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Chapter 5 Magnetostatics
 
 Figures
Figure 5.1: The direction of the magnetic force exerted on a charged particle moving in a magnetic field is (a) perpendicular to both B and u and (b) depends on the charge polarity (positive or negative).
Figure 5.2: When a slightly flexible vertical wire is placed in a magnetic field directed into the page (as denoted by the crosses), it is (a) not deflected when the current through it is zero, (b) deflected to the left when I is upward, and (c) deflected to the right when I is downward.
Figure 5.3: In a uniform magnetic field, (a) the net force on a closed current loop is zero because the integral of the displacement vector dl over a closed contour is zero, and (b) the force on a line segment is proportional to the vector between the end point (Fm = IXB).
Figure 5.4:Semicircular conductor in a uniform field (Example 5-1).
Figure 5.5: The force F acting on a circular disk pivoted along the z-axis generates a torque T = dXF that causes the disk to rotate.
Figure 5.6: Rectangular loop pivoted along the y-axis: (a) front view and (b) bottom view. The combination of forces F1 and F3 on the loop generates a torque that tends to rotate the loop in a clockwise direction as shown in (b).
Figure 5.7: Rectangular loop in a uniform magnetic field with flux density B whose direction is perpendicular to the rotation axis of the loop, but makes an angle with the loop's surface normal n-hat.
Figure 5.8: Mangetic field dH generated by a current element Idl. The direction of the field induced at point P is opposite that induced at point P'.
Figure 5.9: (a) The total current crossing the cross section S of the cylinder is I = integral over S of J dot ds. (b) The total current flowing across the surface of the conductor is I= integral over l Jsdl.
Figure 5.10: Linear conductor of length l carrying a current I. (a) The field dH at point P due to incremental current element dl. (b) Limiting angles 1 and 2, each measured between vector I dl and the vector connecting the end of the conductor associated with that angle to point P (Example 5-2).
Figure 5.11: Pie-shaped loop of radius a carrying a current I (Example 5-3).
Figure 5.12: Circular loop carrying a current I (Example 5-4).
Figure 5.13: Patterns of (a) the electric field of an electric dipole, (b) the magnetic field of a magnetic dipole, and (c) the magnetic field of a bar magnet. Far away from the sources, the field patterns are similar in all three cases.
Figure 5.14: Magnetic forces on parallel current-carrying conductors.
Figure 5.15: Whereas (a) the net electric flux through a closed surface surrounding a charge is not zero, (b) the net magnetic flux through a closed surface surrounding one of the poles of a magnet is zero.
Figure 5.16: Ampere's law states that the line integral of H around a closed contour C is equal to the current traversing the surface bounded by the contour. This is true for contours (a) and (b), but the line integral of H is zero for the contour in (c) because the current I (denoted by the circle-enclosed-dot symbol) is not enclosed by the contour C.
Figure 5.17: Infinitely long wire of radius a carrying a uniform current I along the +z-direction: (a) general configuration showing contours C1 and C2; (b) cross-sectional view; and (c) a plot of H versus r (Example 5-5).
Figure 5.18: Toroidal coil with inner radius a and outer radius b. The wire loops usually are much more closely spaced than shown in the figure (Example 5-6).
Figure 5.19: A thin current sheet in the x-y plane carrying a surface current density Hs = x-hat Js (out of the page) (Example 5-7).
Figure 5.20: An electron generates (a) an orbital magnetic moment mo as it rotates around the nucleus and (b) a spin magnetic moment ms, as it spins about its own axis.
Figure 5.21: Comparison of (a) unmagnetized and (b) magnetized domains in a ferromagnetic material.
Figure 5.22:Typical hysteresis curve for a ferromagnetic material.
Figure 5.23:Comparison of hysteresis curves for (a) a hard ferromagnetic material and (b) a soft ferromagnetic material.
Figure 5.24: Bounary between medium 1 with 1 and medium 2 with 2.
Figure 5.25: Magnetic field lines of (a) a lossely wound solenoid and (b) a tightly wound solenoid.
Figure 5.26: Solenoid cross section showing geometry for calculating H at a point P on the solenoid axis.
Figure 5.27: To compute the inductance per unit length of a two-conductor transmission line, we need to determine the magnetic flux through the area S between the conductors.
Figure 5.28: Cross-sectional view of coaxial transmission line (Example 5-8).
Figure 5.29: Magnetic field lines generated by current I1 in loop 1 linking surface S2 of loop 2.
Figure 5.30:Toroidal coil with two windings used as a transformer.
Figure 5.31: Particle of charge q projected with velocity u into a medium with a uniform field B perpendicular to u (Problem 5.2).
Figure 5.32:Configuration of Problem 5.3.
Figure 5.33:Hinged rectangular loop of Problem 5.4.
Figure 5.34:Rectangular loop of Problem 5.6.
Figure 5.35:Current-carrying linear conductor of Problem 5.8.
Figure 5.36:Configuration of Problem 5.9.
Figure 5.37:Circular loop next to a linear current (Problem 5.11).
Figure 5.38:Arrangement for Problem 5.12.
Figure 5.39:Parallel circular loops of Problem 5.14.
Figure 5.40:Current loop next to a conducting wire (Problem 5.15).
Figure 5.41:Parallel conductors supported by strings (Problem 5.16).
Figure 5.42:A linear current source above a current sheet (Problem 5.17).
Figure 5.43:Three parallel wires of Problem 5.18.
Figure 5.44: Long wire carrying current I2, just above a square loop carrying I1 (Problem 5.19).
Figure 5.45:Adjacent magnetic media (Problem 5.30).
Figure 5.46:Magnetic media separated by the plane x-y=1 (Problem 5.32).
Figure 5.47:Three magnetic media with parallel interfaces (Problem 5.34).
Figure 5.48:Loop and wire arrangement for Problem 5.38.

Contents 1 2 3 4 5 6 7 8 9 index
figures4 figures6 Contents Help
Modules  Demos  Solved Problems 
Fawwaz T. Ulaby, Fundamentals of Applied Electromagnetics. Prentice Hall, Upper Saddle River, New Jersey, 2001. Copyright © 2001 Prentice Hall.