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Study Guide - Smart Notes
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Forces on an Inclined Plane
Analyzing Contact Forces on an Inclined Ramp
When an object of mass M rests on an inclined plane at angle θ, it experiences several forces. Understanding these forces is essential for solving problems involving equilibrium and friction.
Normal Force (FN): The force perpendicular to the surface, balancing the component of gravity normal to the plane.
Friction Force (Ff): The force parallel to the surface, opposing motion or potential motion.
Gravitational Force (Fg): Acts vertically downward, with components both parallel and perpendicular to the plane.
Equilibrium Conditions:
Sum of forces in the x-direction (parallel to the plane):
Sum of forces in the y-direction (perpendicular to the plane):
At rest: ,
Solving for Forces:
Normal force:
Friction force (if at rest):
If friction is limiting:
Direction and Magnitude:
The contact force from the ramp is the vector sum of normal and friction forces.
Magnitude:
Direction: , where is the angle from the normal.
Example: For , kg, m/s2:
N
N
Forces on a Sled: Friction and Pulling Force
Pulling a Sled at Constant Velocity
When pulling a sled across a horizontal surface at constant velocity, the applied force must balance the kinetic friction force.
Applied Force (Fpx): The horizontal force exerted by the rope.
Kinetic Friction Force (Fkf):
Normal Force (FN): (if the rope is horizontal)
Equilibrium Conditions:
Sum of forces in x-direction:
At constant velocity:
Solving for Applied Force:
Example: For kg, , m/s2:
N
Drag Forces and Terminal Velocity
Pressure Drag on Large Objects
For large objects moving through non-viscous fluids, pressure drag is the dominant resistive force. It acts opposite to the direction of motion.
Pressure Drag Force:
Cd: Drag coefficient (dimensionless)
ρ: Fluid density
A: Cross-sectional area
v: Velocity of the object
Terminal Velocity of a Skydiver
When a skydiver falls, they accelerate until the drag force equals their weight, reaching terminal velocity (vt).
Free Body Diagram: Forces are gravity (down) and drag (up).
Equilibrium at Terminal Velocity:
Solving for Terminal Velocity:
Example: For kg, , kg/m3, m2:
m/s
Skydiver Descent and Parachute Deployment
After reaching terminal velocity, a skydiver opens their parachute, increasing the cross-sectional area and drag coefficient, which rapidly decreases their velocity.
New Drag Force: If drag increases by a factor of 5,
Net Force at Deployment:
Example: If , then , so (upward acceleration).
Summary Table: Forces in Different Scenarios
Scenario | Key Forces | Equilibrium Condition | Formula for Required Force |
|---|---|---|---|
Inclined Plane (at rest) | Normal, Friction, Gravity | , | |
Sled (constant velocity) | Applied, Kinetic Friction, Gravity, Normal | ||
Skydiver (terminal velocity) | Gravity, Drag |
Additional info: The FANCL checklist referenced in the notes stands for Free body diagram, Axes, Newton's laws, Components, and Links to equations. This systematic approach helps organize force analysis in physics problems.