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Theory/Dynamics

Dynamics · Chapter 09

Constraint Relations

Constraint Relations detailed theory study guide for Physics.

18 min read · 4 topics

01

Key Concepts

Key concepts will be added here.

02

Examples

Examples will be added here.

03

Introduction to Constraint Relations

Welcome to Constraint Relations. Content to be added.

04

Connected Systems and Constraint Motion

Systems of Connected Objects

Many problems involve multiple objects connected by strings, in contact, or constrained to move together. Two approaches:

1. System Approach: Treat all objects as one system, find common acceleration

2. Individual FBD Approach: Draw separate FBDs for each object, solve simultaneously

Often, you use both: system approach for acceleration, individual FBDs for internal forces (tension, contact forces).

Example 1: Two Blocks in Contact

Two blocks (m1=2m_1 = 2m1​=2 kg, m2=4m_2 = 4m2​=4 kg) on smooth surface. Force F=30F = 30F=30 N pushes m1m_1m1​ toward m2m_2m2​. Find acceleration and contact force.

Two blocks pushed together

System approach: Total mass M=6M = 6M=6 kg

F=Ma  ⟹  30=6a  ⟹  a=5 m/s2F = Ma \implies 30 = 6a \implies a = 5 \, \text{m/s}^2F=Ma⟹30=6a⟹a=5m/s2

Contact force N (using FBD of m2m_2m2​):

FBD of second block

N=m2a=4×5=20 NN = m_2 a = 4 \times 5 = 20 \, \text{N}N=m2​a=4×5=20N

In the two-block system, is the contact force between blocks less than the applied force?

Example 2: Two Blocks Connected by String

Two blocks (m1=5m_1 = 5m1​=5 kg, m2=3m_2 = 3m2​=3 kg) connected by string on smooth surface. Force F=40F = 40F=40 N applied to m1m_1m1​. Find tension.

Two blocks connected by string

System: M=8M = 8M=8 kg, a=F/M=40/8=5 m/s2a = F/M = 40/8 = 5 \, \text{m/s}^2a=F/M=40/8=5m/s2

Tension (using FBD of m2m_2m2​):

FBD of second block

T=m2a=3×5=15 NT = m_2 a = 3 \times 5 = 15 \, \text{N}T=m2​a=3×5=15N

Atwood Machine

Classic problem: Two masses connected over a pulley.

Atwood machine setup

Example: m1=2m_1 = 2m1​=2 kg, m2=3m_2 = 3m2​=3 kg. Find acceleration and tension.

FBD of mass 1

FBD of mass 2

Solution: m2m_2m2​ accelerates down, m1m_1m1​ up, magnitude aaa

For m1m_1m1​ (up positive): T−20=2aT - 20 = 2aT−20=2a ... (1)

For m2m_2m2​ (down positive): 30−T=3a30 - T = 3a30−T=3a ... (2)

Add: 10=5a  ⟹  a=2 m/s210 = 5a \implies a = 2 \, \text{m/s}^210=5a⟹a=2m/s2

From (1): T=20+4=24 NT = 20 + 4 = 24 \, \text{N}T=20+4=24N

In an Atwood machine, is the tension between the two weights (allowing heavier to accelerate down)?

General Atwood Machine Formula

For masses m1m_1m1​ and m2m_2m2​ (where m2>m1m_2 > m_1m2​>m1​):

Acceleration:

a=(m2−m1)gm1+m2a = \dfrac{(m_2 - m_1)g}{m_1 + m_2}a=m1​+m2​(m2​−m1​)g​

Tension:

T=2m1m2gm1+m2T = \dfrac{2m_1 m_2 g}{m_1 + m_2}T=m1​+m2​2m1​m2​g​

These formulas can be derived by solving the force equations as shown above.

Example: Three Blocks in Contact

Three blocks (1 kg, 2 kg, 3 kg) pushed by F=24F = 24F=24 N on smooth surface. Find accelerationand contact forces.

Three blocks pushed

System: M=6M = 6M=6 kg, a=24/6=4 m/s2a = 24/6 = 4 \, \text{m/s}^2a=24/6=4m/s2

Contact forces:

FBD of third block

For m3m_3m3​: N23=m3a=3×4=12N_{23} = m_3 a = 3 \times 4 = 12N23​=m3​a=3×4=12 N

FBD of second block

For m2m_2m2​: N12−N32=m2a  ⟹  N12=12+8=20N_{12} - N_{32} = m_2 a \implies N_{12} = 12 + 8 = 20N12​−N32​=m2​a⟹N12​=12+8=20 N

Contact forces: N12=20N_{12} = 20N12​=20 N, N23=12N_{23} = 12N23​=12 N

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