be treated like a point mass). Pls post your solution.

Abhijeet Verma - 5 years, 11 months ago

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@Abhijeet Verma I treated it as a point mass. Sorry for the trouble.

Rajdeep Dhingra - 5 years, 11 months ago

Sir I agree with @Rajdeep Dhingra and would be pleased if you take out some time and clear our doubt...thanking you!!

Mridul Chaturvedi - 6 years ago

I got that wrong.....oh....but thanks a neat solution.....

ashutosh mahapatra - 6 years ago
Jason Zou
Jun 29, 2015

The ball is at rest, so τ N e t = 0 \tau_{Net}=0 . From this, we have F T = F f r F_T=F_{fr} .

We also see that the horizontal forces must balance, so F T sin θ = F N F_T\sin\theta=F_N . Thus, F f r = μ F T sin θ F_{fr}=\mu F_T\sin\theta

From the equation F T = F f r F_T=F_{fr} , we have F T = μ F T sin θ F_T=\mu F_T\sin\theta . Simplifying, we have μ = 1 sin θ = csc θ \mu=\frac {1}{\sin\theta}=\csc\theta

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