By Fatskills Exam Guides Team — the exam nerds behind 28,500+ quizzes and 2.1M practice questions across 500+ global exams.
Tension, normal force, and spring force are contact forces that appear in almost every AP Physics problem involving objects at rest or in motion. These forces explain how ropes pull, surfaces push, and springs stretch or compress. Mastering them is essential for free-body diagrams (FBDs), Newton’s laws, and equilibrium problems—all high-frequency AP exam topics. Real-world example: When you stand on a bathroom scale, the normal force from the scale balances your weight, giving your "weight" reading. If you pull a rubber band, Hooke’s Law explains why it snaps back.
Example: For a block on a ramp, include weight (mg), normal force (N), friction (f), and tension (T) if a rope is attached.
Choose a Coordinate System:
For springs, let +x be the direction of stretch/compression.
Resolve Forces into Components:
Break forces into x and y components if needed (e.g., weight on a ramp: mg sin? and mg cos?).
Apply Newton’s Laws:
Accelerating (?F = ma): Set sum of forces equal to mass × acceleration.
Solve for Unknowns:
For springs, remember F? = -kx (the negative sign is crucial for direction!).
Check Units and Reasonableness:
Mistake: Assuming normal force always equals weight. Correction: Normal force equals weight only on flat surfaces with no vertical acceleration. On ramps or in elevators, N-mg. Example: On a 30° ramp, N = mg cos?.
Mistake: Ignoring the negative sign in Hooke’s Law (F? = -kx). Correction: The negative sign means the spring force opposes displacement. If x is positive (stretched), F? is negative (pulls back).
Mistake: Forgetting to include all forces in the FBD. Correction: Every force acting on the object must be drawn. Example: A hanging sign has tension and weight.
Mistake: Mixing up tension in ropes with different masses. Correction: Tension is not always the same in a rope with mass. For massless ropes, tension is uniform.
Mistake: Using F = ma for equilibrium problems. Correction: If an object is not accelerating, ?F = 0, not ma.
Apparent weight (e.g., elevator problems where N-mg).
Multiple-Choice Traps:
Tension in ropes: If a rope has mass, tension varies (rare on AP, but possible).
Tricky Distinctions:
Static vs. Dynamic Equilibrium: Both have ?F = 0, but dynamic includes constant velocity.
Lab-Based Questions:
A 5 kg block is at rest on a horizontal table. A rope pulls horizontally with 20 N of tension, but the block doesn’t move. What is the normal force exerted by the table on the block? (A) 0 N (B) 20 N (C) 49 N (D) 69 N
Answer: (C) 49 N. Explanation: The block is in equilibrium (?F = 0). Normal force balances weight (mg = 5 × 9.8 = 49 N). Tension is horizontal and doesn’t affect N.
A spring with spring constant k = 200 N/m is compressed by 0.1 m. What is the magnitude and direction of the spring force?
Answer: 20 N, opposite the direction of compression. Explanation: F? = -kx = -(200 N/m)(-0.1 m) = +20 N (positive because it pushes back against compression).
A 10 kg box is suspended by two ropes at angles of 30° and 60° from the vertical. Which rope has greater tension? (A) The rope at 30° (B) The rope at 60° (C) Both have equal tension (D) Not enough information
Answer: (A) The rope at 30°. Explanation: The vertical components of tension must sum to mg. The rope at 30° has a smaller vertical component (T cos30°), so its tension must be larger to compensate.
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