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Image for A 20 N horizontal force F pushes a block weighing 3.0 N against a vertical wall. The coefficient of static fri
A 20 N horizontal force F pushes a block weighing 3.0 N against a vertical wall. The coefficient of static friction between the wall and the block is 0.60, and the coefficient of kinetic friction is 0.40. Assume that the block is not moving initially.


In unit-vector notation, what is the force exerted on the block by the wall?
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Answer #1
Concepts and reason

The concepts used to solve this problem are frictional force, static equilibrium condition, vector algebra.

Draw the free body diagram of the system and apply the equilibrium condition to the force exerted by the wall.

Calculate the vertical and horizontal frictional force. After that calculate the total force exerted by wall on the block.

Fundamentals

The expression for weight (W)\left( W \right) of a body is:

W=mgW = mg

Here mm is the mass and gg is acceleration due to gravity.

Write the expression for frictional force (f)\left( f \right) .

f=μsFNf = {\mu _s}{F_N}

Here μs{\mu _s} is the coefficient of static friction and FN{F_N} is the normal reaction force acting on the body.

Write the expression for force in vector notation.

F=(Fx)neti^+(Fy)netj^F = {\left( {{F_{x}}} \right)_{net}}\hat i + {\left( {{F_y}} \right)_{net}}\hat j

Here, (Fx)net{\left( {{F_x}} \right)_{net}} is the net force acting on the body in x direction and (Fy)net{\left( {{F_y}} \right)_{net}} is the net force acting on the body in y direction.

Draw free body diagram of the system.

FN
>F = 20 N
mg =3 N

Here, ff is the frictional force between the wall and the block , mm is the mass of the block, FN{F_N} is the normal reaction force acting on the block and gg is the acceleration due to gravity.

From the free body diagram, the static equilibrium condition for vertical and horizontal forces.

The horizontal force is,

FFN=0F=FN\begin{array}{l}\\F - {F_N} = 0\\\\F = {F_N}\\\end{array}

Substitute 20N20{\rm{ N}} for FF .

FN=20N{F_N} = 20{\rm{ N}}

The vertical force is,

fW=0f=W\begin{array}{l}\\f - W = 0\\\\f = W\\\end{array}

Substitute 3N3{\rm{ N}} for WW .

f=3Nf = 3{\rm{ N}}

Write the expression for frictional force.

fs=μsFN{f_s} = {\mu _s}{F_N}

Here μs{\mu _s} is the coefficient of static friction.

Substitute 0.600.60 for μs{\mu _s} and 20N20{\rm{ N}} for FN{F_N} .

fs=(0.60)(20N)=12N\begin{array}{c}\\{f_s} = \left( {0.60} \right)\left( {20{\rm{ N}}} \right)\\\\ = 12{\rm{ N}}\\\end{array}

The frictional force ff acting on the object. Now if f<μsFNf < {\mu _s}{F_N} then the block will not slide and if f>μsFNf > {\mu _s}{F_N} the block will slide.

Here,

3N<12N3{\rm{ N < 12 N}}

Thus, the block does not move.

Write the expression for net force in the horizontal direction.

(Fx)net=FN{\left( {{F_x}} \right)_{net}} = - {F_N}

The negative sign is taken as FN{F_N} acts along the negative x axis.

Substitute 20 N for FN{F_N} .

(Fx)net=20N{\left( {{F_x}} \right)_{net}} = - 20{\rm{ N}}

Write the expression for net force in the vertical direction.

(Fy)net=f{\left( {{F_y}} \right)_{net}} = f

Substitute 3N3{\rm{ N}} for ff .

(Fy)net=3N{\left( {{F_y}} \right)_{net}} = 3{\rm{ N}}

Write the expression for the force exerted by the wall on the block in vector form.

F=(Fx)neti^+(Fy)netj^F = {\left( {{F_{x}}} \right)_{net}}\widehat i + {\left( {{F_y}} \right)_{net}}\widehat j

Substitute 20N - 20{\rm{ N}} for (Fx)net{\left( {{F_x}} \right)_{net}} and 3N3{\rm{ N}} for (Fy)net{\left( {{F_y}} \right)_{net}} .

F=20Ni^+3Nj^F = - 20{\rm{ N }}\widehat i + 3{\rm{ N }}\widehat j

Ans:

The force exerted by the wall on the block is F=20Ni^+3Nj^F = - 20{\rm{ N }}\widehat i + 3{\rm{ N }}\widehat j .

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