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Related Concept Videos

Elastic Collisions: Introduction01:00

Elastic Collisions: Introduction

An elastic collision is one that conserves both internal kinetic energy and momentum. Internal kinetic energy is the sum of the kinetic energies of the objects in a system. Truly elastic collisions can only be achieved with subatomic particles, such as electrons striking nuclei. Macroscopic collisions can be very nearly, but not quite, elastic, as some kinetic energy is always converted into other forms of energy such as heat transfer due to friction and sound. An example of a nearly...
Elastic Collisions: Case Study01:15

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Elastic collision of a system demands conservation of both momentum and kinetic energy. To solve problems involving one-dimensional elastic collisions between two objects, the equations for conservation of momentum and conservation of internal kinetic energy can be used. For the two objects, the sum of momentum before the collision equals the total momentum after the collision. An elastic collision conserves internal kinetic energy, and so the sum of kinetic energies before the collision equals...
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When two or more objects collide with each other, they can stick together to form one single composite object (after collision). The total mass of the object after the collision is the sum of the masses of the original objects, and it moves with a velocity dictated by the conservation of momentum. Although the system's total momentum remains constant, the kinetic energy decreases, and thus such a collision is an inelastic collision. Most of the collisions between objects in daily life are...
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It is far more common for collisions to occur in two dimensions; that is, the initial velocity vectors are neither parallel nor antiparallel to each other. Let's see what complications arise from this. The first idea is that momentum is a vector. Like all vectors, it can be expressed as a sum of perpendicular components (usually, though not always, an x-component and a y-component, and a z-component if necessary). Thus, when the statement of conservation of momentum is written for a problem,...
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Impact occurs when two bodies collide, leading to the application of impulsive forces between them. Analyzing impact mechanics involves considering two colliding particles moving along a line known as the line of impact, which passes through their centers and is perpendicular to the contact plane.
When particles with different initial velocities collide, they induce deformation by applying equal and opposite impulses. At the point of maximum deformation, the particles move together with...
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When two objects come in direct contact with each other, it is called a collision. During a collision, two or more objects exert forces on each other in a relatively short amount of time. A collision can be categorized as either an elastic or inelastic collision. If two or more objects approach each other, collide and then bounce off, moving away from each other with the same relative speed at which they approached each other, the total kinetic energy of the system is said to be conserved. This...

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Cusp kernels for velocity-changing collisions.

B H McGuyer1, R Marsland, B A Olsen

  • 1Department of Physics, Princeton University, Princeton, New Jersey 08544, USA.

Physical Review Letters
|June 12, 2012
PubMed
Summary
This summary is machine-generated.

We developed a new "cusp" kernel to model atomic collisions in buffer gases. This analytical tool is more accurate and easier to use than existing methods for understanding atomic behavior.

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Area of Science:

  • Atomic, Molecular, and Optical Physics
  • Chemical Physics

Background:

  • Velocity-changing collisions significantly impact optically pumped atoms in low-pressure environments.
  • Existing models, like the Keilson-Storer kernel, have limitations in accurately representing these collision effects.

Purpose of the Study:

  • To introduce a novel analytical kernel, the "cusp" kernel, for modeling velocity-changing collisions.
  • To provide a more accurate and computationally tractable alternative to existing kernel models.

Main Methods:

  • Developed an analytical kernel (the "cusp" kernel) characterized by a single parameter.
  • Ensured the kernel preserves a Maxwellian velocity distribution, a key physical property.
  • Investigated the properties and utility of cusp kernels and their superpositions.

Main Results:

  • The cusp kernel effectively models the effects of velocity-changing collisions on optically pumped atoms.
  • Cusp kernels demonstrate greater similarity to experimentally and theoretically inferred collision kernels compared to Keilson-Storer kernels.
  • Superpositions of cusp kernels offer enhanced modeling capabilities.

Conclusions:

  • The cusp kernel represents a significant advancement in modeling atomic collisions in buffer gases.
  • Its ease of inversion and improved accuracy make it a valuable tool for researchers in AMO physics and chemical physics.
  • This new kernel facilitates a deeper understanding of steady-state velocity distributions in optically pumped atomic systems.