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Related Concept Videos

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An object absorbing an electromagnetic wave would experience a force in the direction of propagation of the wave. This force occurs because electromagnetic waves contain and transport momentum. The force accounts for the wave's radiation pressure exerted on the object. Maxwell's prediction was confirmed in 1903 by Nichols and Hull by precisely measuring radiation pressures with a torsion balance. The measuring instrument had mirrors suspended from a fiber kept inside a glass container.
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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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The radiation pressure applied by an electromagnetic wave on a perfectly absorbing surface equals the energy density of the wave. The wave's momentum also gets transferred to the surface when an electromagnetic wave is entirely absorbed by it. The rate at which momentum is transmitted to an absorbing surface perpendicular to the propagation direction equals the force on the surface.
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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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Updated: Oct 5, 2025

Laboratory Drop Towers for the Experimental Simulation of Dust-aggregate Collisions in the Early Solar System
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Stellar Shocks from Dark Matter Asteroid Impacts.

Anirban Das1, Sebastian A R Ellis1,2, Philip C Schuster1

  • 1SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, California 94025, USA.

Physical Review Letters
|January 28, 2022
PubMed
Summary
This summary is machine-generated.

Macroscopic dark matter, if it exists, could be detected by observing the transient optical, UV, and X-ray emissions produced when it passes through stars. This method offers a novel way to search for dark matter in various cosmic environments.

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Area of Science:

  • Astrophysics
  • Particle Physics
  • Cosmology

Background:

  • Macroscopic dark matter remains largely unconstrained in the
  • asteroidlike
  • mass range.
  • Such dark matter could interact with baryonic matter via scattering with a geometric cross section.

Purpose of the Study:

  • To propose a novel observational signature for detecting macroscopic dark matter.
  • To investigate the potential of using stellar transient emissions as a probe for dark matter.

Main Methods:

  • Simulating the passage of macroscopic dark matter objects through stars.
  • Analyzing the resulting shock waves and their emission signatures (optical, UV, X-ray).
  • Evaluating the feasibility of detecting these signatures with existing telescopes, particularly in dense stellar environments like globular clusters.

Main Results:

  • The passage of macroscopic dark matter through a star generates shock waves that produce distinctive transient optical, UV, and X-ray emissions.
  • These transient events can be observed across various stellar types and locations.
  • In dense globular clusters, the predicted event rate significantly exceeds background flare events.

Conclusions:

  • The proposed stellar emission signature provides a viable method for searching for macroscopic dark matter.
  • Dedicated observations with existing UV telescopes could constrain orders of magnitude of dark matter mass within a week.
  • This research opens new avenues for dark matter detection beyond traditional methods.