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particle and motion
An additional line of reasoning in support of particle theory ( and by extension atomic theory ) began in 1827 when botanist Robert Brown used a microscope to look at dust grains floating in water and discovered that they moved about erratically — a phenomenon that became known as " Brownian motion ".
Bohr, Mottelson and Rainwater were jointly awarded the 1975 Nobel Prize in Physics " for the discovery of the connection between collective motion and particle motion in atomic nuclei and the development of the theory of the structure of the atomic nucleus based on this connection ".
The angular momentum of a particle or rigid body in rectilinear motion ( pure translation ) is a vector with constant magnitude and direction.
This is a simulation of the Brownian motion of a big particle ( dust particle ) that collides with a large set of smaller particles ( molecules of a gas ) which move with different velocities in different random directions.
The term " Brownian motion " can also refer to the mathematical model used to describe such random movements, which is often called a particle theory.
* Mechanics of planar particle motion
Classical physics draws a distinction between particles and energy, holding that only the latter exhibit waveform characteristics, whereas quantum mechanics is based on the observation that matter has both wave and particle aspects and postulates that the state of every subatomic particle can be described by a wavefunction — a mathematical expression used to calculate the probability that the particle, if measured, will be in a given location or state of motion.
The second term of the right-hand side is the convective rate of change and expresses the contribution of the particle changing position in space ( motion ).
Newton's law of motion for a particle of mass m written in vector form is:
Unlike the other two fictitious forces, the centrifugal force always points radially outward from the axis of rotation of the rotating frame, with magnitude, and unlike the Coriolis force in particular, it is independent of the motion of the particle in the rotating frame.
The equations of motion for r that result from this equation for the rotating 2D frame are the same that would arise from a particle in a fictitious one-dimensional scenario under the influence of the force in the equation above.
* Mechanics of planar particle motion
Contrary to brownian motion, which is the diffusion of a single particle, interactions between particles may have to be considered, unless the particles form an ideal mix with their solvent ( ideal mix conditions correspond to the case where the interactions between the solvent and particles are identical to the interactions between particles and the interactions between solvent molecules ; in this case, the particles do not interact when inside the solvent ).
The motion due to any one particle will vary due to the motion of all the other particles in the system.
Lorentz force f on a charged particle ( of electric charge | charge q ) in motion ( instantaneous velocity v ).
Because this is a cross product, the force is perpendicular to both the motion of the particle and the magnetic field.
For example, one can talk about motion of a wave or a quantum particle ( or any other field ) where the configuration consists of probabilities of occupying specific positions.
: Note this model assumes the particle is a point mass, which is certainly known to be false in many cases in which we use this model ; for example, as a model of planetary motion.
The best-known instance of the parabola in the history of physics is the trajectory of a particle or body in motion under the influence of a uniform gravitational field without air resistance ( for instance, a baseball flying through the air, neglecting air friction ).
If the spin of a particle has a positive projection on its direction of motion then it is called left-handed ; otherwise, it is right-handed.

