5318:
5355:
3302:
5317:
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5698:
situation is analyzed in the article, in which, when writing the integral equations of the electromagnetic field in a four-dimensional covariant form, in the
Faraday’s law the total time derivative of the magnetic flux through the circuit appears instead of the partial time derivative. Thus, electromagnetic induction appears either when the magnetic field changes over time or when the area of the circuit changes. From the physical point of view, it is better to speak not about the induction emf, but about the induced electric field strength
1102:
135:
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958:
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1005:
107:) describes the fact that a spatially varying (and also possibly time-varying, depending on how a magnetic field varies in time) electric field always accompanies a time-varying magnetic field, while Faraday's law states that there is emf (electromotive force, defined as electromagnetic work done on a unit charge when it has traveled one round of a conductive loop) on a conductive loop when the magnetic flux through the surface enclosed by the loop varies in time.
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4848:{\displaystyle (\mathbf {v} \times \mathbf {B} )\cdot \mathrm {d} \mathbf {l} =((\mathbf {v} _{t}+\mathbf {v} _{l})\times \mathbf {B} )\cdot \mathrm {d} \mathbf {l} =(\mathbf {v} _{t}\times \mathbf {B} +\mathbf {v} _{l}\times \mathbf {B} )\cdot \mathrm {d} \mathbf {l} =(\mathbf {v} _{l}\times \mathbf {B} )\cdot \mathrm {d} \mathbf {l} }
4073:{\displaystyle \left.{\frac {\mathrm {d} \Phi _{B}}{\mathrm {d} t}}\right|_{t=t_{0}}=\left(-\oint _{\partial \Sigma (t_{0})}\mathbf {E} (t_{0})\cdot \mathrm {d} \mathbf {l} \right)+\left(-\oint _{\partial \Sigma (t_{0})}{\bigl (}\mathbf {v} _{\mathbf {l} }(t_{0})\times \mathbf {B} (t_{0}){\bigr )}\cdot \mathrm {d} \mathbf {l} \right)}
4424:
3017:{\displaystyle \left.{\frac {\mathrm {d} \Phi _{B}}{\mathrm {d} t}}\right|_{t=t_{0}}=\left(\int _{\Sigma (t_{0})}\left.{\frac {\partial \mathbf {B} }{\partial t}}\right|_{t=t_{0}}\cdot \mathrm {d} \mathbf {A} \right)+\left({\frac {\mathrm {d} }{\mathrm {d} t}}\int _{\Sigma (t)}\mathbf {B} (t_{0})\cdot \mathrm {d} \mathbf {A} \right)}
4082:
3585:
2225:
5258:
1943:
5563:{\displaystyle {\mathcal {E}}=\int _{\partial \Sigma }(\mathbf {E} +\mathbf {v} _{m}\times \mathbf {B} )\cdot \mathrm {d} \mathbf {l} =-\int _{\Sigma }{\frac {\partial \mathbf {B} }{\partial t}}\cdot \mathrm {d} \Sigma +\oint _{\partial \Sigma }(\mathbf {v} _{m}\times \mathbf {B} )\cdot \mathrm {d} \mathbf {l} }
2759:
2626:
3037:
7106:
Note that the law relating flux to emf, which this article calls "Faraday's law", is referred to in
Griffiths' terminology as the "universal flux rule". Griffiths uses the term "Faraday's law" to refer to what this article calls the "Maxwell–Faraday equation". So in fact, in the textbook, Griffiths'
6035:
The observable phenomenon here depends only on the relative motion of the conductor and the magnet, whereas the customary view draws a sharp distinction between the two cases in which either the one or the other of these bodies is in motion. For if the magnet is in motion and the conductor at rest,
6039:
But if the magnet is stationary and the conductor in motion, no electric field arises in the neighbourhood of the magnet. In the conductor, however, we find an electromotive force, to which in itself there is no corresponding energy, but which gives rise—assuming equality of relative motion in the
5697:
appearance by action of the magnetic force on the charges in the moving wire or in the circuit changing its area is unsatisfactory. As a matter of fact, the charges in the wire or in the circuit could be completely absent, will then the electromagnetic induction effect disappear in this case? This
5347:
drives a current along the conducting radius to the conducting rim, and from there the circuit completes through the lower brush and the axle supporting the disc. This device generates an emf and a current, although the shape of the "circuit" is constant and thus the flux through the circuit does
3570:{\displaystyle \mathrm {d} \Phi _{B}=\int \mathbf {B} \cdot \mathrm {d} \mathbf {A} _{\text{sweep}}=\int \mathbf {B} \cdot (\mathbf {v} _{\mathbf {l} }\mathrm {d} t\times \mathrm {d} \mathbf {l} )=-\int \mathrm {d} t\,\mathrm {d} \mathbf {l} \cdot (\mathbf {v} _{\mathbf {l} }\times \mathbf {B} )}
3033:
is any given fixed time. We will show that the first term on the right-hand side corresponds to transformer emf, the second to motional emf (from the magnetic
Lorentz force on charge carriers due to the motion or deformation of the conducting loop in the magnetic field). The first term on the
5302:
This statement, however, is not always true and the reason is not just from the obvious reason that emf is undefined in empty space when no conductor is present. As noted in the previous section, Faraday's law is not guaranteed to work unless the velocity of the abstract curve
4306:
6031:
It is known that
Maxwell's electrodynamics—as usually understood at the present time—when applied to moving bodies, leads to asymmetries which do not appear to be inherent in the phenomena. Take, for example, the reciprocal electrodynamic action of a magnet and a conductor.
2479:{\displaystyle \mathbf {E} _{s}(\mathbf {r} ,t)\approx -{\frac {1}{4\pi }}\iiint _{V}\ {\frac {\left({\frac {\partial \mathbf {B} (\mathbf {r} ',t)}{\partial t}}\right)\times \left(\mathbf {r} -\mathbf {r} '\right)}{|\mathbf {r} -\mathbf {r} '|^{3}}}d^{3}\mathbf {r'} }
4524:
2126:
5115:
6043:
Examples of this sort, together with unsuccessful attempts to discover any motion of the earth relative to the "light medium," suggest that the phenomena of electrodynamics as well as of mechanics possess no properties corresponding to the idea of absolute rest.
3297:
3340:
The proof of this is a little more difficult than the first term; more details and alternate approaches for the proof can be found in the references. As the loop moves and/or deforms, it sweeps out a surface (see the right figure). As a small part of the loop
4981:
are along the same direction. Now we can see that, for the conductive loop, emf is same to the time-derivative of the magnetic flux through the loop except for the sign on it. Therefore, we now reach the equation of
Faraday's law (for the conductive loop) as
2648:
2515:
4290:{\displaystyle \left.{\frac {\mathrm {d} \Phi _{B}}{\mathrm {d} t}}\right|_{t=t_{0}}=-\oint _{\partial \Sigma (t_{0})}{\bigl (}\mathbf {E} (t_{0})+\mathbf {v} _{\mathbf {l} }(t_{0})\times \mathbf {B} (t_{0}){\bigr )}\cdot \mathrm {d} \mathbf {l} .}
5158:
3772:{\displaystyle {\frac {\mathrm {d} }{\mathrm {d} t}}\int _{\Sigma (t)}\mathbf {B} (t_{0})\cdot \mathrm {d} \mathbf {A} =-\oint _{\partial \Sigma (t_{0})}(\mathbf {v} _{\mathbf {l} }(t_{0})\times \mathbf {B} (t_{0}))\cdot \mathrm {d} \mathbf {l} }
1849:
1443:
Faraday's law contains the information about the relationships between both the magnitudes and the directions of its variables. However, the relationships between the directions are not explicit; they are hidden in the mathematical formula.
110:
Faraday's law had been discovered and one aspect of it (transformer emf) was formulated as the
Maxwell–Faraday equation later. The equation of Faraday's law can be derived by the Maxwell–Faraday equation (describing transformer emf) and the
1237:
5759:
1756:
992:
Within two months, Faraday had found several other manifestations of electromagnetic induction. For example, he saw transient currents when he quickly slid a bar magnet in and out of a coil of wires, and he generated a steady
6462:
1639:
1383:
1302:, defined as the energy available from a unit charge that has traveled once around the wire loop. (Although some sources state the definition differently, this expression was chosen for compatibility with the equations of
5041:
1448:
5634:
So the "flux rule" that the emf in a circuit is equal to the rate of change of the magnetic flux through the circuit applies whether the flux changes because the field changes or because the circuit moves (or both) ...
3201:{\displaystyle \int _{\Sigma (t_{0})}\left.{\frac {\partial \mathbf {B} }{\partial t}}\right|_{t=t_{0}}\cdot \mathrm {d} \mathbf {A} =-\oint _{\partial \Sigma (t_{0})}\mathbf {E} (t_{0})\cdot \mathrm {d} \mathbf {l} }
1030:, who in 1861–62 used Faraday's ideas as the basis of his quantitative electromagnetic theory. In Maxwell's papers, the time-varying aspect of electromagnetic induction is expressed as a differential equation which
7008:
This example of
Faraday's Law makes it very clear that in the case of extended bodies care must be taken that the boundary used to determine the flux must not be stationary but must be moving with respect to the
4455:
1079:
Alternating electric current flows through the solenoid on the left, producing a changing magnetic field. This field causes, by electromagnetic induction, an electric current to flow in the wire loop on the
3213:
115:(describing motional emf). The integral form of the Maxwell–Faraday equation describes only the transformer emf, while the equation of Faraday's law describes both the transformer emf and the motional emf.
5153:
6489:"71 years earlier, this scientist beat Einstein to relativity - Michael Faraday's 1834 law of induction was the key experiment behind the eventual discovery of relativity. Einstein admitted it himself"
5823:
3393:(note that this vector is toward out from the display in the right figure). Therefore, the change of the magnetic flux through the loop due to the deformation or movement of the loop over the time
4896:
989:
that occurred when the battery was connected and disconnected. His notebook entry also noted that fewer wraps for the battery side resulted in a greater disturbance of the galvanometer's needle.
4419:{\displaystyle {\frac {\mathrm {d} \Phi _{B}}{\mathrm {d} t}}=-\oint _{\partial \Sigma }\left(\mathbf {E} +\mathbf {v} _{\mathbf {l} }\times \mathbf {B} \right)\cdot \mathrm {d} \mathbf {l} .}
5046:
5913:
in K’ is considered as a result of the induction effect in the moving circuit, regardless of whether the charges are present in the circuit or not. In the conducting circuit, the field
2630:(by definition). This total time derivative can be evaluated and simplified with the help of the Maxwell–Faraday equation and some vector identities; the details are in the box below:
1056:
in 1834, describes "flux through the circuit", and gives the direction of the induced emf and current resulting from electromagnetic induction (elaborated upon in the examples below).
