Radar System Engineering

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398 R-F COh[PONENTS [SEC. 113 dielectric of nominal outer diameter 0.280 in. A section of the cable with the standard type N connector is shown in Fig. 11.7. The connectors match the 50-ohm impedance of the cable at 10-cm and longer wavelengths. The mismatch at 3 cm is not great. Breakdown in the connectors limits the peak power to a few kilowatts; the most common use of such cable is in test equipment. Attenuation data are given in Table 11.1. 11.3. Waveguide.—Although a metallic pipe of almost any shape will transmit or guide electromagnetic waves if their wavelength in air is short enough, rectangular tubing whose internal dimensions have a ratio between 2.0 and 2.5 has been almost universally adopted where the problem is simply the transfer of microwave energy. (Use of round guide in the special case where axial symmetry is required is discussed in a later paragraph.) A detailed understanding of the propagation of waves in a region bounded by conducting walls can only be obtained from the solution of Maxwell’s equations. Practically, however, the results of the mathematical analysisl have come to be used in a procedure which retains most of the concepts of transmission-line theory, with equivalent lumped reactance connected at suitable points to account for the effects of discontinuities. The resemblance between a rectangular waveguide and a two-wire transmission line is shown in Fig. 11.8a to 11.Sd. In Fig. 11.8a is shown a single quarter-wave stub support, analogous to the coaxial stub support described in Sec. 11.2. At the proper frequency the input impedance of the short-circuited stub is extremely high and there is no effect on the propagation of the wave on the line. In Fig. 11.8b a great many stubs, extending both ways from the two-wire line, have been added, still without affecting the propagation of the frequency in question. In Fig. 11.8c the stubs have coalesced into a rectangular tube which looks like a wave- Wide. For a single stub, a slight correction to the length is necessary to allow for the inductance of the crosspiece, but when the stubs become a solid tube, no lines of force can link the narrow side, and the quarterwave distance becomes exact. This also implies that the length of the narrow side of the tube is not critical. The two-wire transmission-line model explains how a waveguide can transmit all frequencies higher (wavelengths shorter) than that for which the quarter-wave stubs were designed. In such a case, as shown in Fig. 11.8d, the two wires”become broad busbars with only as much of the wide side of the guide given over to stubs as is required by the now shorter wavelength. However, wavelengths greater than twice the broad dimension cannot be propagated because then the stubs become less Waveguide Handbook, Vol. 10; Microwave Trammi.ssimi Circuits, Vol. 9.
SEC,113] JVA VEGUIDE 399 than a quarter wave and shunt the line with a rather low inductive impedance which would stop transmission. Sngle stub suPPort Multiple stubs - Shortened stubs for higher frequency FIG. 11 X.—Waveguide derived from stub-supported two-wire tranmnission line. El ‘ ‘“‘ “‘‘ ‘a) I 111 I I , (b) FIQ. l19.-Fundamentaln,odeo fwavepropagationi na rectangularguide; (a) and (b) show the electric field in a transverse and longitudinal cross section; (c) shows the lin& of current flow in the top and side of the waveguide as long dashes; the dotted lines represent tangential magnetic field at the wall. Figure 11.9 shows an instantaneous picture of the electric and magnetic fields in a rectangular waveguide whose wide dimension is slightly over half the free-space wavelength. The lines of current flow in the
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CHAPTER 1 INTRODUCTION BY LOUIS N.
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4 IN TRODUC7”ION [SEC.1.2 flik~c
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6 INTRODUCTION [SEC.1.3 pulse leaki
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8 INTRODUCTION [SEC.1.4 antenna is
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10 INTRODUCTION [SEC.14 step in out
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12 INTRODUCTION [SEC.1.5 where high
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14 INTRODUCTION [SEC.1.6 England, F
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16 INTRODUCTION [SEC.1°7 Microwave
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CHAPTER 2 THE lU.DAR EQUATION BY E.
