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Energy levels for particle in 1-D box

 E = \frac {\pi^2 \hbar^2 n^2} {2 m a^2}

Where n is an integer,  n= 1,2,3,\dots

and  \hbar = \frac h {2 \pi}

so  E = \frac {\pi^2 h^2 n^2} {2 m a^2 4 \pi^2} = \frac {h^2 n^2} { 8 m a^2}

Relativistic energy

\ {E^2=p^2 c^2 + m_0^2 c^4}

One-dimensional Schrödinger wave equation

 - \frac {\hbar^2} {2m} \frac {d^2 \psi (x)} {dx^2} + U(x)\psi(x) = E\psi(x)

Magnetic field around a single wire

 r = \frac {\mu _{0}I} {2 \pi B}

Probability of finding an object on the other side of a quantum barrier

 P = \exp \left( -2d \sqrt  { \frac {2m(V-E)} { \hbar^2} } \right)

Uncertainty in energy of a state with lifetime  \tau\

 {\delta}E = \frac h {2 \pi\ } \tau\

Van Der Waals Gas

\left ( p + \frac {an^2} {V^2} \right )  (V - nb) = nRT

Diffraction Experiment

 F(hkl) = \sum _{j} f _j (\theta) \cdot \exp[-8\pi^2U_j\sin^2 \frac {\theta} {\lambda^2}] \cdot \exp [2 \pi i (hx_j + ky_j + i z_j]

Eyring constant

 k= \frac {k_B T} n k^ \ddagger\

Difference Map


\Delta \rho (xyz) = \frac 1 {V} \sum _{hkl} ( \left| F _{obs} \right| - \left| F_{calc} \right|) \exp[-2 \pi i(hx+hy+lz-\alpha _{hkl})]

Quadratic formula

 x_{0,1} = \frac {-b \pm \sqrt { b^2 - 4ac } } {2a}

Arithmetic mean

 r =  \frac {1} {N} \sum_{n=1}^N r_n

Geometric mean

 r = [ ( 1 + r_1 ) ( 1 + r_2 ) \dots ( 1 + r_N ) ] ^\frac { 1 } { N } - 1

 r = (\sum_{n=1}^N  1 + r_n)^\frac {1}{N} - 1

Mexican Hat

\psi(t) = {2 \over {\sqrt {3\sigma}\pi^{1 \over 4}}} \left( 1 - {t^2 \over \sigma^2} \right) e^{-t^2 \over 2\sigma^2}

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