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Study Guide: AP Physics – Tension, Normal Force, and Spring Force (Hooke’s Law)
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AP Physics – Tension, Normal Force, and Spring Force (Hooke’s Law)

By Fatskills Exam Guides Team — the exam nerds behind 28,500+ quizzes and 2.1M practice questions across 500+ global exams.

⏱️ ~6 min read

AP Physics – Tension, Normal Force, and Spring Force (Hooke’s Law)

AP Physics: Tension, Normal Force, and Spring Force (Hooke’s Law) – Exam-Ready Study Guide


What This Is

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.


Key Terms & Concepts

  • Tension (T): A pulling force exerted by a rope, string, or cable. Acts along the rope, away from the object. Example: A tow truck pulling a car.
  • Normal Force (N or F?): The perpendicular force a surface exerts to support an object. Not always equal to weight! Example: A book resting on a table.
  • Spring Force (F?): The restoring force exerted by a spring when stretched or compressed. Given by Hooke’s Law: F? = -kx, where:
  • F? = spring force (N)
  • k = spring constant (N/m, measures stiffness)
  • x = displacement from equilibrium (m, negative sign indicates force opposes displacement).
  • Equilibrium: When the net force on an object is zero (?F = 0). Objects at rest or moving at constant velocity are in equilibrium.
  • Free-Body Diagram (FBD): A sketch showing all forces acting on an object. Essential for solving problems!
  • Newton’s First Law: An object in motion stays in motion (or at rest) unless acted upon by a net force. Explains why tension and normal force adjust to maintain equilibrium.
  • Newton’s Second Law: ?F = ma. Used to solve for acceleration when forces are unbalanced.
  • Newton’s Third Law: For every action, there’s an equal and opposite reaction. Example: The normal force from the floor pushes up on you because you push down on the floor.
  • Apparent Weight: The normal force you feel (e.g., in an elevator accelerating upward, you feel heavier).
  • Static vs. Kinetic Friction: Static friction adjusts to prevent motion (up to a max), while kinetic friction is constant. Not directly related to tension/normal force, but often tested together.

Step-by-Step / Process Flow

How to Solve Tension/Normal Force/Spring Force Problems

  1. Draw a Free-Body Diagram (FBD):
  2. Sketch the object and all forces acting on it (label magnitudes and directions).
  3. Example: For a block on a ramp, include weight (mg), normal force (N), friction (f), and tension (T) if a rope is attached.

  4. Choose a Coordinate System:

  5. Align axes with the direction of motion (e.g., parallel/perpendicular to a ramp).
  6. For springs, let +x be the direction of stretch/compression.

  7. Resolve Forces into Components:

  8. Break forces into x and y components if needed (e.g., weight on a ramp: mg sin? and mg cos?).

  9. Apply Newton’s Laws:

  10. Equilibrium (?F = 0): Set sum of forces in each direction to zero.
  11. Accelerating (?F = ma): Set sum of forces equal to mass × acceleration.

  12. Solve for Unknowns:

  13. Use algebra to isolate the variable (e.g., tension, normal force, or spring constant).
  14. For springs, remember F? = -kx (the negative sign is crucial for direction!).

  15. Check Units and Reasonableness:

  16. Ensure forces are in Newtons (N), masses in kg, and displacements in meters (m).
  17. Example: A normal force of 500 N for a 50 kg person is reasonable (?500 N weight).

Common Mistakes

  • 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.


AP Exam Insights

  • Frequent FRQ Topics:
  • Equilibrium problems (e.g., a block on a ramp with friction and tension).
  • Spring force questions (e.g., calculating k from a graph of F vs. x).
  • Apparent weight (e.g., elevator problems where N-mg).

  • Multiple-Choice Traps:

  • Normal force-weight: Look for ramps, elevators, or horizontal acceleration.
  • Hooke’s Law direction: The negative sign is often omitted in answer choices.
  • Tension in ropes: If a rope has mass, tension varies (rare on AP, but possible).

  • Tricky Distinctions:

  • Tension vs. Normal Force: Tension pulls (ropes), normal force pushes (surfaces).
  • Static vs. Dynamic Equilibrium: Both have ?F = 0, but dynamic includes constant velocity.

  • Lab-Based Questions:

  • AP loves asking about spring constant (k) experiments. Know how to find k from a F vs. x graph (slope = k).

Quick Check Questions

1. Multiple Choice

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.


2. Short FRQ

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).


3. Multiple Choice

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.


Last-Minute Cram Sheet

  1. Tension (T): Pulling force along a rope; same throughout a massless rope.
  2. Normal Force (N): Perpendicular push from a surface; not always equal to weight!
  3. Hooke’s Law: F? = -kx ( negative sign = force opposes displacement).
  4. Equilibrium: ?F = 0 (object at rest or constant velocity).
  5. Apparent Weight: N = mg + ma (elevator accelerating upward).
  6. Ramp Problems: N = mg cos?, parallel force = mg sin?.
  7. Spring Constant (k): Slope of F vs. x graph (N/m).
  8. FBDs: Always draw all forces acting on the object.
  9. Newton’s Third Law: Normal force is the reaction to your push on the surface.
  10. Tension-Weight: Only equal if the rope is vertical and the object is in equilibrium.