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Collisions in Multiple Dimensions: Introduction01:05

Collisions in Multiple Dimensions: Introduction

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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...
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Elastic Collisions: Introduction01:00

Elastic Collisions: Introduction

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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...
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Collisions in Multiple Dimensions: Problem Solving01:06

Collisions in Multiple Dimensions: Problem Solving

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In multiple dimensions, the conservation of momentum applies in each direction independently. Hence, to solve collisions in multiple dimensions, we should write down the momentum conservation in each direction separately. To help understand collisions in multiple dimensions, consider an example.
A small car of mass 1,200 kg traveling east at 60 km/h collides at an intersection with a truck of mass 3,000 kg traveling due north at 40 km/h. The two vehicles are locked together. What is the...
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Elastic Collisions: Case Study01:15

Elastic Collisions: Case Study

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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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Intermolecular Forces in Solutions02:28

Intermolecular Forces in Solutions

30.5K
The formation of a solution is an example of a spontaneous process, a process that occurs under specified conditions without energy from some external source.
When the strengths of the intermolecular forces of attraction between solute and solvent species in a solution are no different than those present in the separated components, the solution is formed with no accompanying energy change. Such a solution is called an ideal solution. A mixture of ideal gases (or gases such as helium and argon,...
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Solvating Effects02:12

Solvating Effects

7.8K
An understanding of the solvating effect helps rationalize the relation between solvation and acidity of the compound. In addition, this also explains the relative stability of conjugate bases for compounds with different pKa values. This lesson details, in-depth, the principle of solvating effects. The strength of an acid and the stability of its corresponding conjugate base are determined using pKa values. This observed relationship is a consequence of solvation, which is the interaction...
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Related Experiment Video

Updated: Apr 29, 2026

Rapid Repetition Rate Fluctuation Measurement of Soliton Crystals in a Microresonator
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Rapid Repetition Rate Fluctuation Measurement of Soliton Crystals in a Microresonator

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Many-body interaction in fast soliton collisions.

Avner Peleg1, Quan M Nguyen2, Paul Glenn1

  • 1Department of Mathematics, State University of New York at Buffalo, Buffalo, New York 14260, USA.

Physical Review. E, Statistical, Nonlinear, and Soft Matter Physics
|May 16, 2014
PubMed
Summary

High-order pulse interactions significantly impact nonlinear Schrödinger (NLS) soliton collisions with weak nonlinear loss. These complex dynamics, dependent on initial positions, differ from standard cubic loss scenarios.

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Area of Science:

  • Nonlinear dynamics
  • Soliton interactions
  • Mathematical physics

Background:

  • Cubic nonlinear Schrödinger (NLS) equation governs many physical phenomena.
  • Soliton collisions are crucial for understanding wave packet behavior.
  • Nonlinear loss complicates soliton dynamics.

Purpose of the Study:

  • To investigate n-pulse interactions in fast NLS soliton collisions.
  • To analyze the effect of generic weak nonlinear loss on soliton amplitude shifts.
  • To develop a generalized model for predicting these interactions.

Main Methods:

  • Development of a generalized reduced model for n-pulse interactions.
  • Numerical solutions of the perturbed NLS equation.
  • Analysis of collisions with septic loss (m=3) and generic nonlinear loss (mc=3).

Main Results:

  • Three-pulse interaction dominates amplitude shifts even in four-soliton collisions.
  • Amplitude shifts are highly sensitive to initial soliton positions.
  • High-order pulse interactions are key in generic nonlinear loss scenarios.

Conclusions:

  • n-pulse interactions play a critical role in fast NLS soliton collisions with weak nonlinear loss.
  • Collision dynamics become complex and deviate from cubic loss behavior.
  • The developed model quantitatively demonstrates these effects.