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Theory/Dynamics

Dynamics · Chapter 07

Applications: Objects in Equilibrium

Applications: Objects in Equilibrium detailed theory study guide for Physics.

20 min read · 4 topics

01

Key Concepts

Key concepts will be added here.

02

Examples

Examples will be added here.

03

Introduction to Applications: Objects in Equilibrium

Welcome to Applications: Objects in Equilibrium. Content to be added.

04

Problem-Solving Strategies and Practice

Systematic Problem-Solving Approach

Follow these steps for dynamics problems:

  1. Identify the system: What object(s) are you analyzing?
  2. Draw FBDs: For each object, show all external forces
  3. Choose coordinates: Align axes with acceleration when possible
  4. Apply Newton's Second Law: ∑F⃗=ma⃗\sum \vec{F} = m\vec{a}∑F=ma in component form
  5. Solve equations: Use algebra or simultaneous equations
  6. Check: Do signs make sense? Are units correct?

Practice 1: Hanging Lamp

A 2 kg lamp hangs motionless from a wire. Find tension.

Lamp hanging

FBD of lamp

Solution: Equilibrium (ay=0a_y = 0ay​=0)

Forces: Weight W=mg=20W = mg = 20W=mg=20 N (down), Tension TTT (up)

∑Fy=0  ⟹  T−W=0  ⟹  T=20 N\sum F_y = 0 \implies T - W = 0 \implies T = 20 \, \text{N}∑Fy​=0⟹T−W=0⟹T=20N

Practice 2: Block Pushed on Surface

A 10 kg block on smooth horizontal floor pushed with 20 N horizontally. Find normal force and acceleration.

Block pushed on surface

FBD of pushed block

Solution:

Vertical: Equilibrium → N=W=100N = W = 100N=W=100 N

Horizontal: F=ma  ⟹  20=10a  ⟹  a=2 m/s2F = ma \implies 20 = 10a \implies a = 2 \, \text{m/s}^2F=ma⟹20=10a⟹a=2m/s2

Normal force = 100 N, acceleration = 2 m/s² (horizontal push doesn't affect vertical forces!).

In the pushed block example, does the 20 N horizontal push affect the normal force?

Practice 3: Block Against Wall

A 2 kg block held against smooth vertical wall by 30 N horizontal force and vertical string. Find normal force and tension for equilibrium.

Block against wall

FBD of block

Solution: Equilibrium (ax=0a_x = 0ax​=0, ay=0a_y = 0ay​=0)

Horizontal: F−N=0  ⟹  N=30F - N = 0 \implies N = 30F−N=0⟹N=30 N

Vertical: T−W=0  ⟹  T=mg=20T - W = 0 \implies T = mg = 20T−W=0⟹T=mg=20 N

Practice 4: Weighing Machine in Elevator

An 80 kg person on a scale in an elevator. Find scale reading when elevator:

Person in elevator

FBD of person

(a) Moving at constant 2 m/s upward:

a=0a = 0a=0 → N=W=800N = W = 800N=W=800 N → Reading = 80 kg

(b) Accelerating upward at 2 m/s²:

N−W=maN - W = maN−W=ma → N=800+160=960N = 800 + 160 = 960N=800+160=960 N → Reading = 96 kg

(c) Accelerating downward at 2 m/s²:

N−W=m(−2)N - W = m(-2)N−W=m(−2) → N=800−160=640N = 800 - 160 = 640N=800−160=640 N → Reading = 64 kg

Does a person feel heavier (higher scale reading) when an elevator accelerates upward?

Practice 5: Force on Pulley Support

An Atwood machine with m1=4m_1 = 4m1​=4 kg, m2=6m_2 = 6m2​=6 kg has tension T=48T = 48T=48 N. What force does the clamp exert on the pulley axle?

Solution: Pulley is massless and stationary (equilibrium)

Forces on pulley:

  • Tension T=48T = 48T=48 N downward (from m1m_1m1​ side)
  • Tension T=48T = 48T=48 N downward (from m2m_2m2​ side)
  • Support force FclampF_{clamp}Fclamp​ upward

Fclamp−T−T=0  ⟹  Fclamp=2T=96 NF_{clamp} - T - T = 0 \implies F_{clamp} = 2T = 96 \, \text{N}Fclamp​−T−T=0⟹Fclamp​=2T=96N

The clamp exerts 96 N upward on the pulley.

Key Problem-Solving Tips

  • Always start with a clear FBD
  • Be consistent with sign conventions
  • For connected systems, identify constraints (same acceleration, etc.)
  • Check if object is in equilibrium or accelerating
  • Remember: N≠mgN \neq mgN=mg in general!
  • Friction is self-adjusting (static) or constant (kinetic)
  • Pseudo forces appear only in non-inertial frames
PreviousNewton's Laws and Free Body DiagramsNextApplications: Objects in Motion
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