The key to analyzing this system successfully is to choose the correct orientation for the

and

axes. If you choose axes parallel and perpendicular to the plane, the analysis is (relatively) easy. You can use the conventional horizontal and vertical orientation, but be prepared for more difficult trigonometry!

Resolving

into

and

components is the next step; the components (parallel and perpendicular to the plane) are also shown.

Physically, the block can only move parallel to the plane—assuming the plane is smooth and straight means the block is never going to jump off the surface of the plane and is confined to sliding along the surface. This means that the speed and net force in the

direction, that is, perpendicular to the plane, must be zero.

Assuming that the plane is "frictionless" means that the plane does not exert any force on the block that is parallel to the surface. Therefore, any force exerted by the plane on the block must be perpendicular to the surface. This is the reason for the name "normal" force: it is always oriented "normal", or perpendicular, to the surface of the plane.

In order to have no net force on the block perpendicular to the plane, the "normal" force exerted by the plane and the

component of

must cancel exactly, leaving no net force on the block in the

direction. As a result, the

component of

is the only remaining, or net, force. Thus, expected, the net force is pointing parallel to the plane, and in fact, down the plane.

Mathematically, the angle of the plane

and the diagonal distance

from the starting point to the bottom determines

, the acceleration (or rate of change of the speed) from Newton's second law:

or

This finds the time

to reach the bottom from the relationship between distance and time for constant acceleration:

, or

. This is the final speed

at the bottom (or at any time

), assuming that the block starts from rest

, from the definition of acceleration:

, or

, and, substituting for

and

from above,

.

This result for

is much easier to get from the principle of conservation of energy (which holds because the motion is frictionless):

The kinetic energy at the bottom equals the gravitational field (potential) energy at the starting point, or

, where

is the vertical height of the block above the bottom of the plane before the block starts moving.

From the blue triangle,

, so

. Substituting this into the equation above and canceling

yields

.

Solving,

, which is the same as the result above.