5360:
A wire (solid red lines) connects to two touching metal plates (silver) to form a circuit. The whole system sits in a uniform magnetic field, normal to the page. If the abstract path
4979:
4923:
4634:
4448:
In the case of a conductive loop, emf (Electromotive Force) is the electromagnetic work done on a unit charge when it has traveled around the loop once, and this work is done by the
5987:
5364:
follows the primary path of current flow (marked in red), then the magnetic flux through this path changes dramatically as the plates are rotated, yet the emf is almost zero. After
2220:{\displaystyle \oint _{\partial \Sigma }\mathbf {E} \cdot \mathrm {d} \mathbf {l} =-{\frac {\mathrm {d} }{\mathrm {d} t}}\int _{\Sigma }\mathbf {B} \cdot \mathrm {d} \mathbf {A} .}
1492:
It is possible to find out the direction of the electromotive force (emf) directly from
Faraday’s law, without invoking Lenz's law. A left hand rule helps doing that, as follows:
1162:
5253:{\textstyle \oint \left(\mathbf {v} \times \mathbf {B} \right)\cdot \mathrm {d} \mathbf {l} =\oint \left(\mathbf {v} _{l}\times \mathbf {B} \right)\cdot \mathrm {d} \mathbf {l} }
6670:
6036:
there arises in the neighbourhood of the magnet an electric field with a certain definite energy, producing a current at the places where parts of the conductor are situated.
4952:
965:
Faraday's notebook on August 29, 1831 describes an experimental demonstration of electromagnetic induction (see figure) that wraps two wires around opposite sides of an iron
5957:
4548:
1938:{\displaystyle \oint _{\partial \Sigma }\mathbf {E} \cdot \mathrm {d} \mathbf {l} =-\int _{\Sigma }{\frac {\partial \mathbf {B} }{\partial t}}\cdot \mathrm {d} \mathbf {A} }
1407:
5847:
is the vector potential. If the circuit area is changing in case of the constant magnetic field, then some part of the circuit is inevitably moving, and the electric field
5307:
matches the actual velocity of the material conducting the electricity. The two examples illustrated below show that one often obtains incorrect results when the motion of
6009:
5933:
5911:
5889:
5867:
5845:
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5376:
moves with the same velocity as the material. Alternatively, one can always correctly calculate the emf by combining
Lorentz force law with the Maxwell–Faraday equation:
6452:
6526:
Faraday's Law, which states that the electromotive force around a closed path is equal to the negative of the time rate of change of magnetic flux enclosed by the path.
977:
suggested that when current started to flow in one wire, a sort of wave would travel through the ring and cause some electrical effect on the opposite side. Indeed, a
1580:
1324:
4985:
2754:{\displaystyle {\frac {\mathrm {d} \Phi _{B}}{\mathrm {d} t}}={\frac {\mathrm {d} }{\mathrm {d} t}}\int _{\Sigma (t)}\mathbf {B} (t)\cdot \mathrm {d} \mathbf {A} }
2621:{\displaystyle {\frac {\mathrm {d} \Phi _{B}}{\mathrm {d} t}}={\frac {\mathrm {d} }{\mathrm {d} t}}\int _{\Sigma (t)}\mathbf {B} (t)\cdot \mathrm {d} \mathbf {A} }
5701:
6201:
1116:
of magnitude equal to the area of the element and with direction normal to the element and pointing "outward" (with respect to the orientation of the surface).
692:
1705:
7488:
665:
2636:
Consider the time-derivative of magnetic flux through a closed boundary (loop) that can move or be deformed. The area bounded by the loop is denoted as
677:
7263:
5667:
We know of no other place in physics where such a simple and accurate general principle requires for its real understanding an analysis in terms of
6498:
2763:
The integral can change over time for two reasons: The integrand can change, or the integration region can change. These add linearly, therefore:
1026:. However, scientists at the time widely rejected his theoretical ideas, mainly because they were not formulated mathematically. An exception was
33:), creating a magnetic field. When the coils are stationary, no current is induced. But when the small coil is moved in or out of the large coil (
1695:
The
Maxwell–Faraday equation states that a time-varying magnetic field always accompanies a spatially varying (also possibly time-varying), non-
7248:
7483:
2040:
is defined by the right-hand rule as one that points with the fingers of the right hand when the thumb points in the direction of the normal
1556:
is negative, the direction of the electromotive force is opposite to the direction of the curved fingers (opposite to the yellow arrowheads).
5580:
and (2) in general, the partial derivative with respect to time cannot be moved outside the integral since the area is a function of time."
6281:
7254:
7281:
5869:
emerges in this part of the circuit in the comoving reference frame K’ as a result of the Lorentz transformation of the magnetic field
5260:
is for the motional emf (due to the magnetic Lorentz force on charges by the motion or deformation of the loop in the magnetic field).
928:
697:
6886:
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two cases discussed—to electric currents of the same path and intensity as those produced by the electric forces in the former case.
707:
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changes, or because the wire loop is moved or deformed, or both—Faraday's law of induction says that the wire loop acquires an
532:
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6861:
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6149:
547:
542:
169:
5627:. In the latter half of Part II of that paper, Maxwell gives a separate physical explanation for each of the two phenomena.
4519:{\displaystyle {\mathcal {E}}=\oint \left(\mathbf {E} +\mathbf {v} \times \mathbf {B} \right)\cdot \mathrm {d} \mathbf {l} }
981:'s needle measured a transient current (which he called a "wave of electricity") on the right side's wire when he connected
7430:
5630:
A reference to these two aspects of electromagnetic induction is made in some modern textbooks. As Richard Feynman states:
4858:
1034:
referred to as Faraday's law even though it is different from the original version of Faraday's law, and does not describe
557:
5573:
where "it is very important to notice that (1) is the velocity of the conductor ... not the velocity of the path element
5589:
5110:{\textstyle {\mathcal {E}}=\oint \left(\mathbf {E} +\mathbf {v} \times \mathbf {B} \right)\cdot \mathrm {d} \mathbf {l} }
3292:{\displaystyle {\frac {\mathrm {d} }{\mathrm {d} t}}\int _{\Sigma (t)}\mathbf {B} (t_{0})\cdot \mathrm {d} \mathbf {A} }
7369:
7223:
7098:
6968:
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6553:
159:
427:
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921:
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164:
37:), the magnetic flux through the large coil changes, inducing a current which is detected by the galvanometer (
6488:
5604:
4957:
4901:
4612:
2497:(including the Maxwell–Faraday equation), along with Lorentz force law, are a sufficient foundation to derive
7463:
7309:
6560:
The magnetic flux is that flux which passes through any and every surface whose perimeter is the closed path.
702:
6915:
Davison, M. E. (1973). "A Simple Proof that the Lorentz Force, Law Implied Faraday's Law of Induction, when
5962:
6386:
6227:
5891:, present in the stationary reference frame K, which passes through the circuit. The presence of the field
1075:
567:
307:
174:
7409:
5288:
is any arbitrary closed loop in space whatsoever, then the total time derivative of magnetic flux through
297:
5935:
causes motion of the charges. In the reference frame K, it looks like appearance of emf of the induction
860:
735:
632:
607:
527:
6401:
3301:
1479:
is positive, the direction of the emf is the same as that of the curved fingers (yellow arrowheads). If
1088:
The electromotive force around a closed path is equal to the negative of the time rate of change of the
6402:"Ueber die Bestimmung der Richtung der durch elektodynamische Vertheilung erregten galvanischen Ströme"
5623:
2502:
1832:
360:
4928:
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2076:
is different from the behavior of the electric field generated by static charges. A charge-generated
2017:
1840:
1696:
914:
875:
402:
392:
332:
327:
267:
73:
5938:
4529:
1544:, is positive, the curved fingers show the direction of the electromotive force (yellow arrowheads).
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412:
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5992:
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5894:
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5850:
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5764:
845:
347:
5638:
Yet in our explanation of the rule we have used two completely distinct laws for the two cases –
2253:
1285:. In more visual terms, the magnetic flux through the wire loop is proportional to the number of
725:
252:
242:
237:
7090:
7084:
6618:
6612:
850:
820:
7044:
6545:
6539:
6294:
6079:
5761:, that occurs in the circuit when the magnetic flux changes. In this case, the contribution to
2494:
1828:
1447:
1043:
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442:
217:
104:
7189:
6958:
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1232:{\displaystyle \Phi _{B}=\iint _{\Sigma (t)}\mathbf {B} (t)\cdot \mathrm {d} \mathbf {A} \,,}
1137:
770:
457:
447:
397:
387:
5754:{\textstyle \mathbf {E} =-\nabla {\mathcal {E}}-{\frac {\partial \mathbf {A} }{\partial t}}}
7151:
6928:
6736:
6685:
6413:
4565:
consists of two components in average; one is the velocity of the charge along the segment
1306:.) Equivalently, it is the voltage that would be measured by cutting the wire to create an
970:
895:
795:
760:
512:
377:
277:
262:
197:
89:
3034:
right-hand side can be rewritten using the integral form of the Maxwell–Faraday equation:
134:
8:
7209:
7053:
7039:
6988:(5th ed.). Berlin: VEB Deutscher Verlag der Wissenschaften. eq. 20, p. 47.
6727:
5618:
5324:
5275:
1437:
1410:
1299:
1144:
1027:
1013:
998:
997:) current by rotating a copper disk near the bar magnet with a sliding electrical lead ("
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477:
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302:
69:
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7213:
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2256:
of the overall electric field, can be approximated in the non-relativistic limit by the
985:
disconnected the left side's wire to a battery. This induction was due to the change in
7399:
7167:
7141:
7065:
6774:
6024:
1995:
to that surface patch, the magnitude is the area of an infinitesimal patch of surface.
1770:
1751:{\displaystyle \nabla \times \mathbf {E} =-{\frac {\partial \mathbf {B} }{\partial t}}}
1303:
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470:
272:
232:
552:
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790:
7130:"On the Covariant Representation of Integral Equations of the Electromagnetic Field"
2505:. Therefore, it is possible to "prove" Faraday's law starting with these equations.
1470:, and the normal n to that area, as represented by the fingers of the left hand. If
1460:, the change in flux, is found based on the relationship between the magnetic field
7468:
7458:
7404:
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7057:
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6744:
6693:
6421:
2228:
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1436:
The laws of induction of electric currents in mathematical form was established by
1307:
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6453:"Relativity Wasn't Einstein's Miracle; It Was Waiting In Plain Sight For 71 Years"
6115:
5611:
generated by an electric force due to a changing magnetic field (described by the
1517:, the change in flux. Determine the initial and final fluxes (whose difference is
7379:
7374:
7325:
7185:
6139:
6094:
6089:
6049:
6020:
5269:
2257:
2013:
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487:
452:
312:
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25:
Faraday's experiment showing induction between coils of wire: The liquid battery
1101:
865:
7473:
7344:
5337:(which direction is along the disk surface normal). The magnetic Lorentz force
3579:
2508:
The starting point is the time-derivative of flux through an arbitrary surface
1811:
1792:
1634:{\displaystyle {\mathcal {E}}=-N{\frac {\mathrm {d} \Phi _{B}}{\mathrm {d} t}}}
1378:{\displaystyle {\mathcal {E}}=-{\frac {\mathrm {d} \Phi _{B}}{\mathrm {d} t}},}
1121:
1023:
994:
974:
785:
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61:
53:
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6019:
Reflection on this apparent dichotomy was one of the principal paths that led
5036:{\displaystyle {\frac {\mathrm {d} \Phi _{B}}{\mathrm {d} t}}=-{\mathcal {E}}}
7531:
7414:
7289:
6871:
6697:
6425:
6375:. Vol. 2 (3rd ed.). Oxford University Press. pp. 178–179, 189.
