Function Conjunction → Functions composed of Physical Expressions

Functions for a point charge $q'$

The electric scalar potential $\mathbf{\varphi}$ at $\left(\mathbf{r},t\right)$ due to a point charge $q'$ at $\left(\mathbf{r'},t'\right)$ is:

$\mathbf{\varphi}\left(\mathbf{r},\mathbf{r'}\right) \quad = \quad \underset{constant}{\frac{q'}{4\pi\ \epsilon_0}} \quad \underset{proximity}{\frac{1}{|\mathbf{r}-\mathbf{r'}|}}$

The magnetic vector potential $A$ at $\left(\mathbf{r},t\right)$ due to a point charge $q'$ which had a velocity $\frac{∂\mathbf{r'}}{∂t}$ at $\left(\mathbf{r'},t'\right)$ is:

$\mathbf{A}\left(\mathbf{r},\mathbf{r'}\right) \quad = \quad \mathbf{\varphi}\left(\mathbf{r},\mathbf{r'}\right) \quad \underset{constant}{\frac{1}{c^2}} \quad \underset{dislocation}{\frac{∂\mathbf{r'}}{∂t}}$

$\mathbf{A}\left(\mathbf{r},\mathbf{r'}\right) \quad = \quad \underset{constant}{\frac{\mu_0\ q'}{4\pi}} \quad \underset{proximity}{\frac{1}{|\mathbf{r}-\mathbf{r'}|}} \quad \underset{dislocation}{\frac{∂\mathbf{r'}}{∂t}}$

Functions for an ordered pair of point charges $(q,q')$

A charge $q$ subject to an electric scalar potential $\varphi$ at $\left(\mathbf{r},t\right)$ due to a point charge $q'$ at $\left(\mathbf{r'},t'\right)$ has an electric potential energy of:

$q\varphi\left(\mathbf{r},\mathbf{r'}\right) \quad = \quad \underset{constant}{\frac{qq'}{4\pi\ \epsilon_0}} \quad \underset{proximity}{\frac{1}{|\mathbf{r}-\mathbf{r'}|}}$

A charge $q$ subject to a magnetic vector potential $A$ at $\left(\mathbf{r},t\right)$ due to a point charge $q'$ which had a velocity $\frac{∂\mathbf{r'}}{∂t}$ at $\left(\mathbf{r'},t'\right)$ has a potential momentum of:

$q\mathbf{A}\left(\mathbf{r},\mathbf{r'}\right) \quad = \quad \varphi\left(\mathbf{r},\mathbf{r'}\right) \quad \underset{constant}{\frac{q}{c^2}} \quad \underset{dislocation}{\frac{∂\mathbf{r'}}{∂t}}$

$q\mathbf{A}\left(\mathbf{r},\mathbf{r'}\right) \quad = \quad \underset{constant}{\frac{\mu_0\ qq'}{4\pi}} \quad \underset{proximity}{\frac{1}{|\mathbf{r}-\mathbf{r'}|}} \quad \underset{dislocation}{\frac{∂\mathbf{r'}}{∂t}}$

Lorentz Force for $(q,q')$

The Lorentz Force between charges $(q,q')$ can be derived from the scalar potential $\varphi$ and the vector potential $\mathbf{A}$.

A charge $q$ which has a velocity of $\mathbf{v}$ at $\left(\mathbf{r},t\right)$ will experience a Lorentz force due to a point charge $q'$ at $\left(\mathbf{r'},t'\right)$ of:

$\mathbf{F} \quad = \quad q\left[\mathbf{E} + \mathbf{v} \times \mathbf{B}\right]$

The electric field $\mathbf{E}$ is:

$\mathbf{E} \quad = \quad - \nabla \varphi - \frac{∂\mathbf{A}}{∂t}$

The magnetic field $\mathbf{B}$ is:

$\mathbf{B} \quad = \quad \nabla \times \mathbf{A}$

The Lorentz Force can be expressed directly in terms of the potentials:

$\mathbf{F} \quad = \quad q\left[- \nabla \varphi - \frac{∂\mathbf{A}}{∂t} + \mathbf{v} \times \left( \nabla \times \mathbf{A} \right)\right]$

Where:

• $-\nabla \varphi$ = negative the gradient of the scalar potential $\varphi$.
• $-\frac{∂\mathbf{A}}{∂t}$ = negative the partial derivative of the magnetic vector potential $\mathbf{A}$ with respect to time $t$.
• $\mathbf{v} \times \left( \nabla \times \mathbf{A} \right)$ = the cross product of the velocity $\mathbf{v}$ of the charge $q$ and the curl of the magnetic vector potential $\nabla \times \mathbf{A} = \mathbf{B}$ due to charge $q'$.

To restate from a previous section, the magnetic vector potential of a charge $q$ experienced by a charge $q$ is:

$\mathbf{A}\left(\mathbf{r},\mathbf{r'}\right) \quad = \quad \underset{constant}{\frac{\mu_0\ q'}{4\pi}} \quad \underset{proximity}{\frac{1}{|\mathbf{r}-\mathbf{r'}|}} \quad \underset{dislocation}{\frac{∂\mathbf{r'}}{∂t}}$

The partial derivative of this with respect to time $t$ is:

$\frac{∂\mathbf{A}\left(\mathbf{r},\mathbf{r'}\right)}{∂t} \quad = \quad \underset{constant}{\frac{\mu_0\ q'}{4\pi}} \left[ \underset{proximity}{ \frac{ ∂\left[ \frac{1}{|\mathbf{r}-\mathbf{r'}|} \right] }{∂t}} \quad \underset{dislocation}{\frac{∂\mathbf{r'}}{∂t}} + \underset{proximity}{\frac{1}{|\mathbf{r}-\mathbf{r'}|}} \quad \underset{dislocation}{ \frac{ ∂\left[ \frac{∂\mathbf{r'}}{∂t} \right] }{∂t}} \right]$

$\frac{∂\mathbf{A}\left(\mathbf{r},\mathbf{r'}\right)}{∂t} \quad = \quad \underset{constant}{\frac{\mu_0\ q'}{4\pi}} \left[ \underset{proximity}{ \frac{ ∂\left[ \frac{1}{|\mathbf{r}-\mathbf{r'}|} \right] }{∂t}} \quad \underset{dislocation}{\frac{∂\mathbf{r'}}{∂t}} + \underset{proximity}{\frac{1}{|\mathbf{r}-\mathbf{r'}|}} \quad \underset{dislocation}{ \frac{∂^2r'}{∂t^2} } \right]$

Where:

• $\frac{∂r'}{∂t}$ = the velocity of $q'$ at the retarded time $t'$ according to an observer at time $t$ sharing the same inertial frame as $q$.
• $\frac{∂^2r'}{∂t^2}$ = the acceleration of $q'$ at the retarded time $t'$ according to an observer at time $t$ sharing the same inertial frame as $q$.
• $\frac{1}{|\mathbf{r}-\mathbf{r'}|}$ = the proximity of the position $r$ of $q$ at time $t$ to the position $r'$ of $q'$ at the retarded time $t'$ (i.e. the inverse of the norm of the vector difference between the two position vectors $r$ and $r'$).
• $\frac{ ∂\left[ \frac{1}{|\mathbf{r}-\mathbf{r'}|} \right] }{∂t}$ = the partial derivative of this proximity with respect to time $t$.

See also

• The Anatomy of a Physical Expression

Site map

HQ ● Glossary ● April 2016 Presentation

Replication Station S.H.O. Drive Mark I Maker's Pledge Bill of materials Video recording methodology Presentation Data collection Replication score card Function Conjunction Magnetic Energy The Anatomy of a Physical Expression Functions composed of Physical Expressions Electromagnetic Potentials Frontier Fork Reading Railroad Media Avenue 2015: Dec 2016: Jan Feb Mar May Jun Aug Dec 2017: Jan Memory Lane YouTube: '06 '07 '08 '09 '10 '11 '12 '13 '14 '15 '16 Precession Circle Script Strip