particle and is
This is a theoretically complicated dipole interaction which causes any extremely small uncharged particle to agglomerate with other small uncharged particles, or to stick to an uncharged surface.
The calibration of piezoelectric sensors in terms of the particle parameters is very uncertain.
This `` ejection '' momentum is linearly related to the particle energy.
The relationship between particle size and infectious dose is illustrated in Table 1.
A consequence of using waveforms to describe particles is that it is mathematically impossible to obtain precise values for both the position and momentum of a particle at the same time ; this became known as the uncertainty principle, formulated by Werner Heisenberg in 1926.
Though the word atom originally denoted a particle that cannot be cut into smaller particles, in modern scientific usage the atom is composed of various subatomic particles.
In quantum mechanics, where all particle momenta are associated with waves, it is the formation of such a wave packet which localizes the wave, and thus the particle, in space.
In states where a quantum mechanical particle is bound, it must be localized as a wave packet, and the existence of the packet and its minimum size implies a spread and minimal value in particle wavelength, and thus also momentum and energy.
In quantum mechanics, as a particle is localized to a smaller region in space, the associated compressed wave packet requires a larger and larger range of momenta, and thus larger kinetic energy.
An equivalent definition is the radius of an unperturbed circular Newtonian orbit about the Sun of a particle having infinitesimal mass, moving with an angular frequency of radians per day ; or that length such that, when used to describe the positions of the objects in the Solar System, the heliocentric gravitational constant ( the product GM < sub >☉</ sub >) is equal to ()< sup > 2 </ sup > AU < sup > 3 </ sup >/ d < sup > 2 </ sup >.
Alpha decay is a type of radioactive decay in which an atomic nucleus emits an alpha particle ( two protons and two neutrons ) and thereby transforms ( or ' decays ') into an atom with a mass number 4 less and atomic number 2 less.
Because an alpha particle is the same as a helium-4 nucleus, which has mass number 4 and atomic number 2, this can also be written as:
The alpha particle also has a charge + 2, but the charge is usually not written in nuclear equations, which describe nuclear reactions without considering the electrons.
Alpha decay is the most likely cluster decay because of the combined extremely high binding energy and relatively small mass of the helium-4 product nucleus ( the alpha particle ).
The alpha particle is trapped in a potential well by the nucleus.
The higher value for alpha radiation is generally attributable to the high linear energy transfer ( LET ) coefficient, which is about one ionization of a chemical bond for every angstrom of travel by the alpha particle.
In particle physics, antimatter is material composed of antiparticles, which have the same mass as particles of ordinary matter but have opposite charge and quantum spin.
Particle-antiparticle pairs can annihilate each other, producing photons ; since the charges of the particle and antiparticle are opposite, total charge is conserved.
Because charge is conserved, it is not possible to create an antiparticle without either destroying a particle of the same charge ( as in beta decay ) or creating a particle of the opposite charge.

particle and described
A particle at position r is described by:
Later, Albert Einstein proposed that the quanta of light might be regarded as real particles, and ( still later ) the particle of light was given the name photon, to correspond with other particles being described around this time, such as the electron and proton.
There may be hypothetical elementary particles not described by the Standard Model, such as the graviton, the particle that would carry the gravitational force, and sparticles, supersymmetric partners of the ordinary particles.
A Feynman diagram is a contribution of a particular class of particle paths, which join and split as described by the diagram.
When calculating scattering cross sections in particle physics, the interaction between particles can be described by starting from a free field which describes the incoming and outgoing particles, and including an interaction Hamiltonian to describe how the particles deflect one another.
Commercially, the term filter is applied to membranes where the separation lattice is so thin that the surface becomes the main zone of particle separation, even though these products might be described as sieves.
Consider a state of the system, described by the single particle states ..., n < sub > N </ sub >.
In the Standard Model of particle physics, this symmetry is described as arising as a consequence of a coupling of particles with rest mass to a postulated additional field, known as the Higgs field.
These descriptions include the simultaneous wave-like and particle-like behavior of both matter and radiation energy, this described in the wave – particle duality.
The equation of the orbit described by the particle is thus:
In the Standard Model of particle physics, photons are described as a necessary consequence of physical laws having a certain symmetry at every point in spacetime.
When it was found in 1900 by Max Planck that the energy of waves could be described as consisting of small packets or " quanta ", Albert Einstein further developed this idea to show that an electromagnetic wave such as light could be described as a particle ( later called the photon ) with a discrete quantum of energy that was dependent on its frequency.
For example, a single electron in an unexcited atom is pictured classically as a particle moving in a circular trajectory around the atomic nucleus, whereas in quantum mechanics it is described by a static, spherically symmetric wavefunction surrounding the nucleus ( Fig.
In quantum mechanics, there is wave-particle duality, so the properties of the particle can be described as the properties of a wave.
In quantum mechanics, a particle ( such as an electron or proton ) is described by a complex wavefunction, ψ ( x, t ), whose time-evolution is governed by the Schrödinger equation:
The contemporary strong force is described by quantum chromodynamics ( QCD ), a part of the standard model of particle physics.
The position of the particle is described by a wave function.
Max Delbrück, an important investigator in the area of bacteriophages, described the basic " life cycle " of a virus in 1937: rather than " growing ", a virus particle is assembled from its constituent pieces in one step ; eventually it leaves the host cell to infect other cells.
In one dimension for one particle, the probability of finding a particle in space at some time t ( not shown ) is distributed as a ( complex-valued ) waveform through space, mathematically described by the particle's wave function ψ.
It only turned out much later ( in one of Einstein's Annus Mirabilis papers ) that light can be equally described as a particle ( wave-particle duality of light ).

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