6144:(4th ed.). New York & Oxford: Oxford University Press. p. 386.
2232:
2056:
1969:
1430:
1423:
1125:
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522:
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Faraday's law is a single equation describing two different phenomena: the
2083:
978:
951:
880:
775:
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682:
617:
537:
502:
382:
257:
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does not contribute to the work done on the charge since the direction of
954:
in 1832. Faraday was the first to publish the results of his experiments.
7364:
7277:
Notes from Physics and Astronomy HyperPhysics at Georgia State University
5331:, sweeping the conducting radius circularly in the static magnetic field
1275:
1247:
1004:
957:
800:
652:
482:
144:
77:
6074:
1992:
1286:
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21:
6940:
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5155:
is for the transformer emf (due to a time-varying magnetic field) and
1496:
Align the curved fingers of the left hand with the loop (yellow line).
1109:
into small surface elements. Each element is associated with a vector
7218:. Oxford: Clarendon Press. ch. III, sec. 530, p. 178.
7117:
The Feynman Lectures on Physics Vol. II Ch. 17: The Laws of Induction
6493:
6084:
1311:
1053:
840:
815:
627:
149:
6117:
Magnetism and Electricity: A manual for students in advanced classes
1664:
7146:
2252:
The electric vector field induced by a changing magnetic flux, the
1762:
1561:
1499:
Stretch your thumb. The stretched thumb indicates the direction of
1105:
The definition of surface integral relies on splitting the surface
592:
587:
207:
93:
81:
7294:
6120:. London and New York: Longmans, Green, & Co. Fig. 248, p. 245
5688:
1067:
theory was presented by this law of induction by Faraday in 1834.
1042:) is the form recognized today in the group of equations known as
6314:
The philosopher's tree: a selection of Michael Faraday's writings
5372:
One can analyze examples like these by taking care that the path
562:
7089:(3rd ed.). Upper Saddle River, NJ: Prentice Hall. pp.
6617:(3rd ed.). Upper Saddle River, NJ: Prentice Hall. pp.
1699:
electric field, and vice versa. The Maxwell–Faraday equation is
1488:
is negative, the direction of the emf is against the arrowheads.
7243:
6457:
5783:
from the change in the magnetic field is made through the term
1147:
is the given loop. Since the wire loop may be moving, we write
647:
154:
1022:
explained electromagnetic induction using a concept he called
7359:
5148:{\textstyle \oint \mathbf {E} \cdot \mathrm {d} \mathbf {l} }
4559:
In a macroscopic view, for charges on a segment of the loop,
966:
6767:"Bypassing Lenz's Rule - A Left Hand Rule for Faraday's Law"
6513:
4088:
3809:
3069:
2864:
2772:
7255:
A simple interactive tutorial on electromagnetic induction
2231:
at the right-hand side is the explicit expression for the
1831:, and therefore plays a fundamental role in the theory of
1668:
An illustration of the Kelvin–Stokes theorem with surface
946:
Electromagnetic induction was discovered independently by
5818:{\textstyle -{\frac {\partial \mathbf {A} }{\partial t}}}
3210:
Next, we analyze the second term on the right-hand side:
7129:
5603:
generated by a magnetic force on a moving wire (see the
2123:
is not changing in time, the equation can be rewritten:
6671:"Allgemeine Gesetze der inducirten elektrischen Ströme"
5989:, taken along the circuit, seems to generate the field
1317:
Faraday's law states that the emf is also given by the
29:
provides a current which flows through the small coil (
5789:
5704:
5161:
5123:
5049:
1814:. These fields can generally be functions of position
5995:
5965:
5941:
5919:
5897:
5875:
5853:
5831:
5767:
5385:
5280:
It is tempting to generalize Faraday's law to state:
4988:
4960:
4931:
4904:
4891:{\displaystyle (\mathbf {v} _{t}\times \mathbf {B} )}
4861:
4642:
4615:
4532:
4458:
4309:
4085:
3806:
3588:
3406:
3216:
3040:
2769:
2651:
2518:
2266:
2129:
1852:
1708:
1583:
1505:(brown), the normal to the area enclosed by the loop.
1429:
The direction of the electromotive force is given by
1391:
1327:
1165:
1084:
The most widespread version of Faraday's law states:
7489:
Institute of Physics Michael Faraday Medal and Prize
6206:(5th ed.). Pearson:Prentice Hall. p. 255.
2012:
have a sign ambiguity; to get the correct sign, the
973:). His assessment of newly-discovered properties of
6856:. 4 (Fourth ed.). Cambridge University Press.
6431:A partial translation of the paper is available in
6353:
6255:
6003:
5981:
5951:
5927:
5905:
5883:
5861:
5839:
5817:
5775:
5753:
5562:
5252:
5147:
5109:
5035:
4973:
4946:
4917:
4890:
4847:
4628:
4542:
4518:
4418:
4289:
4072:
3771:
3569:
3291:
3200:
3016:
2753:
2620:
2478:
2219:
1937:
1750:
1633:
1401:
1377:
1231:
6437:. Cambridge, MA: Harvard Press. pp. 511–513.
7529:
7215:A treatise on electricity and magnetism, Vol. II
6389:. The Institution of Engineering and Technology.
6282:"Faraday's notebooks: Electromagnetic Induction"
2644:), then the time-derivative can be expressed as
1827:The Maxwell–Faraday equation is one of the four
1451:A Left Hand Rule for Faraday's Law. The sign of
6891:. Mineola, NY: Dover Publications. p. 56.
5689:Explanation based on four-dimensional formalism
5583:
4576:, and the other is the velocity of the segment
7019:
7017:
6795:
6232:Member Directory, National Academy of Sciences
5621:drew attention to this fact in his 1861 paper
1985:is an infinitesimal vector element of surface
1063:, much of the groundwork and discovery of his
7484:Royal Society of London Michael Faraday Prize
7310:
7268:– Highly animated lecture, with sound effects
7208:
7107:statement is about the "universal flux rule".
7038:
6960:Basic Theoretical Physics: A Concise Overview
6606:
6604:
6519:
6441:
6370:
6304:
5612:
5311:is divorced from the motion of the material.
4266:
4181:
4047:
3986:
2082:-field can be expressed as the gradient of a
1039:
922:
6845:
6843:
6524:(2nd ed.). Prentice-Hall. p. 100.
1654:is the magnetic flux through a single loop.
76:, is the fundamental operating principle of
7023:
7014:
6888:Introduction to electromagnetic engineering
6720:
6716:
6714:
6641:
6531:
6522:Electromagnetic Waves and Radiating Systems
6477:
6347:
6345:
6343:
6341:
6166:"Applications of electromagnetic induction"
4445:is the velocity of a part of the boundary.
1954:is a surface bounded by the closed contour
1657:
7317:
7303:
7076:
6997:
6995:
6910:
6908:
6884:
6878:
6601:
6578:
6576:
6574:
6572:
6570:
6568:
6520:Jordan, Edward; Balmain, Keith G. (1968).
6310:
6249:
6247:
2512:(that can be moved or deformed) in space:
1155:for the surface. The magnetic flux is the
929:
915:
133:
7190:"On the Electrodynamics of Moving Bodies"
7145:
7082:
6849:
6840:
6610:
6585:"The Feynman Lectures on Physics Vol. II"
3525:
1577:, Faraday's law of induction states that
1278:representing the element of flux through
1225:
1096:
7230:a treatise on electricity and magnetism.
6956:
6711:
6351:
6338:
6311:Faraday, Michael; Day, P. (1999-02-01).
6253:
6203:Fundamentals of applied electromagnetics
6131:
5693:In the general case, explanation of the
4974:{\displaystyle \mathrm {d} \mathbf {l} }
4918:{\displaystyle \mathrm {d} \mathbf {l} }
4629:{\displaystyle \mathrm {d} \mathbf {l} }
3366:, it sweeps out an area whose vector is
3300:
1663:
1446:
1100:
1074:
1003:
956:
20:
7266:Induction: Faraday's law and Lenz's law
7259:National High Magnetic Field Laboratory
7257:(click and drag magnet back and forth)
7134:Progress in Electromagnetics Research C
7127:
6992:
6983:
6952:
6950:
6914:
6905:
6796:Whelan, P. M.; Hodgeson, M. J. (1978).
6668:
6565:
6387:"Archives Biographies: Michael Faraday"
6373:A Treatise on Electricity and Magnetism
6279:
6244:
6055:On the Electrodynamics of Moving Bodies
5959:, the gradient of which in the form of
3305:The area swept out by a vector element
678:Electromagnetism and special relativity
7530:
7042:(1861). "On physical lines of force".
6483:
6447:
6290:The Royal Institution of Great Britain
6137:
6113:
5982:{\displaystyle -\nabla {\mathcal {E}}}
4430:is the boundary (loop) of the surface
3790:is the velocity of a part of the loop
1532:, as indicated by the stretched thumb.
7298:
7272:Electricity and Magnetism course page
6544:(5th ed.). McGraw-Hill. p.
6432:
6379:
6258:Physics: Principles with Applications
6199:
6184:"A Brief History of Electromagnetism"
5327:. The disc rotates with angular rate
2016:is used, as explained in the article
1843:, thereby reproducing Faraday's law:
698:Maxwell equations in curved spacetime
7431:Royal Institution Christmas Lectures
7184:
7024:Hughes, W. F.; Young, F. J. (1965).
6947:
6723:"A Left Hand Rule for Faraday's Law"
6645:Physics for Scientists and Engineers
6537:
6399:
6275:
6273:
3580:identities of triple scalar products
2090:, and has a zero path integral. See
1568:identical turns, each with the same
7324:
7026:The Electromagnetodynamics of Fluid
7004:Intermediate Electromagnetic Theory
7001:
6582:
5590:Moving magnet and conductor problem
3800:Putting these together results in,
2114:for which that path is a boundary.
