MSPS:Constants and Equations Poster

From McGill University Physics Department Technical Services Wiki

This page contains content relevant to the MSPS.
For more, please see our:
  • Website (http://www.ugrad.physics.mcgill.ca/~msps)
  • Forum (http://www.ugrad.physics.mcgill.ca/~msps/phpBB2)
  • Wikipage
Table of contents

Overview

We are trying to compile a list of the most used physical constants and equations. This list will be on a giant poster in the lounge so that any student doing homework in the lounge who needs to look up the value of a physical constant or an equation can literally just look up.

So we leave it to YOU. Please help us compile a list of the physical constants and equations that you would like on the poster. Preferably with their values.

Constants

Universal

  • \mu_0 = 4 \pi\ \times \ 10^{-7}\ N/A^2
  • h = 6.626 068 96 \times 10^{-34} J s
    • = 4.135 667 33 \times 10^{-15} eV s
  • \hbar = 1.054 571 628 \times 10^{-34} J s
    • = 6.582 118 99 \times 10^{-16} eV s
  • \mathrm{c} = 2.99 792 458 \times 10^{8} m/s
  • \epsilon_0 = 8.854 187 817... \times 10^{-12} F m^{-1}
  • G = 6.674 28 \times 10^{-11} m^{3} kg^{-1} s^{-2}

Electromagnetism

  • \mathrm{e} = 1.602 176 487 \times 10^{-19} C

Atomic/Nuclear

  • \alpha = \mu_0 e^2 c / (2 h) \
  • m_e = 9.109 382 15(45) \times 10^{-31} kg
  • m_p = 1.672 621 637(83) \times 10^{-27} kg

Thermodynamics

  • k_B=1.380 6505 \times 10^{-23} J \cdot K^{-1}
  • R=8.314 472 J \cdot K^{-1}\cdot mol^{-1}

Equations

Vector Calculus

  • Green's Theorem

\int_{C^+}P\,dx+Q\,dy=\iint_D(\frac{\delta Q}{\delta x}-\frac{\delta P}{\delta y})\,dx\,dy

  • Green's Theorem (Vector Form)

\int_{\delta D} F\cdot\,ds = \iint_D \nabla \times F\cdot k\,dA

  • Stoke's Theorem

\int_{\delta S}F\cdot ds=\iint_S (\nabla \times F)\cdot dS

  • Gauss' Divergence Theorem

\iint_{\delta W}F\cdot dS=\iiint_W \nabla \cdot F\,dV

Maxwell's Equations

Differential Form

  • Gauss' Law for electricity

\nabla \cdot E = \frac{\rho}{\epsilon_0}

  • Gauss' Law for magnetism

\nabla \cdot B = 0

  • Faraday's Law of induction

\nabla \times E = - \frac{\partial B}{\partial t}

  • Ampere's Circuital Law

\nabla \times B = \mu_0 J + \mu_0 \epsilon_0 \frac{\partial E}{\partial t}

Integral Form

  • Gauss' Law for electricity

\oint_S E \cdot dA = \frac{Q_s}{\epsilon_0}

  • Gauss' Law for magnetism

\oint_S B \cdot dA = 0

  • Faraday's Law of induction

\oint_{\partial S} E \cdot dl = -\frac{d \Phi_B,S}{dt}

  • Ampere's Circuital Law

\oint_{\partial S} B \cdot dl = \mu_0 I_S + \mu_0 \epsilon_0 \frac{d \Phi_E,S}{dt}

Fourier Expansions

f(x) = \frac{a_0}{2} + \sum_{n=1}^{\infty} a_n \cos{(\frac{n \pi L}{L})} + b_n \sin{(\frac{n \pi L}{L})}

where:

a_n = \frac{1}{L} \int_{-L}^{L} f(x) \cos{(\frac{n \pi L}{L})} \, dx

b_n = \frac{1}{L} \int_{-L}^{L} f(x) \sin{(\frac{n \pi L}{L})} \, dx

a_0 = \frac{1}{L} \int_{-L}^{L} f(x) \, dx

and 2L your period.

Taylor Expansions

\sin(x)=x-\frac{x^3}{3!}+\frac{x^5}{5!}-...

\cos(x)=1-\frac{x^2}{2!}+\frac{x^4}{4!}-...

\sinh(x)=x+\frac{x^3}{3!}+\frac{x^5}{5!}+...

\cosh(x)=1+\frac{x^2}{2!}+\frac{x^4}{4!}+...

e^x=1+x+\frac{x^2}{2!}+\frac{x^3}{3!}-...

Plus others from Complex Variables.

Trigonometric Functions

First of all, obviously:

e^{i \theta}= \cos \theta+i \sin{ \theta}\frac{}{}

By using this formula and by plugging in ( - θ) and by making a substitution (that is left to the reader as an exercise), we obtain a pair of equations:

\cos z = \frac{1}{2}(e^{iz}+e^{-iz})

and

\sin z = \frac{1}{2i}(e^{iz}-e^{-iz})

These are similar to the definitions of the hyperbolic sine and cosine of real argument θ:

cosh \theta = \frac{1}{2}(e^{\theta}+e^{-\theta})

and

sinh \theta = \frac{1}{2}(e^{\theta}-e^{-\theta})

Knowing that, we can find a new definition for these trigonometric equations:

\cos z = \cos x \cosh y - i\sin x \sinh y\frac{}{}

and

\sin z = \sin x \cosh y + i \cos x \sinh y\frac{}{}

Tensor Manipulation

(Einstein summation convention follows)

Levi-Civita Symbol

det(A^{(3\times3)})=\varepsilon^{ijk}a_{1i}a_{2j}a_{3k}
\left(\vec{A}\times\vec{B}\right)^{k} = \varepsilon^{ijk}A_i B_j
\varepsilon^{ijk}\varepsilon_{imn} = \delta^{j}_{m}\delta^{k}_{n} - \delta^{j}_{n}\delta^{k}_{m}