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In an elementary-particle experiment, a particle of mass \(m\) is fired, with momentum \(m c\), at a target particle of mass \(2 \sqrt{2} m\). The two particles form a single new particle (completely inelastic collision). Find: a) the speed of the projectile before the collision b) the mass of the new particle c) the speed of the new particle after the collision

Short Answer

Expert verified
a) c b) mc c) 2√2m d) m(1 + 2√2)

Step by step solution

01

Identify the Given Information and Unknowns

We are given: - Mass of the projectile \(m\) - Momentum of the projectile \(mc\) - Mass of the target particle \(2\sqrt{2}m\) We are to find: a) The speed of the projectile before the collision b) The mass of the new particle c) The speed of the new particle after the collision
02

Calculate the Speed of Projectile Before the Collision

We are given the momentum of the projectile which is equal to the product of its mass and velocity (\(p\) = mass × velocity). We can use this relationship to find the speed of the projectile before the collision: $$mc = m \times v_{projectile}$$ Divide both sides by \(m\) to find \(v_{projectile}\): $$v_{projectile} = c$$ So the speed of the projectile before the collision is \(c\).
03

Find the Mass of The New Particle

When the two particles collide and form a new single particle, the mass of this new particle (\(m_{new}\)) will be the sum of the masses of the initial particles: $$m_{new} = m + 2\sqrt{2}m$$ Factoring out \(m\), we have: $$m_{new} = m(1 + 2\sqrt{2})$$
04

Determine the Speed of the New Particle After the Collision

Using the conservation of momentum, the momentum before the collision is equal to the momentum after the collision. Let the final speed of the new particle be \(v_{new}\), then: $$\text{Initial momentum} = \text{Final momentum}$$ We have the initial momentum as \(mc\), and the final momentum as \(m_{new} \times v_{new}\): $$mc = m_{new} \times v_{new}$$ Substitute the expression for \(m_{new}\) from Step 3: $$mc = m(1 + 2\sqrt{2}) \times v_{new}$$ To find \(v_{new}\), we can divide both sides by \(m(1 + 2\sqrt{2})\): $$v_{new} = \frac{mc}{m(1 + 2\sqrt{2})}$$ Canceling \(m\) from the numerator and denominator, we get: $$v_{new} = \frac{c}{1 + 2\sqrt{2}}$$ Now we have the solutions for each part: a) The speed of the projectile before the collision is \(c\). b) The mass of the new particle is \(m(1 + 2\sqrt{2})\). c) The speed of the new particle after the collision is \(\frac{c}{1 + 2\sqrt{2}}\).

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Key Concepts

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

Elementary Particle Experiment
In the fascinating world of physics, an elementary particle experiment involves studying the properties and interactions of the smallest known building blocks of matter. These experiments are crucial for scientists to understand the fundamental forces and constituents of the universe.

During such experiments, high-energy collisions between particles are produced in particle accelerators. Through these collisions, scientists can observe the behavior of particles under extreme conditions, create new particles, and test predictions of theoretical physics. In our given problem, the collision between a projectile particle and a target particle leads to the formation of a new particle. By analyzing the collision's outcomes, we gain insights into the mass and speed of the involved particles, which are essential parameters in the study of particle physics.
Conservation of Momentum
The conservation of momentum is a fundamental concept in physics, stating that in a closed system with no external forces, the total momentum remains constant. This principle is rooted in Newton's third law which implies that for every action, there is an equal and opposite reaction.

In our collision scenario, despite the complexity of particle interactions, the total momentum of the system before and after the collision must be the same. This law is instrumental in solving the problem at hand by allowing us to equate the initial momentum of the projectile with the final momentum of the combined particle post-collision. It's the cornerstone for understanding and calculating the behavior of objects during interactions.
Speed of Projectile
The speed of a projectile in physics refers to how fast a moving object is traveling along its path. It's an important aspect of dynamics, especially in projectile motion and collision problems.

In our exercise, it's the initial velocity of the particle before impact. To determine this speed, we apply the known values of the particle's momentum and mass. By doing so, we realize that the speed of the projectile is a crucial element in predicting the outcome of the collision, as it directly influences the final momentum and therefore the energy involved in the interaction. Understanding the speed of projectiles allows us to calculate trajectories, forces, and post-collision velocities.
Mass of Particles
The mass of an object is a fundamental property in physics, representing the amount of matter it contains. In particle physics, the mass of particles is particularly significant as it contributes to the object's inertia and gravity.

When we deal with collisions, as in our exercise, the masses of the colliding objects play a critical role. They determine how momentum is shared between objects in a collision and influence how much energy is transferred or transformed in the process. In the context of our problem, both the mass of the initial projectile and the target particle must be considered to ascertain the mass of the new particle formed after the collision. It's an excellent example to illustrate how mass is conserved in physical interactions, despite the transformation of particles.

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Most popular questions from this chapter

An astronaut on a spaceship traveling at a speed of \(0.50 c\) is holding a meter stick parallel to the direction of motion. a) What is the length of the meter stick as measured by another astronaut on the spaceship? b) If an observer on Earth could observe the meter stick, what would be the length of the meter stick as measured by that observer?

In some proton accelerators, proton beams are directed toward each other for head-on collisions. Suppose that in such an accelerator, protons move with a speed relative to the lab of \(0.9972 c\). a) Calculate the speed of approach of one proton with respect to another one with which it is about to collide head on. Express your answer as a multiple of \(c\), using six significant digits. b) What is the kinetic energy of each proton beam (in units of \(\mathrm{MeV}\) ) in the laboratory reference frame? c) What is the kinetic energy of one of the colliding protons (in units of \(\mathrm{MeV}\) ) in the rest frame of the other proton?

A gravitational lens should produce a halo effect and not arcs. Given that the light travels not only to the right and left of the intervening massive object but also to the top and bottom, why do we typically see only arcs?

A wedge-shaped spaceship has a width of \(20.0 \mathrm{~m}\) a length of \(50.0 \mathrm{~m},\) and is shaped like an isosceles triangle. What is the angle between the base of the ship and the side of the ship as measured by a stationary observer if the ship is traveling by at a speed of \(0.400 c\) ? Plot this angle as a function of the speed of the ship.

A famous result in Newtonian dynamics is that if a particle in motion collides elastically with an identical particle at rest, the two particles emerge from the collision on perpendicular trajectories. Does the same hold in the special theory of relativity? Suppose a particle of rest mass \(m\) and total energy \(E\) collides with an identical particle at rest, the same two particles emerging from the collision with new velocities. Are those velocities necessarily perpendicular? Explain.

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