1948:where, as indicated in the figure,
1645:is the number of turns of wire and
13:
7202:
6977:
6014:
5974:
5969:
5944:
5806:
5796:
5742:
5732:
5721:
5716:
5551:
5516:
5513:
5502:
5498:
5485:
5475:
5467:
5447:
5404:
5401:
5388:
5241:
5192:
5136:
5098:
5052:
5028:
5010:
4998:
4993:
4962:
4906:
4836:
4794:
4729:
4666:
4617:
4535:
4507:
4461:
4452:. Therefore, emf is expressed as
4404:
4355:
4352:
4331:
4319:
4314:
4275:
4158:
4155:
4111:
4099:
4094:
4056:
3963:
3960:
3930:
3884:
3881:
3832:
3820:
3815:
3760:
3675:
3672:
3652:
3613:
3598:
3592:
3527:
3518:
3496:
3485:
3437:
3413:
3408:
3280:
3241:
3226:
3220:
3189:
3143:
3140:
3120:
3084:
3074:
3046:
3000:
2961:
2946:
2940:
2915:
2879:
2869:
2841:
2795:
2783:
2778:
2742:
2710:
2695:
2689:
2673:
2661:
2656:
2609:
2577:
2562:
2556:
2540:
2528:
2523:
2372:
2340:
2205:
2191:
2176:
2170:
2152:
2138:
2135:
2097:The integral equation is true for
1926:
1913:
1903:
1895:
1875:
1861:
1858:
1739:
1729:
1709:
1621:
1609:
1604:
1586:
1394:
1362:
1350:
1345:
1330:
1216:
1184:
1167:
1035:
14:
7559:
7290:A free simulation on motional emf
7236:
7028:. John Wiley. Eq. (2.6–13) p. 53.
6501:from the original on 28 June 2023
6270:
4587:(the loop is deformed or moved).
72:(emf). This phenomenon, known as
7512:
7511:
7494:Faraday Medal (electrochemistry)
7437:The Chemical History of a Candle
7242:
6820:
6764:
6465:from the original on 3 July 2023
5997:
5921:
5899:
5877:
5855:
5833:
5800:
5769:
5736:
5706:
5594:
5556:
5540:
5526:
5479:
5452:
5436:
5422:
5413:
5353:
5316:
5246:
5228:
5214:
5197:
5179:
5171:
5141:
5128:
5103:
5085:
5077:
5069:
4967:
4947:{\displaystyle \mathbf {v} _{t}}
4934:
4911:
4881:
4867:
4841:
4825:
4811:
4799:
4783:
4769:
4760:
4746:
4734:
4718:
4701:
4686:
4671:
4655:
4647:
4622:
4512:
4494:
4486:
4478:
4409:
4391:
4381:
4375:
4366:
4280:
4244:
4218:
4212:
4187:
4061:
4025:
3999:
3993:
3935:
3906:
3765:
3733:
3707:
3701:
3657:
3628:
3560:
3550:
3544:
3532:
3501:
3478:
3472:
3460:
3443:
3429:
3326:when it has moved with velocity
3285:
3256:
3194:
3165:
3125:
3078:
3005:
2976:
2920:
2873:
2747:
2725:
2614:
2592:
2468:
2433:
2424:
2403:
2394:
2353:
2344:
2283:
2269:
2210:
2197:
2157:
2144:
1931:
1907:
1880:
1867:
1733:
1716:
1221:
1199:
1070:
7178:
7121:
7110:
7086:Introduction to Electrodynamics
7032:
6853:Introduction to Electrodynamics
6814:
6798:Essential Principles of Physics
6789:
6758:
6662:
6635:
6614:Introduction to Electrodynamics
6393:
6364:
6280:Faraday, Michael (1831-08-29).
6114:Poyser, Arthur William (1892).
5679:The Feynman Lectures on Physics
5117:. With breaking this integral,
2108:through space, and any surface
1835:. It can also be written in an
7370:Faraday's laws of electrolysis
6220:
6193:
6176:
6158:
6107:
5952:{\displaystyle {\mathcal {E}}}
5544:
5521:
5440:
5409:
4885:
4862:
4829:
4806:
4787:
4741:
4722:
4711:
4681:
4678:
4659:
4643:
4543:{\displaystyle {\mathcal {E}}}
4261:
4248:
4237:
4224:
4204:
4191:
4174:
4161:
4042:
4029:
4018:
4005:
3979:
3966:
3923:
3910:
3900:
3887:
3753:
3750:
3737:
3726:
3713:
3696:
3691:
3678:
3645:
3632:
3622:
3616:
3564:
3539:
3505:
3467:
3273:
3260:
3250:
3244:
3182:
3169:
3159:
3146:
3062:
3049:
2993:
2980:
2970:
2964:
2857:
2844:
2735:
2729:
2719:
2713:
2602:
2596:
2586:
2580:
2443:
2419:
2367:
2348:
2293:
2279:
1972:vector element of the contour
1402:{\displaystyle {\mathcal {E}}}
1292:When the flux changes—because
1209:
1203:
1193:
1187:
1040:Maxwell–Faraday equation below
1:
7464:Faraday Building (Manchester)
7395:Faraday's ice pail experiment
6957:Krey; Owen (14 August 2007).
6885:Harrington, Roger F. (2003).
6800:(2nd ed.). John Murray.
6669:Neumann, Franz Ernst (1846).
6406:Annalen der Physik und Chemie
6371:Clerk Maxwell, James (1904).
6254:Giancoli, Douglas C. (1998).
6101:
5263:
4556:is the unit charge velocity.
1526:) with respect to the normal
703:Relativistic electromagnetism
16:Basic law of electromagnetism
7083:Griffiths, David J. (1999).
6850:Griffiths, David J. (2017).
6771:www.PhysicsForArchitects.com
6611:Griffiths, David J. (1999).
6541:Engineering Electromagnetics
6352:Williams, L. Pearce (1965).
6141:Elements of Electromagnetics
6004:{\displaystyle \mathbf {E} }
5928:{\displaystyle \mathbf {E} }
5906:{\displaystyle \mathbf {E} }
5884:{\displaystyle \mathbf {B} }
5862:{\displaystyle \mathbf {E} }
5840:{\displaystyle \mathbf {A} }
5776:{\displaystyle \mathbf {E} }
5584:Faraday's law and relativity
4609:is same to the direction of
1289:that pass through the loop.
961:Faraday's 1831 demonstration
7:
7128:Fedosin, Sergey G. (2019).
6986:Theoretische Elektrotechnik
6921:American Journal of Physics
6589:feynmanlectures.caltech.edu
6062:
5366:Feynman Lectures on Physics
2070:. A nonzero circulation of
1264:is the magnetic field, and
1038:. Heaviside's version (see
10:
7564:
7340:Faraday's law of induction
7249:Faraday's law of induction
6829:. Georgia State University
6648:. Macmillan. p. 795.
5624:On Physical Lines of Force
5587:
5273:
5267:
2503:classical electromagnetism
2026:, a positive path element
1833:classical electromagnetism
1008:Faraday's disk, the first
941:
428:Liénard–Wiechert potential
46:Faraday's law of induction
7507:
7499:Faraday Lectureship Prize
7446:
7423:
7385:Faraday-efficiency effect
7332:
7284:Introducing Faraday's law
7062:10.1080/14786431003659180
6963:. Springer. p. 155.
6317:. CRC Press. p. 71.
6262:(5th ed.). pp.
6138:Sadiku, M. N. O. (2007).
693:Mathematical descriptions
403:Electromagnetic radiation
393:Electromagnetic induction
333:Magnetic vector potential
328:Magnetic scalar potential
74:electromagnetic induction
7517:Category:Michael Faraday
7454:Michael Faraday Memorial
6698:10.1002/andp.18461430103
6435:A Source Book in Physics
6426:10.1002/andp.18341073103
6360:. New York, Basic Books.
5648:for "circuit moves" and
5613:Maxwell–Faraday equation
2488:
1658:Maxwell–Faraday equation
1120:For a loop of wire in a
101:Maxwell–Faraday equation
5669:two different phenomena
2020:. For a planar surface
1535:If the change in flux,
1466:, the area of the loop
243:Electrostatic induction
238:Electrostatic discharge
7282:Tankersley and Mosca:
7045:Philosophical Magazine
6919:is Time Independent".
6642:Tipler; Mosca (2004).
6538:Hayt, William (1989).
6200:Ulaby, Fawwaz (2007).
6060:
6005:
5983:
5953:
5929:
5907:
5885:
5863:
5841:
5819:
5777:
5755:
5684:
5564:
5294:equals the emf around
5254:
5149:
5111:
5037:
4975:
4948:
4919:
4892:
4849:
4630:
4544:
4520:
4420:
4291:
4074:
3773:
3571:
3338:
3293:
3202:
3018:
2755:
2622:
2480:
2221:
2086:that is a solution to
1939:
1752:
1692:
1635:
1489:
1403:
1379:
1321:of the magnetic flux:
1250:of the moving surface
1233:
1117:
1097:Mathematical statement
1094:
1081:
1016:
962:
673:Electromagnetic tensor
64:will interact with an
42:
7164:10.2528/PIERC19062902
6433:Magie, W. M. (1963).
6029:
6006:
5984:
5954:
5930:
5908:
5886:
5864:
5842:
5820:
5778:
5756:
5664:for "field changes".
5632:
5588:Further information:
5565:
5348:not change with time.
5255:
5150:
5112:
5038:
4976:
4949:
4920:
4893:
4850:
4631:
4545:
4521:
4421:
4292:
4075:
3774:
3582:are used. Therefore,
3572:
3304:
3294:
3203:
3019:
2756:
2623:
2481:
2222:
2018:Kelvin–Stokes theorem
1940:
1841:Kelvin–Stokes theorem
1753:
1667:
1636:
1450:
1404:
1380:
1234:
1104:
1092:enclosed by the path.
1086:
1078:
1007:
960:
666:Covariant formulation
458:Synchrotron radiation
398:Electromagnetic pulse
388:Electromagnetic field
24:
7251:at Wikimedia Commons
7210:Clerk Maxwell, James
7054:Taylor & Francis
7040:Clerk Maxwell, James
6984:Simonyi, K. (1973).
6721:Yehuda Salu (2014).
6583:Feynman, Richard P.
5993:
5963:
5939:
5917:
5895:
5873:
5851:
5829:
5787:
5765:
5702:
5676:Richard P. Feynman,
5383:
5159:
5121:
5047:
4986:
4958:
4929:
4902:
4898:is perpendicular to
4859:
4640:
4613:
4530:
4456:
4307:
4083:
3804:
3586:
3404:
3348:moves with velocity
3214:
3038:
2767:
2649:
2516:
2264:
2254:solenoidal component
2127:
1850:
1706:
1581:
1560:For a tightly wound
1389:
1325:
1287:magnetic field lines
1163:
971:toroidal transformer
708:Stress–energy tensor
633:Reluctance (complex)
378:Displacement current
84:, and many types of
7548:Maxwell's equations
7156:2019arXiv191111138F
7002:Stewart, Joseph V.
6933:1973AmJPh..41..713D
6741:2014PhTea..52...48S
6728:The Physics Teacher
6690:1846AnP...143...31N
6418:1834AnP...107..483L
6400:Lenz, Emil (1834).
