h2. Part A
!normalbox1.png|width=40%!
A 10 kg box slides at a constant speed of 2 m/s along a smooth floor. What is the magnitude of the normal force exerted on the box by the floor?
h4. Solution
*System:* Box as [point particle] subject to external .
*Interactions:* External influences from the earth (gravity) and the floor (normal force).
*Model:* [Point Particle Dynamics].
*Approach:* We begin with a free body diagram for the box:
!normalfbd1.png!
From the free body diagram, we can write the equations of [Newton's 2nd Law|Newton's Second Law]. We ignore the x-direction, since there are no forces acting.
{latex}\begin{large}\[ \sum F_{y} = N - mg = ma_{y}\]\end{large}{latex}
Because the box is sliding over level ground, it is not moving at all in the _y_ direction. Thus, it certainly has no y-acceleration. Setting _a_~y~ = 0 in the above equation gives:
{latex}\begin{large}\[ N = mg = \mbox{98 N}\]\end{large}{latex}
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h2. Part B
!normalbox2.png|width=40%!
A person pushes a 10 kg box along a smooth floor by applying a perfectly horizontal force of 20 N. The box accelerates horizontally at 2 m/s{color:black}^2^{color}. What is the magnitude of the normal force exerted on the box by the floor?
h4. Solution
*System:* Box as [point particle] subject to external.
*Interactions:* External influences from the earth (gravity), the floor (normal force) and the person (applied force).
*Model:* [Point Particle Dynamics].
*Approach:* We begin with a free body diagram for the box:
!normalfbd2.png!
From the free body diagram, we can write the equations of [Newton's 2nd Law|Newton's Second Law].
{latex}\begin{large}\[ \sum F_{x} = F_{A} = ma_{x} \]
\[ \sum F_{y} = N - mg = ma_{y}\]\end{large}{latex}
Because the box is sliding over level ground, it is not moving at all in the _y_ direction. Thus, it certainly has no y-acceleration. Setting _a_~y~ = 0 in the _y_ direction equation gives:
{latex}\begin{large}\[ N = mg = \mbox{98 N}\]\end{large}{latex}
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h2. Part C
!normalbox3.png|width=40%!
A person is trying to lift a 10 kg box by applying a perfectly vertical force of 20 N with the help of a pulley. What is the magnitude of the normal force exerted on the box by the floor?
h4. Solution
*System:* Box as [point particle] subject to.
*Interactions:* external influences from the earth (gravity), the floor (normal force) and the rope (tension).
*Model:* [Point Particle Dynamics].
*Approach:* We begin with a free body diagram for the box:
!normalfbd3.png!
From the free body diagram, we can write the equations of [Newton's 2nd Law|Newton's Second Law]. We ignore the x-direction, since there are no forces acting.
{latex}\begin{large}\[ \sum F_{y} = T + N - mg = ma_{y}\]\end{large}{latex}
Because the box is sliding over level ground, it is not moving at all in the _y_ direction. Thus, it certainly has no y-acceleration. Setting _a_~y~ = 0 in the _y_ direction equation gives:
{latex}\begin{large}\[ T + N - mg = 0 \]\end{large}{latex}
Solving for the normal force gives:
{latex}\begin{large}\[ N = mg - T = \mbox{78 N}\]\end{large}{latex}
{tip}When three or more forces act in a direction with zero acceleration, it is always a good idea to check your answer by putting the numbers on the free body diagram and making sure that they balance. In this case, T (20 N) and N (78 N) act to balance mg (98 N).{tip}
{note}Follow up question: The floor no longer supports the entire weight of the box (98 N) because the rope is carrying some of the weight (20 N). How will the _person's_ normal force be affected in this situation? If the floor is carrying so much less weight, what part of the building is now feeling an extra load?{note}
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h2. Part D
!normalbox4.png|width=40%!
A person pushes a 10 kg box along a smooth floor by applying force of 20 N. The force is applied at 30° below the horizontal. What is the magnitude of the normal force exerted on the box by the floor?
h4. Solution
*System:* Box as [point particle] subject to external.
*Interactions:* External influences from the earth (gravity), the floor (normal force) and the person (applied force).
*Model:* [Point Particle Dynamics].
*Approach:* We begin with a free body diagram for the box:
!normalfbd4.png!
From the free body diagram, we can write the equations of [Newton's 2nd Law|Newton's Second Law].
{latex}\begin{large}\[\sum F_{x} = F_{A}\cos\theta = ma_{x}\]
\[ \sum F_{y} = N - mg - F_{A}\sin\theta = ma_{y}\]\end{large}{latex}
Because the box is sliding over level ground, it is not moving at all in the _y_ direction. Thus, it certainly has no y-acceleration. Setting _a_~y~ = 0 in the _y_ direction equation gives:
{latex}\begin{large}\[ N - mg -F_{A}\sin\theta = 0 \]\end{large}{latex}
Solving for the normal force gives:
{latex}\begin{large}\[ N = mg + F_{A}\sin\theta = \mbox{108 N}\]\end{large}{latex}
{tip}Again, we can check the force balance in the _y_ direction. In this case _mg_ (98 N) and _F_~A,y~ (10 N) act to balance N (108 N).{tip}
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