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A projectile proton with a speed of \(500 \mathrm{~m} / \mathrm{s}\) collides elastically with a target proton initially at rest. The two protons then move along perpendicular paths, with the projectile path at \(60^{\circ}\) from the original direction. After the collision, what are the speeds of (a) the target proton and (b) the projectile proton?

Short Answer

Expert verified
The target proton speed is \(500\sqrt{3} \, \text{m/s}\); the projectile proton speed is \(1000\, \text{m/s}\).

Step by step solution

01

Understanding the Problem

We have a projectile proton with an initial speed of \(500\, \text{m/s}\) colliding elastically with a proton at rest. After the collision, they move at 90 degrees to each other, with the projectile making an angle of \(60^{\circ}\) from its initial direction.
02

Applying Conservation of Momentum

In an elastic collision, momentum is conserved in both the x and y directions. For the x-direction, we have \(m \cdot 500 = m \cdot v_1 \cdot \cos(60^{\circ}) + m \cdot v_2 \cdot \cos(90^{\circ})\). For y-direction: \(0 = m \cdot v_1 \cdot \sin(60^{\circ}) - m \cdot v_2 \cdot \sin(90^{\circ})\).
03

Simplifying Equations

The mass \(m\) cancels out, simplifying the equations to: \(500 = v_1 \cdot \cos(60^{\circ})\) and \(0 = v_1 \cdot \sin(60^{\circ}) - v_2 \). This gives \(v_2 = v_1 \cdot \sin(60^{\circ})\).
04

Solving for \(v_1\) (Projectile Proton Speed)

Substituting the value for \(v_2\) back into the x-direction equation: \(500 = v_1 \cdot \cos(60^{\circ})\), we have \(v_1 = \frac{500}{\cos(60^{\circ})}\). Simplifying, \(v_1 = 1000 \, \text{m/s}\).
05

Solving for \(v_2\) (Target Proton Speed)

Using the relation from Step 3, \(v_2 = v_1 \cdot \sin(60^{\circ})\) and \(v_1 = 1000 \text{ m/s}\), \(v_2 = 1000 \cdot \sin(60^{\circ})\). With \(\sin(60^{\circ}) = \frac{\sqrt{3}}{2}\), we find \(v_2 = 500\sqrt{3} \, \text{m/s}\).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Conservation of Momentum
When two objects collide in a closed system, the total momentum before and after the collision remains constant. This principle is known as the conservation of momentum and is incredibly useful in analyzing collisions.
In the scenario of two protons colliding, like in our original exercise, the total momentum before the collision must equal the total momentum after the collision. Because momentum is a vector, it must be conserved in both the x and y directions separately.
For the x-direction, we represent the momentum as:
  • The momentum of the projectile proton before the collision: \( m \times 500 \)
  • The momentum of both protons after the collision along the x-axis.
Similarly, for the y-direction:
  • Since the target proton is initially at rest, the initial y-momentum is zero.
  • After the collision, the momenta of the two protons must cancel each other out to maintain zero net y-momentum.
This gives us the equations to solve for the velocities of the two protons after the collision. By applying these principles, we can establish the separate equations for x and y that allow us to find the speed of each proton.
Projectile Motion
Projectile motion refers to the curved path that an object follows when it is thrown or propelled near the earth's surface and is subject to gravity only. In the exercise at hand, after the initial collision, the protons continue their paths as projectiles.

The projectile path of the original proton will be influenced by its speed and the angle at which it leaves the point of collision. The path described by the proton moving at an angle is a classic example of projectile motion.
The angle from the original direction tells us how the velocity components will affect the motion. In this problem:
  • The projectile proton moves along a path at an angle of \( 60^{\circ} \).
  • This angle splits its velocity into horizontal and vertical components.
  • The horizontal component is found using \( v_1 \cdot \cos(60^{\circ}) \).
  • The vertical component is found using \( v_1 \cdot \sin(60^{\circ}) \).
By understanding these components, it becomes easier to break down the motion and solve for the speeds involved in the collision. Projectile motion is critical in determining how the protons interact after the collision.
Collision Angle Calculations
Calculating angles in collision problems helps us understand how objects move after hitting one another. In elastic collisions, like the one between two protons, energy is conserved, and the paths they take often shift dramatically.
When evaluating the angle at which our protons travel post-collision, the crucial angles are shared based on conservation principles. Our exercise gives a specific angle of \( 60^{\circ} \), which is essential for the following:
  • Determining how the initial kinematic values split into perpendicular paths.
  • The equation \( v_2 = v_1 \cdot \sin(60^{\circ}) \) helps to understand how target proton diverges at right angles to the projectile's new path.
These angles directly influence the velocity vectors applied in the conservation of momentum calculations. Understanding this is vital since the change in direction and speed tells us how the collision disperses forces between the protons. Effective use of trigonometry allows us to translate these angles into solutions for real-world velocity and movement values.

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