The
figure above shows a free body diagram for a snowboarder going down a
hill at an angle θ. The gravitational force points down and has a
magnitude of MG, where M=mass of the snowboarder and G=Gravity (9.81
m/s²). The force along the plane of the hill is given by mgsinθ
and the normal force is shown equal to mgcosθ. Friction is equal to the
coefficient of kinetic friction (uk) times the normal force, so in this
situation the force of friction would be: Fk=-ukmgcosθ (minus sign
meaning the force in the negative x-direction). So for the total force
in the x-direction we get:
1) mgsinθ-ukmgcosθ=ma