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Magnetic induction

Storyboard

An inductance is an element that by varying the current flowing through it generates a potential that opposes the same current flow. It operates as a system that dampens the current flowing through it. It works by means of a coil in which the current generates a magnetic field that in turn generates the potential that opposes the current.

>Model

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Magnetic Field around a Wire

Image

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Calculation of the electric potential

Equation

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The electric potential (\varphi) can be calculated from the base electrical potential (\varphi_0) and the electric field (\vec{E}) integrated along a path over the path element traveled (d\vec{s}):

\varphi =\varphi_0 - \displaystyle\int_C \vec{E}\cdot d\vec{s}

\varphi_0
Base electrical potential
V
5478
\vec{E}
Electric field
V/m
9687
\varphi
Electric potential
V
5479
d\vec{s}
Infinitesimal distance
m
5480
DV = l * v * B phi = phi_0 - @INT( &E . d&s , C )phi_0&EphidslBDphiv

The potential difference (\Delta\varphi) is equal to the sum of the electric field (\vec{E}) along an integrated path over the path element traveled (d\vec{s}):

\Delta\varphi = -\displaystyle\int_C \vec{E}\cdot d\vec{s}



As the potential difference (\Delta\varphi) is calculated by considering the electric potential (\varphi) minus the base electrical potential (\varphi_0):

\Delta\varphi = \varphi - \varphi_0



therefore

\varphi =\varphi_0 - \displaystyle\int_C \vec{E}\cdot d\vec{s}

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Induction current by magnetic field

Equation

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If the conductor moves through a magnetic field \vec{B} or the magnetic field with respect to the conductor with a speed \vec{v} a force is generated according to Lorentz's Law equal to

F = q v B \sin \theta



where it was assumed that the charge is q and the velocity is orthogonal to the magnetic field.

The force can be described by an induced electric field \vec{E} and this can be associated with a potential difference \Delta V divided by the length of the l of the driver

F=qE=q\displaystyle\frac{\Delta V}{l}

With this the induced potential is equal to

\Delta V = l v B

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