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Energy in 1D and Successive Collisions Simplified Revision Notes

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15.2.2 Energy in 1D and Successive Collisions

Introduction

This note explores successive direct impacts of elastic spheres and collisions between spheres and smooth surfaces in one dimension. Using the principles of momentum conservation, Newton's law of restitution, and energy considerations, we solve problems involving:

  1. Velocities before and after collisions.
  2. Conditions for further impacts or when collisions cease.

Successive Collisions

When multiple collisions occur between spheres (or between a sphere and a smooth surface), the velocities of each object after one collision become the initial velocities for the next collision.

Conservation of Momentum

The total momentum of the system before and after each collision is conserved:

mAuA+mBuB=mAvA+mBvBm_A u_A + m_B u_B = m_A v_A + m_B v_B

where:

  • mA,mBm_A, m_B: Masses of the spheres,
  • uA,uBu_A, u_B: Initial velocities,
  • vA,vBv_A, v_B: Final velocities.

Newton's Law of Restitution

The coefficient of restitution (ee) relates the speeds of approach and separation:

e=speed of separationspeed of approache = \frac{\text{speed of separation}}{\text{speed of approach}}

or:

e=vBvAuAuBe = \frac{v_B - v_A}{u_A - u_B}

Successive Collisions with a Smooth Plane

For a sphere colliding with a smooth plane:

e=vreboundvimpacte = \frac{v_\text{rebound}}{v_\text{impact}}

where:

  • vimpactv_\text{impact}: Velocity of the sphere just before hitting the plane,
  • vreboundv_\text{rebound}: Velocity of the sphere just after rebounding.

Conditions for Further Impacts

Further impacts between spheres occur if:

vB>vAv_B > v_A

where vBv_B and vAv_A are the final velocities of spheres BB and AA, respectively, after a collision.

If vAvBv_A \geq v_B, the spheres will not collide again.

Worked Examples

infoNote

Example 1: Successive Collisions Between Two Spheres


Problem

Two spheres AA (mass 2 kg) and BB (mass 3 kg) move in a straight line.

Initially:

  • AA moves at 4 ms⁻¹
  • BB moves at 1 ms⁻¹ The coefficient of restitution between AA and BB is e = 0.8.

Determine:

  1. The velocities of AA and BB after their first collision.
  2. Whether the spheres collide again.

Step 1: Apply Conservation of Momentum

mAuA+mBuB=mAvA+mBvBm_A u_A + m_B u_B = m_A v_A + m_B v_B

Substitute the values (mA=2,mB=3,uA=4,uB=1m_A = 2, m_B = 3, u_A = 4, u_B = 1):

2(4)+3(1)=2vA+3vB2(4) + 3(1) = 2v_A + 3v_B

Simplify:

8+3=2vA+3vB11=2vA+3vB.(1)8 + 3 = 2v_A + 3v_B \quad \Rightarrow \quad 11 = 2v_A + 3v_B. \quad \text{(1)}

Step 2: Apply Newton's Law of Restitution

e=vBvAuAuBe = \frac{v_B - v_A}{u_A - u_B}

Substitute e=0.8,uA=4,uB=1e = 0.8, u_A = 4, u_B = 1

8=vBvA418 = \frac{v_B - v_A}{4 - 1}

Simplify:

0.8=vBvA3vBvA=2.4.(2)0.8 = \frac{v_B - v_A}{3} \quad \Rightarrow \quad v_B - v_A = 2.4. \quad \text{(2)}

Step 3: Solve Simultaneous Equations

From equations (1) and (2):

  1. 11=2vA+3vB11 = 2v_A + 3v_B
  2. vB=vA+2.4v_B = v_A + 2.4 Substitute vB=vA+2.4v_B = v_A + 2.4 into (1):
11=2vA+3(vA+2.4)11 = 2v_A + 3(v_A + 2.4)

Simplify:

11=2vA+3vA+7.211=5vA+7.211 = 2v_A + 3v_A + 7.2 \quad \Rightarrow \quad 11 = 5v_A + 7.2

Solve for vAv_A:

5vA=117.2=3.8vA=3.85=0.76ms15v_A = 11 - 7.2 = 3.8 \quad \Rightarrow \quad v_A = \frac{3.8}{5} = 0.76 \, \text{ms}^{-1}

Substitute vA=0.76v_A = 0.76 into vB=vA+2.4v_B = v_A + 2.4

vB=0.76+2.4=3.16ms1v_B = 0.76 + 2.4 = 3.16 \, \text{ms}^{-1}

Step 4: Determine Further Impacts

Further collisions occur if vB>vAv_B > v_A, which is true:

vB=3.16ms1,vA=0.76ms1v_B = 3.16 \, \text{ms}^{-1}, \quad v_A = 0.76 \, \text{ms}^{-1}

Final Answer:

  1. Velocities after the first collision:
  • vₐ = 0.76 ms⁻¹ (sphere A)
  • vᵦ = 3.16 ms⁻¹ (sphere B)
  1. The spheres will collide again.
infoNote

Example 2: Successive Impacts with a Smooth Plane


Problem

A sphere of mass 0.5 kg is dropped from a height of 2 m onto a smooth horizontal plane.

The coefficient of restitution between the sphere and the plane is e = 0.6

Find:

  1. The speed of the sphere just before and just after the first impact.
  2. The height of the sphere after the second rebound.

Part 1: Speed Before and After First Impact


Step 1: Speed before impact:

vimpact=2ghv_\text{impact} = \sqrt{2gh}

where g=9.8ms2,h=2mg = 9.8 \, \text{ms}^{-2}, h = 2 \, \text{m}

Substitute:

vimpact=2×9.8×2=39.26.26ms1v_\text{impact} = \sqrt{2 \times 9.8 \times 2} = \sqrt{39.2} \approx 6.26 \, \text{ms}^{-1}

Step 2: Speed after impact:

vrebound=evimpactv_\text{rebound} = e v_\text{impact}

Substitute e=0.6,vimpact=6.26e = 0.6, v_\text{impact} = 6.26

vrebound=0.6×6.26=3.76ms1v_\text{rebound} = 0.6 \times 6.26 = 3.76 \, \text{ms}^{-1}

Part 2: Height After Second Rebound


Step 1: Use the rebound velocity to find the height:

h=v22gh = \frac{v^2}{2g}

Substitute v=3.76,g=9.8v = 3.76, g = 9.8

h=3.7622×9.8=14.1419.60.72mh = \frac{3.76^2}{2 \times 9.8} = \frac{14.14}{19.6} \approx 0.72 \, \text{m}

Final Answer:

  1. Speed:
  • Before impact: 6.26 ms⁻¹
  • After impact: 3.76 ms⁻¹
  1. Height after the second rebound: 0.72 m

Note Summary

infoNote

Common Mistakes

  1. Incorrect application of restitution: Always ensure the correct relative velocities are used.
  2. Ignoring momentum conservation: Total momentum must always be conserved during collisions.
  3. Misinterpreting conditions for further impacts: Check whether vᵦ > vₐ after collisions.
  4. Forgetting energy loss: With e < 1, kinetic energy is not conserved, so successive rebounds decrease in height.
infoNote

Key Formulas

  1. Newton's Law of Restitution:
e=speed of separationspeed of approache = \frac{\text{speed of separation}}{\text{speed of approach}}
  1. Conservation of Momentum:
mAuA+mBuB=mAvA+mBvBm_A u_A + m_B u_B = m_A v_A + m_B v_B
  1. Free Fall Speed:
v=2ghv = \sqrt{2gh}
  1. Rebound Height:
h=v22gh = \frac{v^2}{2g}
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