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20 THE RADAR EQUATION [SEC.22 radia
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22 THE RADAR EQUATION [SEC.25 Again
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24 THE RADAR EQUATION [SEC.2.5 time
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26 THE RADAR EQUATION [SEC.2.5 smal
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28 THE RADAR EQUATION [SEC.!2.7 lim
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30 THE RADAR EQUATION [SEC.28 Anoth
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32 THE RADAR EQUATION [SEC.28 first
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34 TIIE RADAR EQUATION [Sm. 29 the
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36 THE RADAR EQUATION [SEC.2.10 (Vo
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38 THE RADAR EQUATION [SEC.210 prac
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40 THE RADAR EQUATION [SEC.2.10 tai
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42 THE RADAR EQUATION [SEC.2.11 swe
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44 THE RADAR EQUATION [SEC.2.11 res
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46 THE RADAR EQUATION [SEC.211 Alth
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48 THE RADAR EQUATION [SEC.212 othe
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50 THE RADAR EQUATION [SEC.212 The
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52 THE RADAR EQUATION [SEC. 2.12 Th
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54 THE RADAR EQUATION [SEC.213 smal
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56 THE RADAR EQUATION [SEC. 2.14 an
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58 THE RADAR EQUATION [SEC.2.15 not
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60 TIIE RADAR EQUATION [SEC.2.15 wt
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62 THE RADAR EQUATION [SEC.215 per
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64 PROPERTIES OF RADAR TARGETS [SEC
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66 PROPERTIES OF RADAR TARGET,S [SE
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PROPERTIES OF RADAR TARGETS [SEC.37
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88 PROPERTIES OF R.41~.l R T.-lRGE~
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92 PROPERTIES OF RA1l.4R TARGETS [S
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SEC.315] STRUCTURES 99 example, the
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SF,C. 3.16] CITIES 101 reflection w
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SEC. 3.16] CITIES 103 signal repres
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SEC. 3.16] CITIES 105 four signals
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108 PROPERTIES OF RADAR TARGETS [SE
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112 PROPERTIES OF RADAR TARGETS [SE
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CHAPTER 4 LIMITATIONS OF PULSE RADA
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118 LIMITATIONS OF PULSE RADAR [SEC
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122 LIMITATIONS OF PC’LSE RADAR [
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Page 128 and 129:
128 C-W RADAR SYSTEMS [SEC. 5.1 tar
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130 C-W RADAR SYSTEMS [sm. 53 point
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132 C-W RADAR S’YSTEMS [SEC.56 bi
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134 C-W RADAR SYSTEMS [SEC. 56 tran
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136 C-W RADAR SYSTEMS [SEC. 5.6 int
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138 C-W RADAR SYSTEMS [SEC, 5.6 rel
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140 C-W RADAR SYSTEMS [SEC 37 and j
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142 C-II’ RADAR SYSTEMS [SEC. 57
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144 C-W RADAR SYSTE.JfS [SEC. 58 gi
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146 C-W RADAR SYSTEMS [SEC. 58 Modu
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148 C-T RA DAR S YSTE.lf S [SEC. 59
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150 C-W RADAR SYSTEMS [SEC. 5.11 cy
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152 C-W RADAR SYSTEMS [SEC.5.11 Now
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154 C-W RADAR SYSTEMS [SEC.5.11 exc
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156 C-W RADAR SYSTEMS [SEC. 5.11 in
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158 C-W RADAR SYSTEMS [SEC. 5.12 Pu
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CHAPTER 6 THE GATHERING AND PRESENT
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162 THE GATHERING AND PRESENTATION
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168 THE GATHERING AND pRESENTA TION
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~70 THE GATHERING AND PRESENTA TION
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SEC. 66] PLANE DISPLAYS INVOLVING E
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SEC. 69] IiARLY AIRCRAFT-WARNING RA
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SEC. 69] EARLY AIRCRAFT-WARNING RAD
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f$Ec. 69] EARLY AIRCRAFT-WARNING RA
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SEC. 6.9] EARLY AIRCRAFT-WARNING RA
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SEC. 6.10] PPI RADAR FOR SEARCH, CO
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SEC. 6.11] HEIGHT-FINDING INVOLVING
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SEC.6.12] HEIGHT-FINDING WITH A FRE
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- - -— . .. —-— - .. —-.
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SEC. 612] HEIGHT-FINDING J~ITH A FR
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SEC. 6.13] HOMING 197 ber of the pa
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SEC.6.13] HOMING 199 usually made t
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SEC. 6.13] HOMING 201 application,
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SEC. 6.14] PRECISION TRACKING OF A
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SEC.6.14] PRECISION TRACKING OF A S
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SEC. 614] PRECISION TRACKING OF A S
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f$Ec. 614] PRECISION TRACKING OF A
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SEC. 615] PRECISION TRACKING DURING
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CHAPTER 7 THE EMPLOYMENT OF RADAR D
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SEC.72] AIDS TO INDIVIDUAL NAVIGATI
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SEC. 7.2] AIDS TO INDIVIDUAL NAVIGA
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SEC. 73] AIDS TO PLOTTING AND CONTR
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SEC.7.3] AIDS TO PLOTTING AND CONTR
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SEC.7.3] AIDS TO PLOTTING AND CONTR
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SEC. 7.4] THE RELAY OF RADAR DISPLA
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SEC. 7.51 RA DAR IN THE RAF FIGHTER
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SEC. 7.6] THE U.S. TACTICAL AIR COM
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SEC.7.6] THE U.S. TACTICAL AIR COMM
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238 THE EMPLOYMENT OF RA DAR DATA [
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240 THE EMPLOYiWENT OF RADAR DATA [
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242 THE EMPLOYMENT OF RADAR DATA [S
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244 RADAR BEACONS [SEC. 8 duration
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246 RADAR BEACONS [SEC. 8.1 beacons
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248 RADAR BEACONS [SEC.8.1 4. Porta
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250 RADAR BEACONS [SEC.8.2 Table 8.