6080:Maxwell's equations
5619:James Clerk Maxwell
5325:homopolar generator
2495:Maxwell's equations
1991:. Its direction is
1829:Maxwell's equations
1438:Franz Ernst Neumann
1411:electromotive force
1136:is defined for any
1044:Maxwell's equations
1028:James Clerk Maxwell
1014:homopolar generator
623:Magnetomotive force
508:Electromotive force
478:Alternating current
413:Jefimenko equations
373:Cyclotron radiation
105:Maxwell's equations
70:electromotive force
7400:Faraday efficiency
6678:Annalen der Physik
6025:special relativity
6001:
5979:
5949:
5925:
5903:
5881:
5859:
5837:
5815:
5773:
5751:
5560:
5250:
5145:
5107:
5033:
4971:
4944:
4915:
4888:
4845:
4636:. Mathematically,
4626:
4540:
4516:
4416:
4287:
4070:
3769:
3567:
3359:over a short time
3339:
3289:
3198:
3014:
2751:
2618:
2476:
2217:
2088:Poisson's equation
1935:
1748:
1693:
1681:, and orientation
1631:
1490:
1399:
1375:
1310:, and attaching a
1304:special relativity
1276:vector dot product
1229:
1118:
1082:
1065:special relativity
1017:
1010:electric generator
963:
471:Electrical network
308:Gauss magnetic law
273:Static electricity
233:Electric potential
103:(listed as one of
43:
7525:
7524:
7479:IET Faraday Medal
7247:Media related to
6941:10.1119/1.1987339
6863:978-1-108-42041-9
6754:Video Explanation
6749:10.1119/1.4849156
6707:on 12 March 2020.
6324:978-0-7503-0570-9
6213:978-0-13-241326-8
6170:Boston University
6151:978-0-19-530048-2
5813:
5749:
5492:
5018:
4339:
4301:
4300:
4119:
3840:
3606:
3450:
3234:
3091:
2954:
2886:
2803:
2703:
2681:
2570:
2548:
2454:
2379:
2329:
2315:
2184:
1920:
1746:
1629:
1508:Find the sign of
1370:
1246:is an element of
939:
938:
638:Reluctance (real)
608:Gyrator–capacitor
553:Resonant cavities
443:Maxwell equations
60:predicting how a
7555:
7515:
7514:
7469:Faraday (crater)
7459:Faraday Building
7405:Electrochemistry
7355:Faraday constant
7319:
7312:
7305:
7296:
7295:
7246:
7232:
7197:
7196:
7194:
7186:Einstein, Albert
7182:
7176:
7175:
7149:
7125:
7119:
7114:
7108:
7104:
7080:
7074:
7073:
7036:
7030:
7029:
7021:
7012:
7011:
6999:
6990:
6989:
6981:
6975:
6974:
6954:
6945:
6944:
6912:
6903:
6902:
6882:
6876:
6875:
6847:
6838:
6837:
6835:
6834:
6818:
6812:
6811:
6793:
6787:
6786:
6784:
6782:
6773:. Archived from
6762:
6756:
6752:
6718:
6709:
6708:
6706:
6700:. Archived from
6675:
6666:
6660:
6659:
6639:
6633:
6632:
6608:
6599:
6598:
6596:
6595:
6580:
6563:
6562:
6535:
6529:
6528:
6517:
6511:
6510:
6508:
6506:
6487:(28 June 2023).
6481:
6475:
6474:
6472:
6470:
6451:(1 March 2019).
6445:
6439:
6438:
6429:
6397:
6391:
6390:
6383:
6377:
6376:
6368:
6362:
6361:
6359:
6349:
6336:
6335:
6333:
6331:
6308:
6302:
6301:
6299:
6293:. Archived from
6286:
6277:
6268:
6267:
6261:
6251:
6242:
6241:
6239:
6238:
6224:
6218:
6217:
6197:
6191:
6190:
6188:
6180:
6174:
6173:
6162:
6156:
6155:
6135:
6129:
6128:
6126:
6125:
6111:
6058:
6010:
6008:
6007:
6002:
6000:
5988:
5986:
5985:
5980:
5978:
5977:
5958:
5956:
5955:
5950:
5948:
5947:
5934:
5932:
5931:
5926:
5924:
5912:
5910:
5909:
5904:
5902:
5890:
5888:
5887:
5882:
5880:
5868:
5866:
5865:
5860:
5858:
5846:
5844:
5843:
5838:
5836:
5824:
5822:
5821:
5816:
5814:
5812:
5804:
5803:
5794:
5782:
5780:
5779:
5774:
5772:
5760:
5758:
5757:
5752:
5750:
5748:
5740:
5739:
5730:
5725:
5724:
5709:
5682:
5663:
5647:
5579:
5569:
5567:
5566:
5561:
5559:
5554:
5543:
5535:
5534:
5529:
5520:
5519:
5501:
5493:
5491:
5483:
5482:
5473:
5471:
5470:
5455:
5450:
5439:
5431:
5430:
5425:
5416:
5408:
5407:
5392:
5391:
5375:
5363:
5357:
5346:
5336:
5330:
5320:
5310:
5306:
5298:
5292:
5286:
5276:Hering's_Paradox
5259:
5257:
5256:
5251:
5249:
5244:
5236:
5232:
5231:
5223:
5222:
5217:
5200:
5195:
5187:
5183:
5182:
5174:
5154:
5152:
5151:
5146:
5144:
5139:
5131:
5116:
5114:
5113:
5108:
5106:
5101:
5093:
5089:
5088:
5080:
5072:
5056:
5055:
5042:
5040:
5039:
5034:
5032:
5031:
5019:
5017:
5013:
5007:
5006:
5005:
4996:
4990:
4980:
4978:
4977:
4972:
4970:
4965:
4953:
4951:
4950:
4945:
4943:
4942:
4937:
4924:
4922:
4921:
4916:
4914:
4909:
4897:
4895:
4894:
4889:
4884:
4876:
4875:
4870:
4854:
4852:
4851:
4846:
4844:
4839:
4828:
4820:
4819:
4814:
4802:
4797:
4786:
4778:
4777:
4772:
4763:
4755:
4754:
4749:
4737:
4732:
4721:
4710:
4709:
4704:
4695:
4694:
4689:
4674:
4669:
4658:
4650:
4635:
4633:
4632:
4627:
4625:
4620:
4608:
4597:
4586:
4575:
4564:
4555:
4549:
4547:
4546:
4541:
4539:
4538:
4525:
4523:
4522:
4517:
4515:
4510:
4502:
4498:
4497:
4489:
4481:
4465:
4464:
4444:
4433:
4429:
4425:
4423:
4422:
4417:
4412:
4407:
4399:
4395:
4394:
4386:
4385:
4384:
4378:
4369:
4359:
4358:
4340:
4338:
4334:
4328:
4327:
4326:
4317:
4311:
4296:
4294:
4293:
4288:
4283:
4278:
4270:
4269:
4260:
4259:
4247:
4236:
4235:
4223:
4222:
4221:
4215:
4203:
4202:
4190:
4185:
4184:
4178:
4177:
4173:
4172:
4143:
4142:
4141:
4140:
4124:
4120:
4118:
4114:
4108:
4107:
4106:
4097:
4091:
4079:
4077:
4076:
4071:
4069:
4065:
4064:
4059:
4051:
4050:
4041:
4040:
4028:
4017:
4016:
4004:
4003:
4002:
3996:
3990:
3989:
3983:
3982:
3978:
3977:
3943:
3939:
3938:
3933:
3922:
3921:
3909:
3904:
3903:
3899:
3898:
3864:
3863:
3862:
3861:
3845:
3841:
3839:
3835:
3829:
3828:
3827:
3818:
3812:
3796:
3789:
3778:
3776:
3775:
3770:
3768:
3763:
3749:
3748:
3736:
3725:
3724:
3712:
3711:
3710:
3704:
3695:
3694:
3690:
3689:
3660:
3655:
3644:
3643:
3631:
3626:
3625:
3607:
3605:
3601:
3595:
3590:
3576:
3574:
3573:
3568:
3563:
3555:
3554:
3553:
3547:
3535:
3530:
3521:
3504:
3499:
3488:
3483:
3482:
3481:
3475:
3463:
3452:
3451:
3448:
3446:
3440:
3432:
3421:
3420:
3411:
3399:
3392:
3365:
3358:
3347:
3336:
3325:
3318:
3311:
3298:
3296:
3295:
3290:
3288:
3283:
3272:
3271:
3259:
3254:
3253:
3235:
3233:
3229:
3223:
3218:
3207:
3205:
3204:
3199:
3197:
3192:
3181:
3180:
3168:
3163:
3162:
3158:
3157:
3128:
3123:
3115:
3114:
3113:
3112:
3096:
3092:
3090:
3082:
3081:
3072:
3066:
3065:
3061:
3060:
3032:
3023:
3021:
3020:
3015:
3013:
3009:
3008:
3003:
2992:
2991:
2979:
2974:
2973:
2955:
2953:
2949:
2943:
2938:
2928:
2924:
2923:
2918:
2910:
2909:
2908:
2907:
2891:
2887:
2885:
2877:
2876:
2867:
2861:
2860:
2856:
2855:
2827:
2826:
2825:
2824:
2808:
2804:
2802:
2798:
2792:
2791:
2790:
2781:
2775:
2760:
2758:
2757:
2752:
2750:
2745:
2728:
2723:
2722:
2704:
2702:
2698:
2692:
2687:
2682:
2680:
2676:
2670:
2669:
2668:
2659:
2653:
2643:
2633:
2632:
2627:
2625:
2624:
2619:
2617:
2612:
2595:
2590:
2589:
2571:
2569:
2565:
2559:
2554:
2549:
2547:
2543:
2537:
2536:
2535:
2526:
2520:
2511:
2485:
2483:
2482:
2477:
2475:
2474:
2465:
2464:
2455:
2453:
2452:
2451:
2446:
2440:
2436:
2427:
2422:
2416:
2415:
2411:
2410:
2406:
2397:
2384:
2380:
2378:
2370:
2360:
2356:
2347:
2338:
2331:
2327:
2326:
2325:
2316:
2314:
2303:
2286:
2278:
2277:
2272:
2248:
2242:
2229:surface integral
2226:
2224:
2223:
2218:
2213:
2208:
2200:
2195:
2194:
2185:
2183:
2179:
2173:
2168:
2160:
2155:
2147:
2142:
2141:
2122:
2113:
2107:
2092:gradient theorem
2081:
2075:
2065:
2051:
2045:
2039:
2032:
2025:
2011:
2004:
1990:
1984:
1977:
1967:
1960:
1953:
1944:
1942:
1941:
1936:
1934:
1929:
1921:
1919:
1911:
1910:
1901:
1899:
1898:
1883:
1878:
1870:
1865:
1864:
1823:
1819:
1809:
1790:
1768:
1757:
1755:
1754:
1749:
1747:
1745:
1737:
1736:
1727:
1719:
1686:
1680:
1673:
1653:
1644:
1640:
1638:
1637:
1632:
1630:
1628:
1624:
1618:
1617:
1616:
1607:
1601:
1590:
1589:
1576:
1567:
1555:
1543:
1531:
1525:
1516:
1504:
1487:
1478:
1469:
1465:
1459:
1421:
1408:
1406:
1405:
1400:
1398:
1397:
1384:
1382:
1381:
1376:
1371:
1369:
1365:
1359:
1358:
1357:
1348:
1342:
1334:
1333:
1297:
1284:
1273:
1263:
1257:
1245:
1238:
1236:
1235:
1230:
1224:
1219:
1202:
1197:
1196:
1175:
1174:
1157:surface integral
1154:
1142:
1135:
1115:
1108:
1052:, formulated by
1032:Oliver Heaviside
931:
924:
917:
598:Electric machine
581:Magnetic circuit
543:Parallel circuit
533:Network analysis
498:Electric current
433:London equations
278:Triboelectricity
268:Potential energy
137:
127:Electromagnetism
118:
117:
66:electric circuit
58:electromagnetism
7563:
7562:
7558:
7557:
7556:
7554:
7553:
7552:
7543:Michael Faraday
7538:Electrodynamics
7528:
7527:
7526:
7521:
7503:
7442:
7419:
7380:Faraday rotator
7375:Faraday paradox
7328:
7326:Michael Faraday
7323:
7239:
7226:
7205:
7203:Further reading
7200:
7192:
7183:
7179:
7126:
7122:
7115:
7111:
7105:
7101:
7081:
7077:
7037:
7033:
7022:
7015:
7006:. p. 396.
