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Τι (ποιος) είναι recursion equation - ορισμός
Lindley recursion; Lindley's integral equation
Schrödinger equation
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![[[Erwin Schrödinger]]](https://commons.wikimedia.org/wiki/Special:FilePath/Erwin Schrodinger2.jpg?width=200 "[[Erwin Schrödinger]]")
![spring]], oscillates back and forth. (C–H) are six solutions to the Schrödinger Equation for this situation. The horizontal axis is position, the vertical axis is the real part (blue) or imaginary part (red) of the [[wave function]]. [[Stationary state]]s, or energy eigenstates, which are solutions to the time-independent Schrödinger equation, are shown in C, D, E, F, but not G or H.](https://commons.wikimedia.org/wiki/Special:FilePath/QuantumHarmonicOscillatorAnimation.gif?width=200 "spring]], oscillates back and forth. (C–H) are six solutions to the Schrödinger Equation for this situation. The horizontal axis is position, the vertical axis is the real part (blue) or imaginary part (red) of the [[wave function]]. [[Stationary state]]s, or energy eigenstates, which are solutions to the time-independent Schrödinger equation, are shown in C, D, E, F, but not G or H.")
![harmonic oscillator]]. Left: The real part (blue) and imaginary part (red) of the wave function. Right: The [[probability distribution]] of finding the particle with this wave function at a given position. The top two rows are examples of '''[[stationary state]]s''', which correspond to [[standing wave]]s. The bottom row is an example of a state which is ''not'' a stationary state. The right column illustrates why stationary states are called "stationary".](https://commons.wikimedia.org/wiki/Special:FilePath/StationaryStatesAnimation.gif?width=200 "harmonic oscillator]]. Left: The real part (blue) and imaginary part (red) of the wave function. Right: The [[probability distribution]] of finding the particle with this wave function at a given position. The top two rows are examples of '''[[stationary state]]s''', which correspond to [[standing wave]]s. The bottom row is an example of a state which is ''not'' a stationary state. The right column illustrates why stationary states are called \"stationary\".")
PARTIAL DIFFERENTIAL EQUATION DESCRIBING HOW THE QUANTUM STATE OF A NON-RELATIVISTIC PHYSICAL SYSTEM CHANGES WITH TIME
Schrodingers equation; Schroedinger's equation; Schroedinger equation; Schrödinger Wave Equation; Schrodinger's equation; Schrödinger wave equation; Schrödinger's equation; Schrödinger-equation; Schrödinger Equation; Schrödinger's wave equation; TDSE; Time-independent Schrödinger equation; Time-independent Schrodinger equation; Time-independent schrödinger equation; Time-independent schrodinger equation; Schrodinger Equation; Shrodinger equation; Shrodinger's equation; Schroedinger Equation; Sherdinger's equation; Shredinger's equation; Sherdinger equation; Shredinger equation; Schrodinger's wave equation; Schrodinger`s equation; Schrodiner`s equation; Erwin Schrodinger's wave model; Time independent Schrödinger equation; Schroedinger wave equation; Time-independent Schroedinger equation; Schrodinger Wave Equation; Schroedinger Wave Equation; Schroedinger's wave equation; Time independent Schroedinger equation; Schrodinger-equation; Time independent Schrodinger equation; Time-independent schroedinger equation; Schroedinger-equation; Schrodinger wave equation; Schrodinger equation; TISE; Schrodinger operator; Schrödinger’s equation; Schrodinger's Wave Equation; Schrödinger's Wave Equation; Schrodinger's Equation; Schrödinger's Equation; Schrodinger model; Schrödinger model; Non-Relativistic Schrodinger Wave Equation; Time-dependent Schrödinger equation; Schrodinger’s equation; Schrodenger equation
The Schrödinger equation is a linear partial differential equation that governs the wave function of a quantum-mechanical system. It is a key result in quantum mechanics, and its discovery was a significant landmark in the development of the subject.
Schrodinger equation
PARTIAL DIFFERENTIAL EQUATION DESCRIBING HOW THE QUANTUM STATE OF A NON-RELATIVISTIC PHYSICAL SYSTEM CHANGES WITH TIME
Schrodingers equation; Schroedinger's equation; Schroedinger equation; Schrödinger Wave Equation; Schrodinger's equation; Schrödinger wave equation; Schrödinger's equation; Schrödinger-equation; Schrödinger Equation; Schrödinger's wave equation; TDSE; Time-independent Schrödinger equation; Time-independent Schrodinger equation; Time-independent schrödinger equation; Time-independent schrodinger equation; Schrodinger Equation; Shrodinger equation; Shrodinger's equation; Schroedinger Equation; Sherdinger's equation; Shredinger's equation; Sherdinger equation; Shredinger equation; Schrodinger's wave equation; Schrodinger`s equation; Schrodiner`s equation; Erwin Schrodinger's wave model; Time independent Schrödinger equation; Schroedinger wave equation; Time-independent Schroedinger equation; Schrodinger Wave Equation; Schroedinger Wave Equation; Schroedinger's wave equation; Time independent Schroedinger equation; Schrodinger-equation; Time independent Schrodinger equation; Time-independent schroedinger equation; Schroedinger-equation; Schrodinger wave equation; Schrodinger equation; TISE; Schrodinger operator; Schrödinger’s equation; Schrodinger's Wave Equation; Schrödinger's Wave Equation; Schrodinger's Equation; Schrödinger's Equation; Schrodinger model; Schrödinger model; Non-Relativistic Schrodinger Wave Equation; Time-dependent Schrödinger equation; Schrodinger’s equation; Schrodenger equation
¦ noun Physics a differential equation which forms the basis of the quantum-mechanical description of a particle.
Origin
1920s: named after the Austrian physicist Erwin Schrodinger.
Richards equation
NON-LINEAR PARTIAL DIFFERENTIAL EQUATION THAT REPRESENTS THE MOVEMENT OF WATER IN UNSATURATED SOILS
Richards' Equation; Richards' equation; Richards Equation; The Richards equation
The Richards equation represents the movement of water in unsaturated soils, and is attributed to Lorenzo A. Richards who published the equation in 1931.
Βικιπαίδεια
Lindley equation
In probability theory, the Lindley equation, Lindley recursion or Lindley processes is a discrete-time stochastic process An where n takes integer values and:
- An + 1 = max(0, An + Bn).
Processes of this form can be used to describe the waiting time of customers in a queue or evolution of a queue length over time. The idea was first proposed in the discussion following Kendall's 1951 paper.