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252 RADAR BEACONS [SEC.84 restricte
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254 RADAR BEACONS [SEC. 85 radar se
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256 RADAR BEACONS [SEC.85 In the ca
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258 It Al)AIt BEACONS [S,,c, S3 Sim
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SEC. 86] FREQUENCY CONSIDERATIONS 2
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SEC. 87] INTERR~A TION CODES 263 wi
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SEC. 8.9] TRAFFIC CAPACITY 265 diff
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SEC.8.9] TRAFFIC CAPACITY 267 which
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270 RADAR BEACONS [SEC. 810 range a
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272 ANTENNAS, SCANNERS, A.VD STABIL
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274 ANTENNAS, SCANNERS, AND ST ABIL
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276 ANTENNAS, SCANNERS, AND STABILI
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SEC. 913] THE AN/APQ-7 (EAGLE) SCAN
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SEC.913] THE AN/APQ-7 (EAGLE) SCANN
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SEC. 9.14] SCHWA RZSCHILD ANTENNA 2
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SEC. 9.14] SCH WA RZSCHILD ANTENNA
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SEC. 9.15] SCI HEIGHT FINDER 299 de
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SEC.9.15] SCI HEIGHT FINDER 301 In
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SEC.916] OTHER TYPES OF ELECTRICAL
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SEC,9.17] STABILIZATION OF THE BEAM
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SEC. 9.17] STABILIZATION OF’ THE
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SEC. 9.17] STABILIZATION OF THE BEA
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t$Ec. 9,18] DATA STABILIZATION 311
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SEC. 920] INSTALLATION OF SURFACE-B
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SEC. 922] STREA MLIA”ING 315 func
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SEC. 9.25] EXAMPLES OF RADOMES 317
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SEC.9.25] EXAMPLES OF RADOMES 319 a
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SEC. 10.1] CONSTRUCTION 321 of the
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SEC. 10.1] CONSTRUCTION 323 later r
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SEC.10.2] THE RESONANT SYSTEM 325 m
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SEC. 1021 THE RESONANT SYSTEM 327
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SEC. 10.2] THE RESONANT SYSTEM 329
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SEC. 103] ELECTRON ORBITS AIVD THE
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SEC. 103] ELECTRON ORBITS AND THE S
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SEC. 103] ELECTRON ORBITS AND THE S
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SEC. 10.4] PERFORMANCE CHARTS AND R
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SEC. 10.4] PEIWORMilNCE CHARTS AND
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SEC. 10.5] MAGNETRON CHARACTERISTIC
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SEC.105] MAGNETRON CHARACTERISTICS
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SEC. 105] MAGNETRON CHARACTERISTICS
Page 347 and 348: SEC. 105] MAGNETRON CHARACTERISTICS
Page 349 and 350: SEC. 105] MAGNETRON CHARACTERISTICS
Page 351 and 352: SEC. 10.5] MAGNETRON CHARACTERISTIC
Page 353 and 354: SEC. 10.6] MAQNETRON CHARACTERISTIC
Page 355 and 356: L%C. 10.6] MAGNETRON CHARACTERISTIC
Page 357 and 358: SEC. 10.7] PULSER CIRCUITS 357 and
Page 359 and 360: SEC. 10.7] PULSER CIRCUITS 359 tude
Page 361 and 362: SEC. 10.7] PULSER CIRCUITS 361 cen~
Page 363 and 364: SEC. 108] LOAD REQUIREMENTS 363 TAB
Page 365 and 366: SEC. 10.8] LOAD REQUIREMENTS 365 to
Page 367 and 368: SEC. 109] THE HARD-TUBE P ULSEh? 36
Page 369 and 370: SEC. 10.9] THE HARD-TUBE P ULSER 36
Page 371 and 372: SEC 10.9] THE HARD-lUBE PULSER 371
Page 373 and 374: Sl?lc.10.91 LINE-TYPE PULSERS 373 D
Page 375 and 376: SEC. 10,10] LINE-TYPE PULSERS 375 i
Page 377 and 378: SEC. 10.10] LINE-TYPE PULSERS 377 I
Page 379 and 380: SEC. 10.10] LINE-T YPE PULSERS 379
Page 381 and 382: SEC. 10.10] LINE-TYPE PULSERS 381 T
Page 383 and 384: SEC.10.11] MISCELLANEOUS COMPONENTS
Page 387 and 388: SEC. 1011] MISCELLANEOUS COMPONENTS
Page 391 and 392: R-F CHAPTER 11 COMPONENTS BY A. E.