7000:
6993:
6982:
6978:
6971:
6955:
6948:
6913:
6906:
6899:
6883:
6879:
6864:
6848:
6841:
6832:
6830:
6823:"Faraday's Law"
6819:
6815:
6808:
6794:
6790:
6780:
6778:
6763:
6759:
6719:
6712:
6704:
6673:
6667:
6663:
6656:
6640:
6636:
6629:
6609:
6602:
6593:
6591:
6581:
6566:
6556:
6536:
6532:
6518:
6514:
6504:
6502:
6482:
6478:
6468:
6466:
6446:
6442:
6430:
6412:(31): 483–494.
6398:
6394:
6385:
6384:
6380:
6369:
6365:
6356:Michael Faraday
6350:
6339:
6329:
6327:
6325:
6309:
6305:
6297:
6284:
6278:
6271:
6252:
6245:
6236:
6234:
6226:
6225:
6221:
6214:
6198:
6194:
6186:
6182:
6181:
6177:
6164:
6163:
6159:
6152:
6136:
6132:
6123:
6121:
6112:
6108:
6104:
6099:
6090:Faraday paradox
6065:
6059:
6050:Albert Einstein
6048:
6021:Albert Einstein
6017:
6015:Einstein's view
5996:
5994:
5991:
5990:
5973:
5972:
5964:
5961:
5960:
5943:
5942:
5940:
5937:
5936:
5920:
5918:
5915:
5914:
5898:
5896:
5893:
5892:
5876:
5874:
5871:
5870:
5854:
5852:
5849:
5848:
5832:
5830:
5827:
5826:
5805:
5799:
5795:
5793:
5788:
5785:
5784:
5768:
5766:
5763:
5762:
5741:
5735:
5731:
5729:
5720:
5719:
5705:
5703:
5700:
5699:
5691:
5683:
5675:
5659:
5649:
5639:
5609:transformer emf
5597:
5592:
5586:
5574:
5555:
5550:
5539:
5530:
5525:
5524:
5512:
5508:
5497:
5484:
5478:
5474:
5472:
5466:
5462:
5451:
5446:
5435:
5426:
5421:
5420:
5412:
5400:
5396:
5387:
5386:
5384:
5381:
5380:
5373:
5368:
5361:
5358:
5349:
5338:
5332:
5328:
5321:
5308:
5304:
5296:
5290:
5284:
5278:
5272:
5270:Faraday paradox
5266:
5245:
5240:
5227:
5218:
5213:
5212:
5211:
5207:
5196:
5191:
5178:
5170:
5169:
5165:
5160:
5157:
5156:
5140:
5135:
5127:
5122:
5119:
5118:
5102:
5097:
5084:
5076:
5068:
5067:
5063:
5051:
5050:
5048:
5045:
5044:
5027:
5026:
5009:
5008:
5001:
4997:
4992:
4991:
4989:
4987:
4984:
4983:
4966:
4961:
4959:
4956:
4955:
4938:
4933:
4932:
4930:
4927:
4926:
4910:
4905:
4903:
4900:
4899:
4880:
4871:
4866:
4865:
4860:
4857:
4856:
4840:
4835:
4824:
4815:
4810:
4809:
4798:
4793:
4782:
4773:
4768:
4767:
4759:
4750:
4745:
4744:
4733:
4728:
4717:
4705:
4700:
4699:
4690:
4685:
4684:
4670:
4665:
4654:
4646:
4641:
4638:
4637:
4621:
4616:
4614:
4611:
4610:
4607:
4599:
4596:
4588:
4585:
4577:
4574:
4566:
4560:
4551:
4534:
4533:
4531:
4528:
4527:
4511:
4506:
4493:
4485:
4477:
4476:
4472:
4460:
4459:
4457:
4454:
4453:
4443:
4435:
4431:
4427:
4408:
4403:
4390:
4380:
4379:
4374:
4373:
4365:
4364:
4360:
4351:
4347:
4330:
4329:
4322:
4318:
4313:
4312:
4310:
4308:
4305:
4304:
4303:The result is:
4279:
4274:
4265:
4264:
4255:
4251:
4243:
4231:
4227:
4217:
4216:
4211:
4210:
4198:
4194:
4186:
4180:
4179:
4168:
4164:
4154:
4150:
4136:
4132:
4125:
4110:
4109:
4102:
4098:
4093:
4092:
4090:
4087:
4086:
4084:
4081:
4080:
4060:
4055:
4046:
4045:
4036:
4032:
4024:
4012:
4008:
3998:
3997:
3992:
3991:
3985:
3984:
3973:
3969:
3959:
3955:
3951:
3947:
3934:
3929:
3917:
3913:
3905:
3894:
3890:
3880:
3876:
3872:
3868:
3857:
3853:
3846:
3831:
3830:
3823:
3819:
3814:
3813:
3811:
3808:
3807:
3805:
3802:
3801:
3791:
3788:
3780:
3764:
3759:
3744:
3740:
3732:
3720:
3716:
3706:
3705:
3700:
3699:
3685:
3681:
3671:
3667:
3656:
3651:
3639:
3635:
3627:
3612:
3608:
3597:
3596:
3591:
3589:
3587:
3584:
3583:
3559:
3549:
3548:
3543:
3542:
3531:
3526:
3517:
3500:
3495:
3484:
3477:
3476:
3471:
3470:
3459:
3447:
3442:
3441:
3436:
3428:
3416:
3412:
3407:
3405:
3402:
3401:
3394:
3383:
3374:
3367:
3360:
3357:
3349:
3342:
3335:
3327:
3320:
3313:
3306:
3284:
3279:
3267:
3263:
3255:
3240:
3236:
3225:
3224:
3219:
3217:
3215:
3212:
3211:
3193:
3188:
3176:
3172:
3164:
3153:
3149:
3139:
3135:
3124:
3119:
3108:
3104:
3097:
3083:
3077:
3073:
3071:
3068:
3067:
3056:
3052:
3045:
3041:
3039:
3036:
3035:
3031:
3025:
3004:
2999:
2987:
2983:
2975:
2960:
2956:
2945:
2944:
2939:
2937:
2936:
2932:
2919:
2914:
2903:
2899:
2892:
2878:
2872:
2868:
2866:
2863:
2862:
2851:
2847:
2840:
2836:
2835:
2831:
2820:
2816:
2809:
2794:
2793:
2786:
2782:
2777:
2776:
2774:
2771:
2770:
2768:
2765:
2764:
2746:
2741:
2724:
2709:
2705:
2694:
2693:
2688:
2686:
2672:
2671:
2664:
2660:
2655:
2654:
2652:
2650:
2647:
2646:
2637:
2613:
2608:
2591:
2576:
2572:
2561:
2560:
2555:
2553:
2539:
2538:
2531:
2527:
2522:
2521:
2519:
2517:
2514:
2513:
2509:
2491:
2467:
2466:
2460:
2456:
2447:
2442:
2441:
2432:
2431:
2423:
2418:
2417:
2402:
2401:
2393:
2392:
2388:
2371:
2352:
2351:
2343:
2339:
2337:
2333:
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2321:
2317:
2307:
2302:
2282:
2273:
2268:
2267:
2265:
2262:
2261:
2258:volume integral
2244:
2241:
2235:
2209:
2204:
2196:
2190:
2186:
2175:
2174:
2169:
2167:
2156:
2151:
2143:
2134:
2130:
2128:
2125:
2124:
2118:
2117:If the surface
2109:
2102:
2077:
2071:
2060:
2047:
2046:to the surface
2041:
2034:
2027:
2021:
2014:right-hand rule
2006:
1999:
1986:
1979:
1973:
1962:
1955:
1949:
1946:
1930:
1925:
1912:
1906:
1902:
1900:
1894:
1890:
1879:
1874:
1866:
1857:
1853:
1851:
1848:
1847:
1821:
1815:
1796:
1777:
1766:
1759:
1738:
1732:
1728:
1726:
1715:
1707:
1704:
1703:
1689:right-hand rule
1682:
1675:
1674:, its boundary
1669:
1660:
1652:
1646:
1642:
1620:
1619:
1612:
1608:
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1585:
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1527:
1524:
1518:
1515:
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1500:
1486:
1480:
1477:
1471:
1467:
1461:
1458:
1452:
1420:
1414:
1393:
1392:
1390:
1387:
1386:
1361:
1360:
1353:
1349:
1344:
1343:
1341:
1329:
1328:
1326:
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1322:
1293:
1279:
1265:
1259:
1251:
1240:
1220:
1215:
1198:
1183:
1179:
1170:
1166:
1164:
1161:
1160:
1148:
1140:
1134:
1128:
1110:
1106:
1099:
1073:
1061:Albert Einstein
1020:Michael Faraday
969:(like a modern
948:Michael Faraday
944:
935:
906:
905:
721:
713:
712:
668:
658:
657:
613:Induction motor
583:
573:
572:
488:Current density
473:
463:
462:
453:Poynting vector
363:
361:Electrodynamics
353:
352:
348:Right-hand rule
313:Magnetic dipole
303:Biot–Savart law
293:
283:
282:
218:Electric dipole
213:Electric charge
188:
86:electric motors
17:
12:
11:
5:
7561:
7551:
7550:
7545:
7540:
7523:
7522:
7520:
7519:
7508:
7505:
7504:
7502:
7501:
7496:
7491:
7486:
7481:
7476:
7474:Faraday Future
7471:
7466:
7461:
7456:
7450:
7448:
7444:
7443:
7441:
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7397:
7392:
7387:
7382:
7377:
7372:
7367:
7362:
7357:
7352:
7347:
7345:Faraday effect
7342:
7336:
7334:
7330:
7329:
7322:
7321:
7314:
7307:
7299:
7293:
7292:
7287:
7279:
7274:
7264:Roberto Vega.
7261:
7252:
7238:
7237:External links
7235:
7234:
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7201:
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7013:
6991:
6976:
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6946:
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6897:
6877:
6862:
6839:
6821:Nave, Carl R.
6813:
6806:
6788:
6765:Salu, Yehuda.
