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This page provides a key to interpreting symbols and units in Introductory Electricity & Magnetism, and provides values of constants in SI units.
Good luck!
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| Symbol | Name | Meaning in Physics 102 |
|---|---|---|
| \( \gamma \) | gamma | Symbol for high-energy EM wave |
| \( \Delta \) | Delta | Symbol for change in a quantity |
| \( \epsilon \) or \( \varepsilon \) | epsilon | Electric polarizability of a material ("permittivity") Careful: Similar to emf symbol \( \mathcal{E} \) |
| \( \theta \) | theta | Angle |
| \( \kappa \) | kappa | Dielectric constant of a material |
| \( \lambda \) | lambda | Wavelength |
| \( \mu \) | mu | Linear (charge) density OR Magnetization in a material in a magnetic field |
| \( \pi \) | pi | The ratio of a circle's circumference to its diameter |
| \( \rho \) | rho | Volume (charge) density |
| \( \sigma \) | sigma (lower case) | Area density or Blackbody radiation constant |
| \( \Sigma \) | Sigma (upper case) | The sum of the following quantity |
| \( \tau \) | tau | Symbol for torque OR Symbol for time constant in a circuit |
| \( \phi \) | phi (lower case) | Angle |
| \( \Phi \) | Phi (upper case) | Symbol for flux |
The symbol 𝛑
This section uses the placeholder variable \( A \). You may use any relevant variable in its place.
| Symbol | Meaning | Use/Definition |
|---|---|---|
| \( \Delta \) | Change | \( \Delta A =A_{final}-A_{initial} \) |
| \( \sum{} \) | Sum | For a series of quantities \( A_1 \), \( A_2 \), \( A_3 \), etc., \( \sum A =A_{1}+A_{2}+A_{3}+\cdots \) |
| \( \vec{A} \) | Vector symbol | The variable represents a vector quantity with magnitude and direction. May also be drawn with partial arrow \( \stackrel{\rightharpoonup}{A} \) |
| \( |\vec{A}| \) | Vector magnitude | The magnitude of the vector \( \vec{A} \) If \( \vec{A} \) is known to be a vector, the magnitude may also be written as \( A \) |
| \( A_x \) | x-component of vector A | The projection of the vector \( \vec{A} \) (magnitude and direction) onto the x axis. Similarly, \( A_y \) and \( A_z \) are the projections of \( \vec{A} \) onto the y and z axes, respectively. |
| \( A_\parallel \) | Parallel component notation | The component of vector \( \vec{A} \) that is parallel to a second reference vector. |
| \( A_\perp \) | Perpendicular component notation | The component of vector \( \vec{A} \) that is perpendicular to a second reference vector. |
| \( A(x) \) | \( A \) as a function of the variable \( x \) | An expression for the value of \( A \) for any input value of the variable \( x \). Be careful: \( A(x) \) does not mean \( A\times x \) |
| \( A_0 \) | Initial value of \( A \) | Typically, the value of \( A \) when \( t=0 \). In function format, \( A(t=0)=A_0 \) May be said as "A naught". |
| \( \arccos(A) \) or \( \cos^{-1}(A) \) | Inverse cosine of \( A \) Similar for other trigonometric functions. | Inverse of the cosine function. Finds the value of \( \theta \) that gives \( \cos(\theta)=A \) May appear as "acos" on some calculators. |
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Physics uses SI units - that is, it constructs all units out of seconds, meters, kilograms, amperes, kelvins, and moles.
| Unit (Symbol) | Quantity | Construction from base units |
|---|---|---|
| meters (m) | Length, distance | \( \mathrm{m} \) |
| kilograms (kg) | Mass | \( \mathrm{kg} \) |
| seconds (s) | Time | \( \mathrm{s} \) |
| Newtons (N) | Force | \( \mathrm{kg}\frac{\mathrm{m}}{\mathrm{s^2}} \) |
| Joules (J) | Energy | \( \mathrm{kg}\frac{\mathrm{m^2}}{\mathrm{s^2}} \) |
| Watts (W) | Power | \( \mathrm{kg}\frac{\mathrm{m^2}}{\mathrm{s^3}} \) |
| Coulombs (C) | Charge | \( \mathrm{A}\cdot \mathrm{s} \) |
| Volts (V) | Electric Potential | \( \mathrm{kg}\frac{\mathrm{m^2}}{\mathrm{s}^3 \cdot \mathrm{A}} \) |
| Amperes (A) | Electric Current | \( \mathrm{A} \) |
| Ohms (\( \Omega \)) | Resistance | \( \mathrm{kg}\frac{\mathrm{m^2}}{\mathrm{s}^3 \cdot \mathrm{A}^2} \) |
| Weber (W) | Magnetic flux | \( \mathrm{kg}\frac{\mathrm{m^2}}{\mathrm{s}^2 \cdot \mathrm{A}} \) |
| Farad (F) | Capacitance | \( \mathrm{A}^2\frac{\mathrm{s^4}}{\mathrm{kg} \cdot \mathrm{m}^2} \) |
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\( \LaTeX \) can be used inside your pages. Just like in Latex, we differentiate between inline-math and display-math. One difference betweem \( \LaTeX \) and these pages is when writing math in \( \LaTeX \), you use one backslash \( (\backslash) \), but in the reference pages you need to use two \( (\backslash \backslash) \).