Electrical Engineering is a free introductory textbook to the basics of electrical engineering. See the editorial for more information....



Series Magnetic Circuits

Author: E.E. Kimberly

A magnetic circuit may be made up of sections of different reluctances in series, just as an electric circuit may be made up with different resistances in series.

Fig. 7-4 (a) shows a rod of iron of uniform quality, but of various cross-sections in series. The analogous electric circuit is shown in (b). The different component lengths of the magnetic circuit may be of different materials, and therefore may have different permeabilities, just as the electric circuit may be made up of sections of iron, copper, aluminum, etc., every one of which has different resistivity. There is, however, an important difference. The permeability of any section (being a complex function of flux density in that section) cannot be known unless the flux density is knoAvn. Since the resistance of a metallic conductor does not change (constant temperature being assumed) when the current density in it changes, Ohm's Law may be applied readily regardless of current magnitude. A comparison of the electric, magnetic, and hydraulic circuits is shown in Fig. 7-5.

Fig. 7-4. Comparison of Series Electric and Magnetic Circuits

Although the sum of the differences of magnetic potential in a magnetic circuit is equal to the total applied difference in magnetic potential, the actual percentage division of difference of potential among the several sections of Fig. 7-4 (a) will change as the flux density is changed. Therefore, it is not possible to calculate directly the flux density in any section of Fig. 7-4 (a) when a knoAvn difference of magnetic potential is applied to the whole. Such a problem can be solved by trial and error only. However, it is possible to calculate accurately the total mmf necessary to produce any specific flux density in any part, as is demonstrated in Example 7-1, which follows.

Fig. 7-5. Comparison of Electric, Magnetic, and Hydraulic Circuits: In an electric circuit containing resistance only at constant temperature, the resistance is always the same regardless of the amount of current flowing.

In a magnetic circuit without iron (or high-permeance alloy), the reluctance is always the same regardless of the amount of flux present. In a magnetic circuit containing iron, the reluctance varies as a complicated function of flux density, according to the magnetic characteristics of the iron. When only the mmf applied to the circuit is known, the flux cannot be calculated directly because the reluctance is not known until the flux is known.

In a hydraulic circuit, the resistance to fluid flow varies as a complicated function of the velocity of flow. When only the pressure in pounds per square inch is known, the water flow cannot be calculated directly because pipe friction is not a constant but is a function of velocity of fluid flow.

Example 7-1. - Determine the number of ampere-turns necessary to produce a magnetic field of 1,000,000 lines of flux in the structure of Fig. 7-6 (a). '

Solution. - The first step is to find the number of ampere-turns for part a of the magnetic circuit and the number for part 6. For part a,

ee_001-203.png

Fig. 7-6. Magnetic Circuit for Example 7-1

From curve a in Fig. 7-6 (6) corresponding to the kind of steel in section a in (a), a flux density of 12,730 lines per sq cm requires 11.5 ampere-turns per centimeter.

NIa = amp-turns per centimeter X centimeters in part a NIa = 11.5 X 157 = 1805 amp-turns for part a For part b,

ee_001-205.png

From curve b in (b) corresponding to the kind of steel in section b in (a), a flux density of 19,890 lines per sq cm requires 33 ampere-turns per centimeter.

ee_001-206.png

For the air-gap,

ee_001-207.png

The flux density in the air-gap (fringing being ignored) is the same as that in part 6, or 19,890 lines per sq cm. Hence,

and

ee_001-208.png

The total number of ampere-turns is

ee_001-209.png

When it is required to find the number of ampere-turns necessary to produce a given flux density in air and the dimensions are in inches instead of centimeters, it is convenient to use the converted equation for ampere-turns. Thus,

ee_001-210.png (7-8)

where B = flux density, in lines per square inch; I = length of gap, in inches.




Last Update: 2010-10-06