6757:
6710:
6661:
6654:
6634:
6627:
6600:
6564:
6554:
6530:
6512:
6476:
6440:
6392:
6378:
6363:
6337:
6323:
6303:
6300:on 2021-08-30.
6269:
6243:
6228:"Joseph Henry"
6219:
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2749:
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2691:
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2679:
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2663:
2658:
2616:
2611:
2607:
2604:
2601:
2598:
2594:
2588:
2585:
2582:
2579:
2575:
2568:
2564:
2558:
2552:
2546:
2542:
2534:
2530:
2525:
2490:
2487:
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2459:
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2430:
2426:
2421:
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2400:
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2363:
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2324:
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2298:
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2289:
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2281:
2276:
2271:
2237:
2216:
2212:
2207:
2203:
2199:
2193:
2189:
2182:
2178:
2172:
2166:
2163:
2159:
2154:
2150:
2146:
2140:
2137:
2133:
1933:
1928:
1924:
1918:
1915:
1909:
1905:
1897:
1893:
1889:
1886:
1882:
1877:
1873:
1869:
1863:
1860:
1856:
1845:
1812:magnetic field
1793:electric field
1744:
1741:
1735:
1731:
1725:
1722:
1718:
1714:
1711:
1701:
1659:
1656:
1648:
1627:
1623:
1615:
1611:
1606:
1599:
1596:
1593:
1588:
1571:
1564:, composed of
1558:
1557:
1550:
1545:
1538:
1533:
1520:
1511:
1506:
1497:
1482:
1473:
1454:
1416:
1396:
1374:
1368:
1364:
1356:
1352:
1347:
1340:
1337:
1332:
1319:rate of change
1314:to the leads.
1228:
1223:
1218:
1214:
1211:
1208:
1205:
1201:
1195:
1192:
1189:
1186:
1182:
1178:
1173:
1169:
1130:
1122:magnetic field
1098:
1095:
1072:
1069:
1024:lines of force
999:Faraday's disk
975:electromagnets
943:
940:
937:
936:
934:
933:
926:
919:
911:
908:
907:
904:
903:
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803:
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793:
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783:
778:
773:
768:
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753:
748:
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738:
733:
728:
722:
719:
718:
715:
714:
711:
710:
705:
700:
695:
690:
688:Four-potential
685:
680:
675:
669:
664:
663:
660:
659:
656:
655:
650:
645:
640:
635:
630:
625:
620:
615:
610:
605:
603:Electric motor
600:
595:
590:
584:
579:
578:
575:
574:
571:
570:
565:
560:
558:Series circuit
555:
550:
545:
540:
535:
530:
528:Kirchhoff laws
525:
520:
515:
510:
505:
500:
495:
493:Direct current
490:
485:
480:
474:
469:
468:
465:
464:
461:
460:
455:
450:
448:Maxwell tensor
445:
440:
435:
430:
425:
420:
418:Larmor formula
415:
410:
405:
400:
395:
390:
385:
380:
375:
370:
368:Bremsstrahlung
364:
359:
358:
355:
354:
351:
350:
345:
340:
335:
330:
325:
320:
318:Magnetic field
315:
310:
305:
300:
294:
291:Magnetostatics
289:
288:
285:
284:
281:
280:
275:
270:
265:
260:
255:
250:
245:
240:
235:
230:
225:
223:Electric field
220:
215:
210:
205:
200:
195:
193:Charge density
189:
186:Electrostatics
184:
183:
180:
179:
178:
177:
172:
167:
162:
157:
152:
147:
139:
138:
130:
129:
123:
122:
121:Articles about
68:to produce an
62:magnetic field
15:
9:
6:
4:
3:
2:
7560:
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7544:
7541:
7539:
7536:
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7451:
7449:
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7432:
7429:
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7416:
7415:Line of force
7413:
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7260:
7256:
7253:
7250:
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7241:
7240:
7231:
7227:
7225:0-486-60637-6
7221:
7217:
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7206:
7191:
7187:
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7135:
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7113:
7102:
7100:0-13-805326-X
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6970:9783540368052
6966:
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6900:
6898:0-486-43241-6
6894:
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6859:
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6854:
6846:
6844:
6828:
6824:
6817:
6809:
6807:0-7195-3382-1
6803:
6799:
6792:
6777:on 7 May 2020
6776:
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6655:9780716708100
6651:
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6628:0-13-805326-X
6624:
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6577:
6575:
6573:
6571:
6569:
6561:
6557:
6555:0-07-027406-1
6551:
6547:
6543:
6542:
6534:
6527:
6523:
6516:
6500:
6496:
6495:
6490:
6486:
6485:Siegel, Ethan
6480:
6464:
6460:
6459:
6454:
6450:
6449:Siegel, Ethan
6444:
6436:
6427:
6423:
6419:
6415:
6411:
6407:
6403:
6396:
6388:
6382:
6374:
6367:
6358:
6357:
6348:
6346:
6344:
6342:
6326:
6320:
6316:
6315:
6307:
6296:
6292:
6291:
6283:
6276:
6274:
6265:
6260:
6259:
6250:
6248:
6233:
6229:
6223:
6215:
6209:
6205:
6204:
6196:
6185:
6179:
6172:. 1999-07-22.
6171:
6167:
6161:
6153:
6147:
6143:
6142:
6134:
6119:
6118:
6110:
6106:
6096:
6093:
6091:
6088:
6086:
6083:
6081:
6078:
6076:
6073:
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6068:
6067:
6057:
6056:
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6041:
6037:
6033:
6028:
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6022:
6012:
5966:
5809:
5790:
5745:
5726:
5713:
5710:
5696:
5686:
5681:
5680:
5672:
5670:
5665:
5662:
5658:
5653:
5646:
5642:
5636:
5631:
5628:
5626:
5625:
5620:
5616:
5614:
5610:
5606:
5605:Lorentz force
5602:
5595:Two phenomena
5591:
5581:
5578:
5547:
5536:
5531:
5509:
5505:
5494:
5488:
5463:
5459:
5456:
5443:
5432:
5427:
5417:
5397:
5393:
5379:
5378:
5377:
5367:
5356:
5351:
5345:
5341:
5335:
5326:
5319:
5314:
5313:
5312:
5301:
5295:
5289:
5283:
5277:
5271:
5261:
5237:
5233:
5224:
5219:
5208:
5204:
5201:
5188:
5184:
5175:
5166:
5162:
5132:
5124:
5094:
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5073:
5064:
5060:
5057:
5023:
5020:
5014:
5002:
4939:
4877:
4872:
4832:
4821:
4816:
4803:
4790:
4779:
4774:
4764:
4756:
4751:
4738:
4725:
4714:
4706:
4696:
4691:
4675:
4662:
4651:
4606:
4602:
4595:
4591:
4584:
4580:
4573:
4569:
4563:
4557:
4554:
4503:
4499:
4490:
4482:
4473:
4469:
4466:
4451:
4450:Lorentz force
4446:
4442:
4438:
4413:
4400:
4396:
4387:
4370:
4361:
4348:
4344:
4341:
4335:
4323:
4297:
4284:
4271:
4256:
4252:
4240:
4232:
4228:
4207:
4199:
4195:
4169:
4165:
4151:
4147:
4144:
4137:
4133:
4129:
4126:
4121:
4115:
4103:
4066:
4052:
4037:
4033:
4021:
4013:
4009:
3974:
3970:
3956:
3952:
3948:
3944:
3940:
3926:
3918:
3914:
3895:
3891:
3877:
3873:
3869:
3865:
3858:
3854:
3850:
3847:
3842:
3836:
3824:
3798:
3795:
3787:
3783:
3756:
3745:
3741:
3729:
3721:
3717:
3686:
3682:
3668:
3664:
3661:
3648:
3640:
3636:
3619:
3609:
3602:
3581:
3556:
3536:
3522:
3514:
3511:
3508:
3492:
3489:
3464:
3456:
3453:
3433:
3425:
3422:
3417:
3398:
3391:
3387:
3382:
3378:
3371:
3364:
3356:
3352:
3346:
3334:
3330:
3324:
3317:
3310:
3303:
3299:
3276:
3268:
3264:
3247:
3237:
3230:
3208:
3185:
3177:
3173:
3154:
3150:
3136:
3132:
3129:
3116:
3109:
3105:
3101:
3098:
3093:
3087:
3057:
3053:
3042:
3028:
3010:
2996:
2988:
2984:
2967:
2957:
2950:
2933:
2929:
2925:
2911:
2904:
2900:
2896:
2893:
2888:
2882:
2852:
2848:
2837:
2832:
2828:
2821:
2817:
2813:
2810:
2805:
2799:
2787:
2761:
2738:
2732:
2716:
2706:
2699:
2683:
2677:
2665:
2641:
2635:
2634:
2631:
2628:
2605:
2599:
2583:
2573:
2566:
2550:
2544:
2532:
2506:
2504:
2500:
2496:
2486:
2471:
2461:
2457:
2448:
2437:
2428:
2412:
2407:
2398:
2389:
2385:
2381:
2375:
2364:
2361:
2357:
2334:
2322:
2318:
2311:
2308:
2304:
2299:
2296:
2290:
2287:
2274:
2259:
2255:
2250:
2247:
2240:
2234:
2233:magnetic flux
2230:
2214:
2201:
2187:
2180:
2164:
2161:
2148:
2131:
2121:
2115:
2112:
2106:
2100:
2095:
2093:
2089:
2085:
2080:
2074:
2069:
2064:
2058:
2057:line integral
2053:
2050:
2044:
2038:
2031:
2024:
2019:
2015:
2010:
2003:
1996:
1994:
1989:
1983:
1976:
1971:
1970:infinitesimal
1966:
1959:
1952:
1945:
1922:
1916:
1891:
1887:
1884:
1871:
1854:
1844:
1842:
1838:
1837:integral form
1834:
1830:
1825:
1818:
1813:
1807:
1803:
1799:
