INGENIA

EMG-31

Electric dipole p

Separated-charge dipole.

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GoverningElectric dipole p

Governing equation

p=qdp=q d

d∈[0.1,40]d \in \left[0.1, 40\right]

where

q
q (nC)
d
d (mm)
p
Electric dipole p (pC·m)

The figure, part by part

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EMG-31 · gauge
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①

Governing law — red

p=qdp=q d

d∈[0.1,40]d \in \left[0.1, 40\right]

d=0.1d = 0.1p=0.1p = 0.1

②

Domain of the variable — blue

dmin⁡=0.1,dmax⁡=40d_{\min} = 0.1,\quad d_{\max} = 40

d∈[0.1,40]d \in \left[0.1, 40\right]

d=0.1d = 0.1d=0.1d = 0.1

③

Response curve — green

p=qdp=q d

d∈[0.1,40]d \in \left[0.1, 40\right]

d=0.1d = 0.1p=0.1p = 0.1

④

Rate of change — amber

dpdd\frac{\mathrm{d}p}{\mathrm{d}d}

d∈[0.1,40]d \in \left[0.1, 40\right]

d=0.351d = 0.351p′=1p^{\prime} = 1

Lecture brief

Historical brief

Coulomb, Gauss, Ampère, Faraday and Maxwell (1861–65) unified charge, current and light. The lab computes fields, induction, Poynting flux and the electromagnetic wave in SI. This sheet (EMG-31 — Electric dipole p) is the form associated with Electric dipole p. Working symbols: qq, dd →\rightarrow pp. Separated-charge dipole. Pedagogical SI sheet with a live model and a swept parameter.

Purpose

Purpose: compute pp from qq, dd in Electromagnetism via p=qdp=q d Separated-charge dipole. Use it when a real electromagnetism question must be answered in SI before a code check.

Live realistic example

In symbols

Live case. Given q=1.000 nCq = 1.000\,\mathrm{nC}, d=2.000 mmd = 2.000\,\mathrm{mm}, the governing relation p=qdp=q d yields p=2.000 pC⋅mp = 2.000\,\mathrm{pC·m}. One governing identity, SI units, a single sweep on the sheet. Move a slider: the numbers are this situation, not a canned story.

Calculator

Inputs

Outputs

  • Electric dipole p p2.000 pC·m
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EMG-31 · gauge
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Narration of this film

One governing identity, SI units, a single sweep on the sheet.

Separated-charge dipole. Pedagogical SI sheet with a live model and a swept parameter.

Reading speed

Watch on YouTube