Problem 48
Question
A 10.0 -g marble slides to the left with a velocity of magnitude 0.400 \(\mathrm{m} / \mathrm{s}\) on the frictionless, horizontal surface of an icy New York side- walk and has a head- on, elastic collision with a larger 30.0 -g marble sliding to the right with a velocity of magnitude 0.200 \(\mathrm{m} / \mathrm{s}(\mathrm{Fig} . \mathrm{E} 8.48) .\) (a) Find the velocity of each marble (magnitude and direction) after the collision. (Since the collision is head-on, all the motion is along a line.) (b) Calculate the change in momentum (that is, the momentum after the collision minus the momentum before the collision for each marble. Compare the values you get for each marble. (c) Calculate the change in kinetic energy (that is, the kinetic energy after the collision minus the kinetic energy before the collision) for each marble. Compare the values you get for each marble.
Step-by-Step Solution
VerifiedKey Concepts
Conservation of Momentum
For the marbles, this means:
- The momentum before the collision was the momentum of the 10.0-g marble and the 30.0-g marble added together.
- Since the collision is elastic, no external forces affect the system, hence the momentum is conserved.
- Mathematically, this conservation is expressed as:\[ m_1 v_{1i} + m_2 v_{2i} = m_1 v_{1f} + m_2 v_{2f} \]
Conservation of Kinetic Energy
In our marble collision scenario:
- The total kinetic energy of both marbles before the collision must match the total kinetic energy after.
- For the collision, this is expressed mathematically as:\[ \frac{1}{2}m_1 v_{1i}^2 + \frac{1}{2}m_2 v_{2i}^2 = \frac{1}{2}m_1 v_{1f}^2 + \frac{1}{2}m_2 v_{2f}^2 \]
- Keeping both momentum and kinetic energy equations in view solidifies the understanding that no energy is lost. It merely transfers between the marbles.
One-Dimensional Motion
For the marbles:
- The challenge was figuring out the final velocities along this same line as it simplifies to dealing only with magnitude and positive or negative direction.
- This simplification eliminates complex 3D vector calculations and instead focuses on understanding how the marbles interact linearly.
- Effectively, each marble switches its motion along the line while adhering to conservation laws.
Change in Momentum
For this exercise, the individual changes in momentum for each marble are calculated to illustrate:
- For the 10.0-g marble:\( \Delta p_1 = 0.010(0.200 - (-0.400)) = 0.006 \; \text{kg} \cdot \text{m/s} \)
- For the 30.0-g marble:\( \Delta p_2 = 0.030(-0.400 - 0.200) = -0.018 \; \text{kg} \cdot \text{m/s} \)
- These individual changes confirm total momentum change is zero because they offset each other's changes perfectly.
Change in Kinetic Energy
Key insights include:
- For the 10.0-g marble, the change in kinetic energy before and after the collision was nil:\( \Delta KE_1 = \frac{1}{2}(0.010)(0.200^2 - (-0.400)^2) = 0 \)
- Similarly, the 30.0-g marble experiences no change:\( \Delta KE_2 = \frac{1}{2}(0.030)((-0.400)^2 - 0.200^2) = 0 \)
- This further confirms no energy was converted to other forms like heat or sound, validating the collision's elastic nature.