The normal force is always perpendicular to the surface upon which the object is moving, and is pointed away from said surface. That means we are looking for the value for Z in the diagram.

Observe that Z and Y are equal, but opposite forces.

If we can solve for Y, then we can find Z.

We can use our understanding of trigonometry to find an equation for Y.

If we plug in  for the angle, we see:

Since we are solving for Y, we can multiply both sides by W.

Now that we know an equation for Y, we can return to our original equation to solve for Z.

From here, we can use Newton's second law to find the value of W, the total force of gravity.

Substitute this into our equation for Z.

Now we can solve for Z using the values given in the question for the angle, mass, and gravity.

For this problem use Newton's second law:

We are given the total force and the mass, allowing us to solve for the acceleration.

Force is a vector quantity, meaning that both magnitude and direction are important factors. Net force is calculated by summing all of the forces acting on an object.

For this question, we will assign "to the right" as the positive direction and "to the left" as the negative direction. Under these conditions, we can add the given forces to find the net force.

This means that it has a net force of  to the left.

The force due to friction will always be parallel to the surface upon which the object is traveling. It will come directly from the center of the object, and be pointed in the opposite direction to the motion of the object.

In this diagram, V is pointed parallel to the surface and opposite to the direction of motion.

Remember, in a force diagram, forces come from the center of the object. The force of gravity will always be straight down from the center of the object.

In this diagram, W is pointed directly downward.

When working in an inclined plane, when we break our force due to gravity into components, the angle at the top that triangle will be equal to the angle of the inclined plane.

In the diagram, the total force due to gravity is given by W. X represents the horizontal component, and is parallel to the surface of the plane. Y represents the vertical component, and is perpendicular to the surface of the plane. X and Y thus create a right angle, with W as the hypotenuse. By turning this triangle such that the right angle aligns with the right angle of the inclined plane (between Q and P), we can see that W aligns with the incline surface and Y aligns with the base, P. Based on these alignments, the angle between W and Y must be equal to the angle between the surface and P; thus, .

The normal force is always perpendicular to the surface on which the object is placed, and is pointed away from said surface.

In this diagram, Z is the only force that is perpendicular to the surface and in the upward direction. This force must counteract the vertical force of gravity, which will be perpendicular to the surface in the downward direction (Y).

In this diagram, V represents the force due to friction. The equation for the force due to friction is , where is the coefficient of friction.

In this case, Z represents the normal force. We can re-write the equation for friction:

Z can be re-written in terms of the angle, but will always need to be multiplied by the coefficient of friction in order to give an equation for V.

The other equations are true.

- X and Y form a right angle, so the Pythagorean theorem applies.

- Z is the normal force, which is, by definition, equal and opposite the vertical force of gravity.

- W is the total force of gravity, which will be equal to the mass times the acceleration of gravity.

- the triangle formed by W, X, and Y is similar to the triangle formed by the surface, Q, and P, meaning that these angles must be equal.

In this problem, Y and Z are equal, but opposite forces, and Z is our normal force.

If we can solve for Y, then we can find Z.

We can use our understanding of trigonometry to find an equation for Y.

If we plug in  for the angle, we see:

Since we are solving for Y, we can multiply both sides by W.

Now that we know an equation for Y, we can return to our original equation to solve for Z.

There is no way for us to know the distance the object travels. Even though the force diagram places our object roughly halfway up the plane, we do not know the position where the object starts or where the object ends. We cannot calculate a change in distance.