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A block of mass m rests on an inclined plane. The coefficient of static friction between the block and the plane is μs. A gradually increasing force is pulling down on the spring (force constant k). Find the potential energy U of the spring (in terms of the given symbols) at the moment the block begins to move. (Use any variable or symbol stated above along with the following as necessary: g and θ.)

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Answer:

Potential energy is


U=(1)/(2k)(mg(\mu_(s)\,cos\theta+sin\theta))^(2)\\

Step-by-step explanation:

Given situation is shown in figure 1

In order to calculate the potential energy at the moment block started moving we first have to calculate the net force acting on the block. For this consider figure 2

Forces acting in vertical direction:

Normal force Fn acting on block is in upward direction which is balanced by horizontal component of weight of block acting in opposite direction.


F_(n)= mg\,cos \theta---(1)\\

Forces acting in horizontal direction:

Tension in string is equal and opposite to frictional force and and vertical component of weight as show in figure 2


T=F_(f)+mg\,sin\theta----(2)

Frictional force is:


F_(f)=\mu_(s)F_(n)---(3)

From (1)


F_(f)=\mu_(s)mg\,cos\theta

(2) becomes then


T=\mu_(s)mg\,cos\theta+mg\,sin\theta----(2)

If spring is not accelerating then tension in rope must be equal spring force i.e


T=kx---(4)

Then (2) becomes


kx=\mu_(s)mg\,cos\theta+mg\,sin\theta


x=(mg(\mu_(s)\,cos\theta+sin\theta))/(k)

Potential energy is given as


U=(1)/(2)kx^(2)\\\\U=(1)/(2)k((mg(\mu_(s)\,cos\theta+sin\theta))/(k))^(2)\\\\U=(1)/(2k)(mg(\mu_(s)\,cos\theta+sin\theta))^(2)\\

A block of mass m rests on an inclined plane. The coefficient of static friction between-example-1
A block of mass m rests on an inclined plane. The coefficient of static friction between-example-2
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