Dipole Moment
#Physics #Chemistry
Topics
$\displaystyle \vec{\mu}=q\vec{d}$
- $\displaystyle \mu$ is the dipole moment in debye
- $\displaystyle q$ is the magnitude of the separated charge in Coloumbs
- $\displaystyle \vec{d}$ is a vector pointing from $\displaystyle q_{-}$ to $\displaystyle q_{}$
Electromagnetism
$\displaystyle \vec{p}=\sum_{i = 1}^{n}q_{i}\vec{r}_{i}'$
- Dipole moment of a set of charges
- $\displaystyle \vec{r}'$ is the source vector
- Depends on how origin is defined for physical dipole as opposed to ideal dipole
$\displaystyle \vec{p}\equiv \int \vec{r}' \rho(\vec{r}'), \mathrm{d}\tau'$
- Dipole moment of a distribution
- $\displaystyle \tau'$ is a volume element
$\displaystyle \vec{E}_{\text{dip}}(r,\theta)=\frac{kp}{r^{3}}(2\cos \theta\hat{r}+\sin \theta \hat{\theta})$
- Electric field produced by an dipole moment
- $\displaystyle p$ is the magnitude of the dipole moment
- $\displaystyle r$ is the distance from the dipole moment's center to the point of measurement
- $\displaystyle \theta$ is the angle between the dipole vector and the point of measurement (so imagine pointing the dipole moment in the same direction as the z-axis)
$\displaystyle \vec{\tau}=\vec{p}\times \vec{E}$
- Torque $\displaystyle \vec{\tau}$ experienced by a dipole moment $\displaystyle \vec{p}$ in an electric field $\displaystyle \vec{E}$
$\displaystyle \vec{F}=(\vec{p}\cdot \nabla )\vec{E}$
- The force
Quantum Physics
$\displaystyle \vec{\mu}=\gamma \vec{S}$
- $\displaystyle \gamma$ is the gyromagnetic ratio
- $\displaystyle S$ is the spin angular momentum
$\displaystyle \hat{H}=-\vec{\mu}\cdot \vec{B}=-\gamma \vec{B}\cdot \vec{S}$
$\displaystyle \vec{\tau}=\vec{\mu}\times \vec{B}$
$\displaystyle \vec{F}=\nabla (\vec{\mu}\cdot \vec{B})$
- Force due to an inhomogeneous magnetic field on a dipole $\displaystyle \vec{\mu}$