| Line 21: |
Line 21: |
| | ==Principles== | | ==Principles== |
| | | | |
| − | *Every system can be described by a wave function, which is generally a function of the position coordinates and time. All possible predictions of the physical properties of the system can be obtained from the wave function. The wave function can be obtained by solving the [[Schrodinger equation]] for the system. | + | *Every system can be described by a wave function, which is generally a function of the position coordinates and time. All possible predictions of the physical properties of the system can be obtained from the wave function. The wave function can be obtained by solving the [[Schrodinger equation]] (or the Klein-Gordon equation for relativistic-quantum mechanics) for the system. |
| | | | |
| | *An observable is a property of the system which can be measured. In some systems, many observables can take only certain specific values. | | *An observable is a property of the system which can be measured. In some systems, many observables can take only certain specific values. |
| Line 38: |
Line 38: |
| | | | |
| | ===The uncertainty principle=== | | ===The uncertainty principle=== |
| − | As a result of the wave nature of a particle, certain quantities cannot be known to an arbitrary precision simultaneously. An example is position and [[momentum (physics)|momentum]]. Whenever its position is measured more accurately (beyond a certain limit), its momentum becomes less certain, and vice versa. Hence, there is an inherent uncertainty that prevents precisely measuring both the position and the momentum simultaneously. This is known as the [[Heisenberg Uncertainty Principle]]:<ref>http://hyperphysics.phy-astr.gsu.edu/Hbase/uncer.html</ref> | + | As a result of the wave nature of a particle, certain quantities cannot be known to an arbitrary precision simultaneously. This happens when the operators for the two quantities do not [[Commutative|commute]]. An example is position and [[momentum (physics)|momentum]]. Whenever its position is measured more accurately (beyond a certain limit), its momentum becomes less certain, and vice versa. Hence, there is an inherent uncertainty that prevents precisely measuring both the position and the momentum simultaneously. This is known as the [[Heisenberg Uncertainty Principle]]:<ref>http://hyperphysics.phy-astr.gsu.edu/Hbase/uncer.html</ref> |
| | | | |
| | :<math> \sigma_x \sigma_p \ge \frac{\hbar}{2}</math> | | :<math> \sigma_x \sigma_p \ge \frac{\hbar}{2}</math> |
| Line 45: |
Line 45: |
| | * <math>\sigma_p</math> is the [[standard deviation]] of momentum | | * <math>\sigma_p</math> is the [[standard deviation]] of momentum |
| | * <math>\hbar</math> is the [[Planck's Constant|reduced Planck's constant]] | | * <math>\hbar</math> is the [[Planck's Constant|reduced Planck's constant]] |
| | + | |
| | + | Other examples include energy and time, as well as different components of [[angular momentum]]. |
| | | | |
| | ==Interpretations== | | ==Interpretations== |