Gravity Components
Part of the Mechanics section of Coddy's Physics journey. Lesson 18 of 94.
On a ramp the weight mg splits into a part down along the slope and a part into the slope. The angle between mg and the part into the slope is the ramp angle θ:
F along = mg sin θ, F perpendicular = mg cos θ
The angle between mg and the part into the slope equals the ramp angle θ.
Nothing accelerates into the slope, so N = mg cos θ. On a 30° ramp a 10 kg box is pulled down the slope with 49 N, and N is about 84.9 N instead of 98 N.
Challenge
A 10 kg box slides down a frictionless 60° ramp. Find the normal force N the ramp pushes on it with.
Try it yourself
This lesson includes a short quiz. Start the lesson to answer it and track your progress.
All lessons in Mechanics
1Vectors and Newton's Laws
Right TrianglesWhat is a Vector?Adding VectorsAxes and DirectionsVector ComponentsForces Around UsFriction and TensionNewton's First LawNewton's Second LawNewton's Third LawRecap - Net Force2Friction
What is Friction?Static FrictionKinetic FrictionFriction and Newton's LawsRecap - Sliding Crate3Inclined Planes
Forces on an InclineGravity ComponentsFrictionless InclineIncline with FrictionWill It Slide?Recap - Ramp Challenge6Projectile Motion
Independent AxesHorizontal LaunchLaunch at an AngleRange and Max HeightRecap - Hit the Target9Work and Energy
WorkKinetic EnergyWork-Energy TheoremGravitational PEConservation of EnergyPowerRecap - Roller Coaster12Impulse and Momentum
MomentumImpulseConservation of MomentumElastic CollisionsInelastic CollisionsRecap - Air Track15Simple Harmonic Motion
What is SHM?Mass on a SpringThe PendulumSHM GraphsEnergy in SHMRecap - Oscillator