Page 393 and 394: SEC.11.2] COAXIAL LINES 393 Why a M
Page 395 and 396: SEC.11.2] COAXIAL LINES 395 lines h
Page 397: SEC.11.2] COAXIAL LINES 397 since n
Page 401 and 402: i?EC. 11.3] WA VEGUIDE 401 too grad
Page 403 and 404: SEC. 113) WA VEGUIDE 403 types of m
Page 405 and 406: SEC. 11.4] RESONANT CAVITIES 405 co
Page 407 and 408: SEC. 11.5] D,C”PLEXING AND TR SWI
Page 409 and 410: SEC. 115] DUPLEXING AND TR SWITCHES
Page 411 and 412: SEC. 11.5] DUPLEXING AND TR SWITCHE
Page 413 and 414: SEC.11.6] THE MIXER CRYSTAL 413 sem
Page 415 and 416: SEC. 11.7] THE LOCAL OSCILLATOR 415
Page 417 and 418: SEC. 11 .8] THE MIXER 417 minimum l
Page 419 and 420: SEC.11.10] REASONS FOR AN R-F PACKA
Page 421 and 422: SEC. 11.11] DESIGN CONSZDERA TZONS
Page 423 and 424: SEC.11.11] DESIGN CONSIDERATIONS FO
Page 425 and 426: SEC. 11.12] ILLUSTRATIVE EXAMPLES O
Page 427 and 428: SEC. 11°12] ILL US’TRA TIVE EXAM
Page 429 and 430: SEC. 11.12] ILL USTRA TIVE EXAMPLES
Page 431 and 432: SEC.11.12] ILL US1’IiA TI VE EXA
Page 433 and 434: CHAPTER 12 THE RECEIVING SYSTEM—R
Page 435 and 436: SEC. 122] A TYPICAL RECEIVING SYSTE
Page 437 and 438: SEC.12.2] A TYPICAL RECEIVING SYSTE
Page 439 and 440: SEC. 122] A TYPICAL RECEIVING SYSTE
Page 441 and 442: SEC.12.3] SPECIAL PROBLEMS IN RADAR
Page 443 and 444: SEC.12.4] I-F AMPLIFIER DESIGN 443
Page 445 and 446: SEC.12.4] I-F AMPLIFIER DESIGN 445
Page 447 and 448: SEC.124] I-F AMPLIFIER DESIGN 447 i
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SEC. 125] SECOND DETECTOR 449 This
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SEC.12.6] VIDEO AMPLIFIERS 451 ampl
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SEC.12.7] A UTOMA TIC FREQUENCY CON
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SEC. 12.7] A UTOMA TIC FREQUENCY CO
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S~C. 128] PROTECTION AGAINST EXTRAN
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SEC. 128] PROTECTION AGAINST EXTRAN
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SEC. 12.8] PROTECTION AGAINST E-YTR
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&- L,-self resonant COIIS at mterme
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J All resistors~ watt Interstate co
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SEC. 12.10] LIGHTH”EIGIIT AIRBOR.
