2.3 Contact Forces

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Unit 2.3: Contact Forces in AP Physics 1


Understanding Contact Forces ⛓

In physics, a contact force arises when two objects are physically in contact. This type of force is critical for analyzing motion and interactions between objects. By mastering contact forces, you’ll gain a deeper understanding of how forces like tension, friction, and normal forces shape everyday physical phenomena.

Key Contact Forces

  1. Friction
    Friction opposes the motion of an object in contact with a surface, enabling us to walk, grip, and control vehicles. There are two main types:

    • Static Friction: Resists initial movement between surfaces.
    • Kinetic Friction: Opposes motion between moving surfaces.
  2. Normal Force
    This force acts perpendicular to a surface, supporting an object’s weight. For example, when sitting in a chair, the chair provides an upward normal force to counteract gravity.

  3. Tension
    Tension transmits force along a rope, string, or wire. When you pull on a rope, the tension force transmits that force through the entire length of the rope.

Illustrating Contact Forces in Free-Body Diagrams

When creating free-body diagrams to represent contact forces, keep these principles in mind:

  • Tension: Points along the rope or string in the direction of the force being applied.
  • Friction: Opposes the direction of motion.
  • Normal Force: Always perpendicular to the surface.
  • Spring Force: Opposes the direction of compression or extension.

Example: The diagram of an object on an inclined plane demonstrates key forces, including weight (downward), friction (opposing motion), and the normal force (perpendicular to the surface).

Example Problem: Calculating Normal Force

Problem: A 10.0 kg box is placed on a ramp inclined at 3030^\circ to the horizontal. Calculate the normal force acting on the box.

Solution:

  1. Calculate gravitational force: Fg=mg=(10.0kg)(9.8m/s2)=98.0NF_g = mg = (10.0 \, \text{kg})(9.8 \, \text{m/s}^2) = 98.0 \, \text{N}
  2. Use the normal force equation: Fn=Fgcosθ=(98.0N)cos(30)=86.6NF_n = F_g \cos \theta = (98.0 \, \text{N}) \cos (30^\circ) = 86.6 \, \text{N}

The normal force acting on the box is 86.6 N.

Understanding Hooke’s Law

Hooke’s Law describes how the force exerted by a spring is directly proportional to its displacement:

F=kx

Where:

  • FF = force exerted by the spring (N)
  • kk = spring constant (N/m)
  • xx = displacement from equilibrium (m)

Note: The negative sign indicates the force is restorative (opposing the displacement).

Example Problem: Calculating Spring Force

Problem: How much force is required to stretch a spring with a spring constant of 10N/m10 \, \text{N/m} by 20 m?

Solution:

F=kx=(10N/m)(20m)=200N

The force required is 200 N.

Exploring Friction

Friction opposes motion or attempted motion of an object in contact with a surface. Frictional force can be calculated using:

FfμFnWhere:

  • FfF_f = frictional force (N)
  • μ\mu = coefficient of static or kinetic friction
  • FnF_n = normal force (N)

Static vs. Kinetic Friction

  • Static Friction: Resists the initial movement of an object. Larger than kinetic friction.
  • Kinetic Friction: Acts on moving objects to oppose motion.

Example Problem: Calculating Acceleration on an Inclined Plane

Problem: A 4.00 kg block is placed on a ramp inclined at 3030^\circ to the horizontal. The coefficient of friction between the block and ramp is 0.4000.400. Calculate the block’s acceleration as it slides.

Solution:

  1. Calculate gravitational force: Fg=mg=(4.00kg)(9.81m/s2)=39.24NF_g = mg = (4.00 \, \text{kg})(9.81 \, \text{m/s}^2) = 39.24 \, \text{N}
  2. Calculate normal force: Fn=Fgcosθ=(39.24N)cos(30)=33.97NF_n = F_g \cos \theta = (39.24 \, \text{N}) \cos (30^\circ) = 33.97 \, \text{N}
  3. Calculate frictional force: Ff=μFn=(0.400)(33.97N)=13.59NF_f = \mu F_n = (0.400)(33.97 \, \text{N}) = 13.59 \, \text{N}
  4. Calculate the parallel component of gravity: Fparallel=mgsinθ=(4.00kg)(9.81m/s2)sin(30)=19.62NF_{\text{parallel}} = mg \sin \theta = (4.00 \, \text{kg})(9.81 \, \text{m/s}^2) \sin (30^\circ) = 19.62 \, \text{N}
  5. Find net force: Fnet=FparallelFf=19.62N13.59N=6.03NF_{\text{net}} = F_{\text{parallel}} – F_f = 19.62 \, \text{N} – 13.59 \, \text{N} = 6.03 \, \text{N}
  6. Calculate acceleration: a=Fnetm=6.03N4.00kg=1.51m/s2a = \frac{F_{\text{net}}}{m} = \frac{6.03 \, \text{N}}{4.00 \, \text{kg}} = 1.51 \, \text{m/s}^2

The block’s acceleration down the ramp is 1.51 m/s².


Key Takeaways on Contact Forces

  • Normal Forces support weight and are perpendicular to the contact surface.
  • Tension transmits pulling forces.
  • Friction resists motion and varies depending on surface conditions.
  • Hooke’s Law governs spring force behavior.

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