the inclined plane
An inclined plane is just a flat surface tilted at an angle, a ramp. It is one of the oldest tools for moving heavy things: it is easier to push a barrel up a ramp than to lift it straight up. In physics it is the classic setting for practicing forces, because gravity, the normal force, and friction all come into play at once.
On a plane tilted at angle theta from the horizontal, the smart move is to choose axes along and across the slope, then split the weight m g into two components: one along the slope, m g sin(theta), pulling the object downhill, and one pressing into the slope, m g cos(theta). The normal force balances the perpendicular part, N = m g cos(theta). If the surface is frictionless, the object accelerates down the slope at a = g sin(theta); the steeper the slope, the larger sin(theta), and the faster the acceleration.
Add friction and it acts along the slope, opposing motion, with maximum static value mu_s times N = mu_s m g cos(theta). The object stays put as long as the downhill pull m g sin(theta) does not exceed this, which holds up to a critical angle where tan(theta) = mu_s. Beyond that angle it slides. Inclined planes teach you to resolve forces into components, the single most useful skill in mechanics.
A block on a 30 degree frictionless ramp accelerates down at a = g sin(30) = 9.8 times 0.5 = 4.9 m/s^2, while the normal force is N = m g cos(30), about 0.87 of its flat-ground value.
On a slope, only the along-slope part of gravity, m g sin(theta), drives the motion.
The normal force on a slope is m g cos(theta), NOT m g, a very common error. Always resolve weight into along-slope and perpendicular components before applying Newton's second law.