1794:
1788:
1784:
1780:
1775:
1772:
1764:
1758:
1742:
1723:
1720:
1712:
1700:
1698:
1690:
1685:
1679:
1672:
1666:
1662:
1655:
1651:
1625:
1613:
1597:
1594:
1591:
1574:
1563:
1553:
1546:
1541:
1534:
1530:
1523:
1514:
1507:
1503:
1498:
1495:
1494:
1493:
1485:
1476:
1464:
1457:
1449:
1445:
1441:
1439:
1434:
1432:
1427:
1425:
1424:magnetic flux
1419:
1412:
1372:
1366:
1354:
1338:
1335:
1320:
1315:
1313:
1309:
1305:
1301:
1296:
1290:
1288:
1283:
1277:
1272:
1268:
1262:
1255:
1249:
1244:
1226:
1212:
1206:
1190:
1180:
1176:
1171:
1158:
1152:
1146:
1139:
1133:
1127:
1126:magnetic flux
1123:
1114:
1103:
1093:
1091:
1090:magnetic flux
1085:
1077:
1071:Faraday's law
1068:
1066:
1062:
1059:According to
1057:
1055:
1051:
1047:
1045:
1041:
1037:
1033:
1029:
1025:
1021:
1015:
1011:
1006:
1002:
1000:
996:
990:
988:
987:magnetic flux
984:
980:
976:
972:
968:
959:
955:
953:
949:
932:
927:
925:
920:
918:
913:
912:
910:
909:
902:
899:
897:
894:
892:
889:
887:
884:
882:
879:
877:
874:
872:
869:
867:
864:
862:
859:
857:
854:
852:
849:
847:
844:
842:
839:
837:
834:
832:
829:
827:
824:
822:
819:
817:
814:
812:
809:
807:
804:
802:
799:
797:
794:
792:
789:
787:
784:
782:
779:
777:
774:
772:
769:
767:
764:
762:
759:
757:
754:
752:
749:
747:
744:
742:
739:
737:
734:
732:
729:
727:
724:
723:
717:
716:
709:
706:
704:
701:
699:
696:
694:
691:
689:
686:
684:
681:
679:
676:
674:
671:
670:
667:
662:
661:
654:
651:
649:
646:
644:
641:
639:
636:
634:
631:
629:
626:
624:
621:
619:
616:
614:
611:
609:
606:
604:
601:
599:
596:
594:
591:
589:
586:
585:
582:
577:
576:
569:
566:
564:
561:
559:
556:
554:
551:
549:
546:
544:
541:
539:
536:
534:
531:
529:
526:
524:
523:Joule heating
521:
519:
516:
514:
511:
509:
506:
504:
501:
499:
496:
494:
491:
489:
486:
484:
481:
479:
476:
475:
472:
467:
466:
459:
456:
454:
451:
449:
446:
444:
441:
439:
438:Lorentz force
436:
434:
431:
429:
426:
424:
421:
419:
416:
414:
411:
409:
406:
404:
401:
399:
396:
394:
391:
389:
386:
384:
381:
379:
376:
374:
371:
369:
366:
365:
362:
357:
356:
349:
346:
344:
341:
339:
338:Magnetization
336:
334:
331:
329:
326:
324:
323:Magnetic flux
321:
319:
316:
314:
311:
309:
306:
304:
301:
299:
296:
295:
292:
287:
286:
279:
276:
274:
271:
269:
266:
264:
261:
259:
256:
254:
251:
249:
246:
244:
241:
239:
236:
234:
231:
229:
228:Electric flux
226:
224:
221:
219:
216:
214:
211:
209:
206:
204:
201:
199:
196:
194:
191:
190:
187:
182:
181:
176:
173:
171:
168:
166:
165:Computational
163:
161:
158:
156:
153:
151:
148:
146:
143:
142:
141:
140:
136:
132:
131:
128:
125:
124:
120:
119:
116:
114:
113:Lorentz force
108:
106:
102:
97:
95:
91:
87:
83:
79:
75:
71:
67:
63:
59:
55:
51:
50:Faraday's law
47:
40:
36:
32:
28:
23:
19:
7435:
7410:Faraday disc
7390:Faraday wave
7350:Faraday cage
7339:
7283:
7265:
7229:
7214:
7180:
7137:
7133:
7123:
7112:
7085:
7078:
7049:
7043:
7034:
7025:
7007:
7003:
6985:
6979:
6959:
6924:
6920:
6916:
6887:
6880:
6852:
6831:. Retrieved
6827:HyperPhysics
6826:
6816:
6797:
6791:
6779:. Retrieved
6775:the original
6770:
6760:
6732:
6726:
6702:the original
6684:(1): 31–44.
6681:
6677:
6664:
6644:
6637:
6613:
6592:. Retrieved
6588:
6559:
6540:
6533:
6525:
6521:
6515:
6503:. Retrieved
6492:
6479:
6467:. Retrieved
6456:
6443:
6434:
6409:
6405:
6395:
6381:
6372:
6366:
6355:
6328:. Retrieved
6313:
6306:
6295:the original
6288:
6257:
6235:. Retrieved
6231:
6222:
6202:
6195:
6178:
6160:
6140:
6133:
6122:. Retrieved
6116:
6109:
6095:Felici's law
6070:Eddy current
6053:
6042:
6038:
6034:
6030:
6018:
5695:motional emf
5694:
5692:
5685:
5677:
5668:
5666:
5660:
5656:
5651:
5644:
5640:
5637:
5633:
5629:
5622:
5617:
5608:
5601:motional emf
5600:
5598:
5576:
5572:
5371:
5365:
5343:
5339:
5333:
5299:
5293:
5287:
5281:
5279:
4604:
4600:
4593:
4589:
4582:
4578:
4571:
4567:
4561:
4558:
4552:
4447:
4440:
4436:
4302:
3799:
3793:
3785:
3781:
3577:
3396:
3389:
3385:
3380:
3376:
3369:
3362:
3354:
3350:
3344:
3332:
3328:
3322:
3315:
3308:
3209:
3026:
2762:
2645:
2639:
2629:
2507:
2498:
2492:
2251:
2245:
2238:
2119:
2116:
2110:
2104:
2098:
2096:
2084:scalar field
2078:
2072:
2062:
2054:
2048:
2042:
2036:
2029:
2022:
2008:
2001:
1997:
1987:
1981:
1974:
1964:
1957:
1950:
1947:
1846:
1836:
1826:
1816:
1805:
1801:
1797:
1786:
1782:
1778:
1760:
1702:
1697:conservative
1694:
1683:
1677:
1670:
1661:
1649:
1572:
1562:coil of wire
1559:
1551:
1539:
1528:
1521:
1512:
1501:
1491:
1483:
1474:
1462:
1455:
1442:
1435:
1428:
1417:
1316:
1308:open circuit
1294:
1291:
1281:
1270:
1266:
1260:
1253:
1242:
1150:
1131:
1119:
1112:
1087:
1083:
1058:
1048:
1036:motional emf
1018:
1012:, a type of
991:
982:
979:galvanometer
964:
952:Joseph Henry
950:in 1831 and
945:
683:Four-current
618:Linear motor
503:Electrolysis
407:
383:Eddy current
343:Permeability
263:Polarization
258:Permittivity
109:
100:
98:
78:transformers
49:
45:
44:
38:
34:
30:
26:
18:
7365:Faraday cup
7140:: 109–122.
6023:to develop
5607:), and the
4550:is emf and
2068:circulation
1687:set by the
1248:area vector
653:Transformer
483:Capacitance
408:Faraday law
203:Coulomb law
145:Electricity
48:(or simply
7532:Categories
7147:1911.11138
6927:(5): 713.
6833:2011-08-29
6594:2020-11-07
6237:2016-12-30
6124:2009-08-06
6102:References
6075:Inductance
5323:Faraday's
5274:See also:
5268:See also:
5264:Exceptions
3312:of a loop
2499:everything
2066:is called
1993:orthogonal
1776:and again
1431:Lenz's law
1413:(emf) and
1050:Lenz's law
720:Scientists
568:Waveguides
548:Resistance
518:Inductance
298:Ampère law
90:generators
7172:208095922
7070:135524562
7056:: 11–23.
6872:965197645
6735:(1): 48.
6494:Big Think
6330:28 August
6085:Crosstalk
5970:∇
5967:−
5807:∂
5797:∂
5791:−
5743:∂
5733:∂
5727:−
5717:∇
5714:−
5548:⋅
5537:×
5517:Σ
5514:∂
5510:∮
5503:Σ
5495:⋅
5486:∂
5476:∂
5468:Σ
5464:∫
5460:−
5444:⋅
5433:×
5405:Σ
5402:∂
5398:∫
5238:⋅
5225:×
5205:∮
5189:⋅
5176:×
5163:∮
5133:⋅
5125:∮
5095:⋅
5082:×
5061:∮
5024:−
4999:Φ
4878:×
4833:⋅
4822:×
4791:⋅
4780:×
4757:×
4726:⋅
4715:×
4663:⋅
4652:×
4504:⋅
4491:×
4470:∮
4401:⋅
4388:×
4356:Σ
4353:∂
4349:∮
4345:−
4320:Φ
4272:⋅
4241:×
4159:Σ
4156:∂
4152:∮
4148:−
4100:Φ
4053:⋅
4022:×
3964:Σ
3961:∂
3957:∮
3953:−
3927:⋅
3885:Σ
3882:∂
3878:∮
3874:−
3821:Φ
3757:⋅
3730:×
3676:Σ
3673:∂
3669:∮
3665:−
3649:⋅
3614:Σ
3610:∫
3557:×
3537:⋅
3515:∫
3512:−
3493:×
3465:⋅
3457:∫
3434:⋅
3426:∫
3414:Φ
3277:⋅
3242:Σ
3238:∫
3186:⋅
3144:Σ
3141:∂
3137:∮
3133:−
3117:⋅
3085:∂
3075:∂
3047:Σ
3043:∫
2997:⋅
2962:Σ
2958:∫
2912:⋅
2880:∂
2870:∂
2842:Σ
2838:∫
2784:Φ
2739:⋅
2711:Σ
2707:∫
2662:Φ
2606:⋅
2578:Σ
2574:∫
2529:Φ
2493:The four
2429:−
2399:−
2386:×
2373:∂
2341:∂
2319:∭
2312:π
2300:−
2297:≈
2260:equation
2202:⋅
2192:Σ
2188:∫
2165:−
2149:⋅
2139:Σ
2136:∂
2132:∮
2033:of curve
1923:⋅
1914:∂
1904:∂
1896:Σ
1892:∫
1888:−
1872:⋅
1862:Σ
1859:∂
1855:∮
1820:and time
1740:∂
1730:∂
1724:−
1713:×
1710:∇
1610:Φ
1595:−
1440:in 1845.
1351:Φ
1339:−
1312:voltmeter
1213:⋅
1185:Σ
1181:∬
1168:Φ
1054:Emil Lenz
876:Steinmetz
806:Kirchhoff
791:Jefimenko
786:Hopkinson
771:Helmholtz
766:Heaviside
628:Permeance
513:Impedance
253:Insulator
248:Gauss law
198:Conductor
175:Phenomena
170:Textbooks
150:Magnetism
94:solenoids
82:inductors
7424:Lectures
7212:(1881).
6499:Archived
6463:Archived
6063:See also
6047:—
5825:, where
5674:—
3319:in time
2472:′
2438:′
2408:′
2358:′
2243:through
1774:operator
1765:) where
1763:SI units
1145:boundary
901:Wiechert
856:Poynting
746:Einstein
593:DC motor
588:AC motor
423:Lenz law
208:Electret
7447:Related
7333:Physics
7152:Bibcode
6929:Bibcode
6781:30 July
6737:Bibcode
6686:Bibcode
6619:301–303
6414:Bibcode
6264:623–624
2059:around
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1409:is the
1138:surface
942:History
886:Thomson
861:Ritchie
851:Poisson
836:Neumann
831:Maxwell
826:Lorentz
821:Liénard
751:Faraday
736:Coulomb
563:Voltage
538:Ohm law
160:History
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866:Savart
846:Ørsted
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801:Kelvin
756:Fizeau
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1998:Both
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891:Volta
881:Tesla
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781:Hertz
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761:Gauss
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