A \(1 \mathrm{~kg}\) mass traveling in the positive \(x\)-direction at \(3 \mathrm{~m} / \mathrm{s}\) strikes a \(3 \mathrm{~kg}\) mass traveling at \(1 \mathrm{~m} / \mathrm{s}\) in the negative \(x\)-direction. The collision is perfectly elastic. What are possible final velocities for the \(1 \mathrm{~kg}\) mass and the \(3 \mathrm{~kg}\) mass, respectively? (A) \(0 \mathrm{~m} / \mathrm{s} ; 3 \mathrm{~m} / \mathrm{s}\) (B) \(3 \mathrm{~m} / \mathrm{s} ;-1 \mathrm{~m} / \mathrm{s}\) (C) \(-3 \mathrm{~m} / \mathrm{s} ; 1 \mathrm{~m} / \mathrm{s}\) (D) \(3 \mathrm{~m} / \mathrm{s} ; 0 \mathrm{~m} / \mathrm{s}\) (E) \((\mathrm{B})\) and (C)

Short Answer

Expert verified
(A) For mass 1: \(v_{1f} = 0\,\mathrm{m/s}\); For mass 2: \(v_{2f} = 3\,\mathrm{m/s}\) (B) For mass 1: \(v_{1f} = -3\,\mathrm{m/s}\); For mass 2: \(v_{2f} = 1\,\mathrm{m/s}\) (C) Both A and B Ans: (C) Both A and B

Step by step solution

01

Understand the properties of perfectly elastic collision and list the given information

A perfectly elastic collision is a collision in which both the momentum and the kinetic energy are conserved. The given information for this problem is: - Mass 1: \(m_1=1 \mathrm{~kg}\) and initial velocity \(v_{1i}=3 \mathrm{~m} / \mathrm{s}\) - Mass 2: \(m_2=3 \mathrm{~kg}\) and initial velocity \(v_{2i}=-1 \mathrm{~m} / \mathrm{s}\)
02

Define the conservation of momentum and kinetic energy

We know that for any collision, the momentum must be conserved. For this problem, the conservation of momentum can be written as \[ m_1 \cdot v_{1i}+m_2 \cdot v_{2i}= m_1 \cdot v_{1f}+m_2 \cdot v_{2f}\] Both kinetic energy and momentum are conserved for perfectly elastic collision, hence the conservation of kinetic energy can be written as \[ \frac{1}{2} {m_1}{v_{1i}}^2 +\frac{1}{2}{m_2}{v_{2i}}^2 = \frac{1}{2} {m_1}{v_{1f}}^2+\frac{1}{2} {m_2}{v_{2f}}^2\]
03

Plug in the given values and solve for the unknowns

Using the given values, we can rewrite the conservation of momentum equation as \[1 \cdot 3 + 3 \cdot (-1) = 1 \cdot v_{1f}+ 3 \cdot v_{2f}\] And rewrite conservation of kinetic energy as \[\frac{1}{2} \cdot 1 \cdot 3^2 + \frac{1}{2} \cdot 3 \cdot (-1)^2 = \frac{1}{2} \cdot 1 \cdot v_{1f}^2 + \frac{1}{2} \cdot 3 \cdot v_{2f}^2\]
04

Simplify and solve the equations

Simplifying the equations, we get \[ 3 - 3 = v_{1f} + 3v_{2f} \ (1) \] \[ 4.5 + 1.5 = 0.5v_{1f}^2 + 1.5v_{2f}^2 \ (2)\] Now multiply equation (1) by 3 and sum it with equation (2). We obtain: \[6 = v_{1f}^2 + 3v_{2f}^2 \] Now, we can rewrite equation (1) as \(v_{1f} = -3v_{2f}+6\). Substitute this into the new equation: \[ 6 = (-3v_{2f}+6)^2 + 3v_{2f}^2 \] Solving this equation, we obtain the possible values for \(v_{2f}\): \(v_{2f} = 3\,\mathrm{m/s}\) or \(v_{2f} = 1\,\mathrm{m/s}\). Now, we can use equation (1) to find the corresponding values of \(v_{1f}\): - For \(v_{2f} = 3\,\mathrm{m/s}\), we have \(v_{1f} = 0\,\mathrm{m/s}\) - For \(v_{2f} = 1\,\mathrm{m/s}\), we have \(v_{1f} = -3\,\mathrm{m/s}\)
05

Match the solution with the given options

From our calculations, we have found two possible final velocities - For mass 1: \(v_{1f} = 0\,\mathrm{m/s}\) or \(v_{1f} = -3\,\mathrm{m/s}\) - For mass 2: \(v_{2f} = 3\,\mathrm{m/s}\) or \(v_{2f} = 1\,\mathrm{m/s}\) This corresponds to options (A) and (C), so the correct answer is (E) \((\mathrm{B})\) and (C).

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Most popular questions from this chapter

A crate of mass \(m\) sits atop a frictionless ramp that has a height and length \(L\). The ramp has mass \(2 m\), which is concentrated at the lower left corner, and it sits on a frictionless ice pond. The crate is released and slides down the ramp. By the instant that the crate reaches the bottom, how far has the ramp moved and in what direction? (A) It hasn't moved. (B) It has moved to the left a distance \(L / 3\). (C) It has moved to the right a distance \(L / 3\). (D) It has moved to the left a distance \(L / 2\). (E) It has moved to the right a distance \(L / 2\).

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