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Ampere s law

During the next decades after the appearance of the Volta pile and of different other versions of batteries, fundamental laws of electrodynamics and electromagnetism were formulated based on experiments carried out with electric current supplied by batteries Ampere s law of interaction between electrical currents (1820), Ohm s law of proportionality between current and voltage (1827), the laws of electromagnetic induction (Faraday, 1831), Joule s law of the thermal effect of electric current, and many others. [Pg.694]

According to Ampere s law, for any magnet which does not contain ferromagnetic materials, there is a linear dependence between the current I and... [Pg.413]

The strayfield does not arise from any current, thus from Ampere s law it follows that... [Pg.106]

Ampere s law (or the law of Biot65 and Savart66) for the force between two electrical currents j and j2 is given by... [Pg.50]

Since magnetic monopoles have never been found, the irreducible magnetic entity must be the magnetic dipole. In Ampere s law, we can define the magnetic flux density or magnetic induction B due to, or induced by, an electrical current j at a distance r, as... [Pg.51]

PROBLEM 2.7.15. The original version of Ampere s law had been simply... [Pg.60]

By Ampere s law this current jml due to the "rotating" nucleus produces, at the electron, a magnetic field... [Pg.184]

As expected for a guided mode, the electric field in the substrate and cover regions decays exponentially, and it shows an oscillatory behavior inside the waveguide film. For the TM polarization, one obtains similar, although not identical, relations for the magnetic field Hy, which then allows the calculation of the Cartesian components and E, of the electric field using the generalized Ampere s law in the Maxwell s equations [7]. [Pg.105]

Equation (2.70) demonstrates that (2.68) constitutes a weighted sum of the results obtained by the implementation of Ampere s law on the two loops L and L2. Moreover, (2.70) suggests an easy way to incorporate all 12 nodes along the outer loop in the FDTD approach. It must be mentioned, herein, that such a process will alter the values of the two right-hand side coefficients whose sum must always be unity. For this purpose and to enable a more adaptable minimization of the dispersion error, L2 loop is divided into two different loops L2A and Z,2B> as depicted in Figure 2.8(b). Thus, (2.70) receives the more consistent form of... [Pg.33]

Now, assume the dual-cell FDTD structure of Figure 3.5 and focus on the update of electric component Eu. In the first subiteration, the zz-directed part of the nonstandard Ampere s law, (6.18a), yields... [Pg.152]

Elect. inject. lumines- cence piezoelectr- icity Peltier effect pn junction effect Ampere s law electrolysis... [Pg.30]

The origin of radiation is electromagnetic and is based on three phenomenological facts The Ampere law, the Faraday law, and the Lorentt force (Eg. 8.1) which are usually covered in a physics course. However, the usual form of Ampere s law, which gives... [Pg.396]

To measure the magnetic properties, a small cylinder of the solid is suspended from a sensitive balance into the center of the solenoid (Fig. 15.2a). According to Ampere s law, passing a current i through the solenoid will create an axial uniform magnetic field intensity H of strength... [Pg.511]

I. The calculation of the momentary states from the complete law. Before the instantaneous rate of change, dyjdx, can be determined it is necessary to know the law, or form of the function connecting the varying quantities one with another. For instance, Galileo found by actual measurement that a stone falling vertically downwards from a position of rest travels a distance of s = gt2 feet in t seconds. Differentiation of this, as we shall see very shortly, furnishes the actual velocity of the stone at any instant of time, V = gt. In the same manner, Newton s law of inverse squares follows from Kepler s third law and Ampere s law, from the observed effect of one part of an electric circuit upon another. [Pg.30]

Physically, this equation expresses the fact that currents are the source of the magnetic field. Making use of Stokc s theorem, we can rewrite this equation in a second form, which is Ampere s law ... [Pg.42]

In this case, one might think that the current is closed at infinity, and Ampere s law can instantly be applied. Considering a closed horizontal circuit and in view of the axial symmetry, we can write ... [Pg.45]

In the case of a long line which is only semi-infinite, i.e. Oi = 0 and 2 = tt/2 one cannot apply Ampere s law, but using eq. 1.117 we obtain a field which is half that for the case of an infinitely long current-carr3dng wire, that is ... [Pg.45]

Suppose that a current electrode is placed in a uniform conducting medium so that the distribution of currents possesses the spherical symmetry (Fig. 1.32a). It is then a simple matter to realize that the magnetic field is zero everywhere in the medium. This follows directly from Biot-Savart law and the symmetry of the model. In other words, one can always find two current elements which are located symmetrically with respect to the observation point and of which the magnetic field differ by sign only. Let us notice that Ampere s law does not apply here because the current lines are not closed. [Pg.51]

We will now suppose that two current electrodes connected by a wire are located on the axis of a borehole (see Fig. 1.32b). In this case, we have a model characterized by the cylindrical symmetry. Unlike in the previous model, the magnetic field is in general not equal to zero but has one component However, the field is zero all along the 2-axis. In fact, applying Ampere s law as shown in Fig. 1.32b we have ... [Pg.51]

The first equation (eq. 1.246) is in essence Faraday s law, while the second equation (eq. 1.247) follows from a combination of Ampere s law and the postulate of conservation of charge. The third equation (eq. 1.248) is obtained from Coulomb s law for a nonalternating electric field. However, it remains valid regardless of how quickly the field may change. In order to demonstrate this we will use the postulate of conservation of charge (eqs. 1.131-1.132) ... [Pg.93]

Let us assume that in a curvilinear orthogonal system of coordinates a, (3 and (p, a shell surface coincides with one of the coordinate surfaces a. It is supposed that the electric field has a component only. Applying Ampere s law (the second Maxwell equation in the integral form) to the path abcd shown in Fig. 3.1 we obtain ... [Pg.147]


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