Menu Home Action My entries Defined browse Select Select in the list MathematicsPhysics Then Select Select in the list Then Select Select in the list Search

susceptibility

 Definition/Summary Susceptibility is a property of material. In a vacuum it is zero. Susceptibility is an operator (generally a tensor), converting one vector field to another. It is dimensionless. Electric susceptibility $\chi_e$ is a measure of the ease of polarisation of a material. Magnetic susceptibility $\chi_m$ is a measure of the strengthening of a magnetic field in the presence of a material. Diamagnetic material has negative magnetic susceptibility, and so weakens a magnetic field.

 Equations Electric susceptibility $\chi_e$ and magnetic susceptibility $\chi_m$ are the operators which convert the electric field and the magnetic intensity field, $\varepsilon_0\mathbf{E}$ and $\mathbf{H}$ ($not$ the magnetic field $\mathbf{B}$), respectively, to the polarisation and magnetisation fields $\mathbf{P}$ and $\mathbf{M}$: $$\mathbf{P}\ = \chi_e\,\varepsilon_0\,\mathbf{E}$$ $$\mathbf{M}\ = \chi_m\,\mathbf{H}\ = \frac{1}{\mu_0}\,\chi_m\,(\chi_m\,+\,1)^{-1}\,\mathbf{B}\ = \frac{1}{\mu_0}\,(1\,-\,(\chi_m\,+\,1)^{-1})\,\mathbf{B}$$

 Scientists

 Breakdown Physics > Electromagnetism >> Physical Quantities & Units

 Extended explanation Bound charge and current: Electric susceptibility converts $\mathbf{E}$, which acts on the total charge, to $\mathbf{P}$, which acts only on bound charge (charge which can move only locally within a material). Magnetic susceptibility converts $\mathbf{H}$, which acts on free current, to $\mathbf{M}$, which acts only on bound current (current in local loops within a material, such as of an electron "orbiting" a nucleus). Relative permittivity $\mathbf{\varepsilon_r}$ and relative permeability $\mathbf{\mu_r}$: $$\mathbf{\varepsilon_r}\ =\ \mathbf{\chi_e}\ +\ 1$$ $$\mathbf{\mu_r}\ =\ \mathbf{\chi_m}\ -\ 1$$ $$\mathbf{D}\ =\ \varepsilon_0\,\mathbf{E}\ +\ \mathbf{P}\ =\ \varepsilon_0\,(1\,+\,\mathbf{\chi_e})\,\mathbf{E}\ =\ \mathbf{\varepsilon_r}\,\mathbf{E}$$ $$\mathbf{B}\ =\ \mu_0\,(\mathbf{H}\ +\ \mathbf{M})\ =\ \mu_0\,(1\,+\,\mathbf{\chi_m})\,\mathbf{H}\ =\ \mathbf{\mu_r}\,\mathbf{H}$$ Note that the magnetic equations analogous to $\mathbf{P}\ = \mathbf{\chi_e}\,\varepsilon_0\,\mathbf{E}$ and $\mathbf{D}\ =\ \mathbf{\varepsilon_r}\,\mathbf{E}$ are $\mathbf{M}\ = \frac{1}{\mu_0}\,(1\,-\,(\mathbf{\chi_m}\,+\,1)^{-1})\,\mathbf{B}$ and $\mathbf{H}\ =\ \mathbf{\mu_r}^{-1}\,\mathbf{B}$ In other words, the magnetic analogy of relative permittivity is the inverse of relative permeability, and the magnetic analogy of electric susceptibility is the inverse of a part of magnetic susceptibility. Permittivity: $\mathbf{\varepsilon}\ =\ \varepsilon_0\,\mathbf{\varepsilon_r}$ Permeability: $\mathbf{\mu}\ =\ \mu_0\,\mathbf{\mu_r}$ Units: Relative permittivity and relative permeability, like susceptibility, are dimensionless (they have no units). Permittivity is measured in units of farad per metre ($F.m^{-1}$). Permeability is measured in units of henry per metre ($H.m^{-1}$) or tesla.metre per amp or newton per amp squared. cgs (emu) values: Some books which give values of susceptibility use cgs (emu) units for electromagnetism. Although susceptibility has no units, there is still a dimensionless difference between cgs and SI values, a constant, $4\pi$. To convert cgs values to SI, divide by $4\pi$ for electric susceptibility, and multiply by $4\pi$ for magnetic susceptibility. Tensor nature of susceptibility: For crystals and other non-isotropic material, susceptibility depends on the direction, and changes the direction, and therefore is represented by a tensor. For isotropic material, susceptibility is the same in every direction, and $\mathbf{P}$ (or $\mathbf{M}$) is in the same direction as $\mathbf{E}$ (or $\mathbf{H}$): $$\mathbf{P}\ = \varepsilon_0\,\chi_e\,\mathbf{E}$$ where $\chi_e$ is a multiple of the unit tensor, and therefore is effectively a scalar: $$P^i\ =\ \varepsilon_0\,\chi_e\,E^i$$Ordinary susceptibility is a tensor (a linear operator whose components form a 3x3 matrix) which converts one vector field to another: $$P^i\ =\ \varepsilon_0\,\chi_{e\ j}^{\ i}\,E^j$$ Second-order susceptibility is a tensor (a linear operator whose components form a 3x3x3 "three-dimensional matrix") which converts two copies of one vector field to another: $$P^i\ =\ \varepsilon_0\,\chi_{e\ \ jk}^{(2)\,i}\,E^j\,E^k$$ It is used in non-linear optics. Susceptibility, being a tensor, is always linear in each of its components. The adjective "non-linear" refers to the presence of two (or more) copies of $\bold{E}$. More generally, one can have: $$P^i\ =\ \varepsilon_0\,\sum_{n\ =\ 1}^{\infty}\chi_{e\ \ \ j_1\cdots j_n}^{(n)\,i}\,E^{j_1}\cdots E^{j_n}$$