A ball with a mass of # 3 kg# is rolling at #16 m/s# and elastically collides with a resting ball with a mass of # 1 kg#. What are the post-collision velocities of the balls?
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To find the post-collision velocities of the balls, you can use the principle of conservation of momentum and the equation for elastic collisions. The post-collision velocities can be calculated using the following formulas:
[ v_{1f} = \frac{m_1 - m_2}{m_1 + m_2} \cdot v_{1i} + \frac{2m_2}{m_1 + m_2} \cdot v_{2i} ] [ v_{2f} = \frac{2m_1}{m_1 + m_2} \cdot v_{1i} + \frac{m_2 - m_1}{m_1 + m_2} \cdot v_{2i} ]
Where:
- ( v_{1f} ) and ( v_{2f} ) are the final velocities of the two balls,
- ( v_{1i} ) is the initial velocity of the first ball (3 kg),
- ( v_{2i} ) is the initial velocity of the second ball (1 kg),
- ( m_1 ) is the mass of the first ball (3 kg),
- ( m_2 ) is the mass of the second ball (1 kg).
Plugging in the given values:
[ v_{1f} = \frac{3 - 1}{3 + 1} \cdot 16 + \frac{2 \cdot 1}{3 + 1} \cdot 0 ] [ v_{2f} = \frac{2 \cdot 3}{3 + 1} \cdot 16 + \frac{1 - 3}{3 + 1} \cdot 0 ]
[ v_{1f} = \frac{2}{4} \cdot 16 + \frac{2}{4} \cdot 0 ] [ v_{2f} = \frac{6}{4} \cdot 16 + \frac{-2}{4} \cdot 0 ]
[ v_{1f} = 8 + 0 ] [ v_{2f} = 12 - 0 ]
Therefore, the final velocity of the first ball (( v_{1f} )) is 8 m/s, and the final velocity of the second ball (( v_{2f} )) is 12 m/s.
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To find the post-collision velocities of the balls:
- Use the principle of conservation of momentum, which states that the total momentum before the collision is equal to the total momentum after the collision.
- Calculate the initial momentum of the system using the formula: initial momentum = mass × velocity.
- Since the collision is elastic, kinetic energy is conserved as well. Use the formula for kinetic energy: KE = 0.5 × mass × velocity^2.
- Set up equations based on conservation of momentum and conservation of kinetic energy.
- Solve the system of equations to find the post-collision velocities of the balls.
Given:
- Mass of ball 1 (before collision): (m_1 = 3 \text{ kg})
- Mass of ball 2 (before collision): (m_2 = 1 \text{ kg})
- Velocity of ball 1 (before collision): (v_1 = 16 \text{ m/s})
- Velocity of ball 2 (before collision): (v_2 = 0 \text{ m/s})
Using conservation of momentum: (m_1v_1 + m_2v_2 = m_1v_{1f} + m_2v_{2f})
Using conservation of kinetic energy: (\frac{1}{2}m_1v_1^2 + \frac{1}{2}m_2v_2^2 = \frac{1}{2}m_1v_{1f}^2 + \frac{1}{2}m_2v_{2f}^2)
Solving these equations:
From conservation of momentum: (3(16) + 1(0) = 3v_{1f} + 1v_{2f}) (48 = 3v_{1f} + v_{2f}) ...(1)
From conservation of kinetic energy: (\frac{1}{2}(3)(16)^2 + \frac{1}{2}(1)(0)^2 = \frac{1}{2}(3)(v_{1f})^2 + \frac{1}{2}(1)(v_{2f})^2) (192 = 24v_{1f} + \frac{1}{2}v_{2f}^2) ...(2)
Using equation (1) to express (v_{2f}) in terms of (v_{1f}): (v_{2f} = 48 - 3v_{1f})
Substitute this expression for (v_{2f}) into equation (2) and solve for (v_{1f}):
(192 = 24v_{1f} + \frac{1}{2}(48 - 3v_{1f})^2)
Solve for (v_{1f}) and then find (v_{2f}) using equation (1).
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When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
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