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INTRODUCTION TO MACHINERY PRINCIPLES

                             INTRODUCTION TO MACHINERY PRINCIPLES          2.3

            H   represents effort exerted by current to establish a magnetic field
            	   represents relative ease of establishing a magnetic field in a given material
            In SI, the units are as follows:  H ampere-turns per meter;  	 henrys/meter (H/m);  B
                   2
            webers/m , known as teslas (T). And 	 is the permeability of free space. Its value is
                                        0
                                     	   4   10 
7  H/m
                                      0
              The relative permeability compares the magnetizability of materials. For example, in mod-
            ern machines, the steels used in the cores have relative permeabilities of 2000 to 7000. Thus,
            for a given current, the flux established in a steel core is 2000 to 7000 times stronger than in a
            corresponding area of air (air has the same permeability as free space). Thus, the metals of the
            core in transformers, motors, and generators play an essential part in increasing and concen-
            trating the magnetic flux in the device. The magnitude of the flux density is given by
                                               	Ni
                                      B  	H
                                                l
                                                 c
            Thus, the total flux in the core in Fig. 2.1 is

                                              	NiA
                                         BA
                                                l
                                                c
            where A is the cross-sectional area of the core.


            MAGNETIC BEHAVIOR OF FERROMAGNETIC
            MATERIALS

            The magnetic permeability is defined by the equation
                                         B  	H
            The permeability of ferromagnetic materials is up to 6000 times higher than the perme-
            ability of free space. However, the permeability of ferromagnetic materials is not constant.
            Suppose we apply a direct current to the core shown in Fig. 2.1 (starting with 0 A and
            increasing the current). Figure 2.2a illustrates the variation of the flux produced in the core
            versus the magnetomotive force. This graph is known as the saturation curve or magneti-
            zation curve. At first, a slight increase in the current (magnetomotive force) results in a sig-
            nificant increase in the flux. However, at a certain point, a further increase in current results
            in no change in the flux. The region where the curve is flat is called the saturation region.
            The core has become saturated. The region where the flux changes rapidly is called the
            unsaturated region. The transition region between the unsaturated region and the saturated
            region is called the knee of the curve.
              Figure 2.2b illustrates the variation of magnetic flux density B with magnetizing inten-
            sity H. These are the equations:
                                             Ni
                                         H
                                              l
                                              c

                                         B
                                              A

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