微波工程第三版英文原版pptch09

Microwave Engineering, 3rd Edition by David M. Pozar Copyright © 2004 John Wiley & Sons
Figure 9-15 (p. 472)
Geometry of a nonreciprocal latching phase shifter using a ferrite toroid.
Figure 9-17 (p. 474)
Differential phase shift for the two-slab remanent phase shifter of Example 9.4.
Microwave Engineering, 3rd Edition by David M. Pozar Copyright © 2004 John Wiley & Sons
Figure 9-4a (p. 451)
Complex susceptibilities for a typical ferrite. (a) Real and imaginary parts of xxx. (b) Real and imaginary parts of xxy.
Microwave Engineering, 3rd Edition by David M. Pozar Copyright © 2004 John Wiley & Sons
Figure 9-1 (p. 443)
Spin magnetic dipole moment and angular momentum vectors for a spinning electron.
Microwave Engineering, 3rd Edition by David M. Pozar Copyright © 2004 John Wiley & Sons
Microwave Engineering, 3rd Edition by David M. Pozar Copyright © 2004 John Wiley & Sons
Figure 9-10 (p. 464)
Geometry of a rectangular waveguide loaded with two symmetrical ferrite slabs.
Figure on page 454
Microwave Engineering, 3rd Edition by David M. Pozar Copyright © 2004 John Wiley & Sons
Figure 9-7 (p. 458)
Normalized phase and attenuation constants for circularly polarized plane waves in the ferrite medium of Example 9.1.
Microwave Engineering, 3rd Edition by David M. Pozar Copyright © 2004 John Wiley & Sons
Figure 9-11 (p. 466)
Two resonance isolator geometries. (a) E-plane, full-height slab. (b) H-plane slab.
Figure 9-3 (p. 449)
Forced procession of a magnetic dipole with circularly polarized fields. (a) RHCP, M > H. (b) M < H.
Microwave Engineering, 3rd Edition by David M. Pozar Copyright © 2004 John Wiley & Sons
Microwave Engineering, 3rd Edition by David M. Pozar Copyright © 2004 John Wiley & Sons
Figure 9-23 (p. 478)
A stripline junction circulator. (a) Pictorial view. (b) Geometry.
Microwave Engineering, 3rd Edition by David M. Pozar Copyright © 2004 John Wiley & Sons
Figure 9-9 (p. 461)
Geometry of a rectangular waveguide loaded with a transverely biased ferrite slab.
Figure 9-6 (p. 452)
Internal and external fields for a thin ferrite plate. (a) Normal bias. (b) Tangential bias.
Microwave Engineering, 3rd Edition by David M. Pozar Copyright © 2004 John Wiley & Sons
Figure 9-21 (p. 476)
An isolator constructed with a gyrator and two quadrature hybrids. The forward wave () is passed, while the reverse wave () is absorbed in the matched load of the first hybrid.
Microwave Engineering, 3rd Edition by David M. Pozar Copyright © 2004 John Wiley & Sons
Figure 9-13 (p. 469)
Geometry and electric fields of a field displacement isolator.
Symbol for a gyrator, which has a differential phase shift of 180°.
Microwave Engineering, 3rd Edition by David M. Pozar Copyright © 2004 John Wiley & Sons
Figure 9-18 (p. 475)
Nonreciprocal Faraday rotation phase shifter.
Microwave Engineering, 3rd Edition by David M. Pozar Copyright © 2004 John Wiley & Sons
Figure 9-19 (p. 475)
Reggia-Spencer reciprocal phase shifter.
Microwave Engineering, 3rd Edition by David M. Pozar Copyright © 2004 John Wiley & Sons
Figure 9-20 (p. 476)
Microwave Engineering, 3rd Edition by David M. Pozar Copyright © 2004 John Wiley & Sons
Figure 9-8 (p. 460)
Effective permeability, e, versus bias field H0, for various saturation magnetizations and frequencies.
Microwave Engineering, 3rd Edition by David M. Pozar Copyright © 2004 John Wiley & Sons
Figure 9-12 (p. 468)
Forward and reverse attenuation constants for the resonance isolator of Example 9.2. (a) Versus slab position. (b) Versus frequency.
Microwave Engineering, 3rd Edition by David M. Pozar Copyright © 2004 John Wiley & Sons
Figure 9-14 (p. 470)
Propagation constants and electric field distribution for the field displacement isolator of Example 9.3. (a) Forward and reverse propagation constants versus slab position. (b) Electric field amplitudes for the forward and reverse waves.
Microwave Engineering, 3rd Edition by David M. Pozar Copyright © 2004 John Wiley & Sons
Figure 9-22 (p. 477)
Photograph of a disassembled ferrite junction circulator, showing the stripline conductor, the ferrite disks, and the bias magnet. The middle port of the circulator is terminated with a matched load, so this circulator is actually configured as an isolator. Note the change in the width of the stripline conductors, due to the different dielectric constants of the ferrite and the surrounding plastic material.
Figure 9-5 (p. 451)
Definition of the linewidth, H, of the gyromagnetic resonance.
Microwave Engineering, 3rd Edition by David M. Pozar Copyright © 2004 John Wiley & Sons
Microwave Engineering, 3rd Edition by David M. Pozar Copyright © 2004 John Wiley & Sons
Microwave Engineering, 3rd Edition by David M. Pozar Copyright © 2004 John Wiley & Sons
Figure 9-16 (p. 472)
A hysteresis curve for a ferrite toroid.
Microwave Engineering, 3rd Edition by David M. Pozar Copyright © 2004 Johnபைடு நூலகம்Wiley & Sons
Figure 9-2 (p. 445)
Magnetic moment of a ferrimagnetic material versus bias field, H0.
Microwave Engineering, 3rd Edition by David M. Pozar Copyright © 2004 John Wiley & Sons