
The normal force is the contact force exerted by a surface on an object in contact with it.
The word “normal” means:
perpendicular to the surface
Thus, the normal force always acts perpendicular to the surface of contact.
The normal force is commonly written as:
\(\vec{N}\)
It is a vector quantity.
When an object presses against a surface:
This restoring contact force is the normal force.
The normal force:
Examples:
Normal force points vertically upward.
Normal force points perpendicular to the slope.
A common misconception is:
\(N=mg\)
This is only true in specific situations.
The normal force depends on:
For an object at rest on a flat surface:
Vertical forces:
Since vertical acceleration is zero:
\(\Sigma{F_y}=0\)
Thus:
\(N=mg\)
For an incline at angle θ\thetaθ:
Weight has components:
The perpendicular component is:
\(mg\cos\theta\)
Since acceleration perpendicular to the plane is zero:
\(N=mg\cos\theta\)
The normal force becomes smaller as the incline angle increases.
If an elevator accelerates upward:
\(N-mg=ma\)
Then:
\(N=mg+ma\)
The normal force increases.
If accelerating downward:
\(N=mg-ma\)
The normal force decreases.
In free-body diagrams:
Friction depends on the normal force.
For kinetic friction:
\(f_k=\mu_kN\)
For static friction:
\(f_s\le\mu_sN\)
Larger normal force generally produces larger frictional force.
The normal force is a reaction force from a surface.
It exists only when surfaces are in contact.
If contact disappears:
\(N=0\)
Example:
The normal force:
\(\vec{N}\)
Important relationships:
Horizontal surface:
\(N=mg\)
Inclined plane:
\(N=mg\cos\theta\)
Key ideas:
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