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s, 0.001 $180 b To reflector To sea
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+ 180v T +120V 470 470 470 470 e“
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SEC.12.11] AN EXTREMELY WIDEBAND RE
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CHAPTER 13 THE RECEIVING SYSTEM—I
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SEC.13.1] ELECTRICAL PROPERTIES OF
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SEC 13.2] CATHODE-RAY TUBE SCREENS
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SEC.13.2] CATHODE-RAY TUBE SCREENS
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SEC. 13.3] SELECTIO.V OF THE CATHOD
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SEC. 13.3] SELECTION OF THE CATHODE
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SEC. 13.4] ANGLE-DATA TRANSMITTERS
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SEC.13.4] ANGLE-DATA TRANSMITTERS 4
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SEC. 13.5] ELECTROMECHANICAL REPEAT
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SEC. 13.6] AMPLIFIERS 493 whence th
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SEC. 13.6] AMPLIFIERS 495 by using
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SEC. 13.7] GENERA TION OF RECTANGUL
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SEC. 13.7] GENERATION OF RECTANGULA
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. SEC. 13.8] GENERA TION OF SHARP P
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SEC. 139] ELECTRONIC SWITCHES 503 T
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SEC. 13.9] ELECTRONIC SWITCHES 505
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SEC. 13.9] ELECTRO.VIC ISWI TCHES 5
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SEC. 13.9] ELECTRONIC SWITCHES 509
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SEC. 1310] SAWTOOTH GENERATORS 511
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SEC.13.10] SAWTOOTH GE,VBliATOh?S 5
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SEC. 1311] ANGLE INDICES 515 bright
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SEC. 13.11] ANGLE INDICES 517 the s
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. . “4 100k.lw $4.7k-lw .& t, T 0
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SEC.K3.121 RANGE AND HEIGIiT INDICE
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i%C.13121 RANGE AND HEIGHT INDICES;
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SEC. 13.13] DESIGN OF A-SCOPES 525
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SEC. 1313] DESIGN OF A-SCOPES 527 f
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SEC.1314] B-SCOPE DESIGN 529 \
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SEC. 13.14] B-SCOPE DESIG.V 531 wil
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Trigger I I I (CT)Sawtooth —. (A)
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SEC.1316] RESOLVED TIME BASE PPI 53
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SEC. 13.16] RESOLVED mi? TIME BASE
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SEC. 13.17] RESOLVED-CURRENT PPI 53
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SEC. 13.17] RESOLVED-CURRENT PPI 54
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+ 200V— — — J 60k . Llk )k 60
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SEC. 13.19] 1’HE RANGB-ll EIGII1
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SEL!. 13.19] THE RANGE-HEIGHT INDIC
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SEC. 13.20] RESOLUTION AND CONTRAST
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SEC. 13.211 SPECIAL RECEIVING TECHN
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554 THE RECEIVING SYSTEM-INDICATORS
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556 PRIME POWER SUPPLIES FOR RADAR
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. . . 0.9 P~- 860-’CPS CF over 2
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Page 562 and 563:
562 PRIME POWER SLTPPLIES FOR RADAR
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SEC. 14.6] SPEED REGULATORS 575 ‘
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SEC. 146] SPEED REGULATORS 577 havi
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SEC. 14.7] DYNAMOTORS 579 14.7. Dyn
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SEC.14.8] VIBRATOR POWER SUPPLIES 5
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SEC. 1410] FIXED LOCATIONS 583 port
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SEC. 14.13] ULTRAPORTABLE UNITS 585
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SEC. l’k~~] SHIP RADAR SYSTEMS 58
Page 589 and 590:
SEC. 151] INTRODCCTIO,\- 589 the pr
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SEC, 152] NEED FOR SYSTEM TESTING 5
Page 593 and 594:
SEC, 153] INITIAL PLANNING AND OBJE
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SEC. 15.4] THE RANGE EQUATION 595 n
Page 597 and 598:
SEC. 15.5] CHOICE OF PULSE LENGTH 5
Page 599 and 600:
SEC. 15.7] AZIMUTH SCAN RATE 599 to
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SEC. 15.8] CHOICE OF BEAM SHAPE 601
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SEC. 15.8] CHOICE OF BEAM SHAPE 603
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SEC. 15.9] CHOICE OF WAVELENGTH 605
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SEC. 15.10] COMPONENTS DESIGN 607 1
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SEC.16.11] MODIFICA TIO.VS A,YD ADD
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SEC. 15.12] DESIGN OBJECTIVES AND L
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SEC. 15.12] DESIGN OBJECTIVES AND L
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SEC. 15.13] GENERAL DESIGN OF THE A
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SEC. 15.14] DETAILED DESIGN OF THE
Page 619 and 620:
SEC. 15.14] DETAILED DESIGN OF THE
Page 621 and 622:
,/ / /“)4 Providenc~ (b) Fm. 16.1
Page 624 and 625:
624 EXAMPLES OF RADAR SYSTEM DESIGN
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CHAPTER 16 MOVING-TARGET INDICATION
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628 MOVING-TARGET INDICATION [SEC,
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630 MOVING-TARGET INDICATION [SEC.
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632 MOVING TARGET INDICATION [SEC.
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Page 646 and 647:
. 646 MOVING- TARGET INDICATION [SE
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648 MOVING- TARGET lNDICA TION [SEC
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Page 652 and 653:
652 MOVING-TARGET INDICATION [SEC 1
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656 MOVING-TARGET INDICATION [SEC.1
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658 When o = Othe instead MOVING-TA
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662 MOVING TARGET INDICATION [SEC.1
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670 MO VINGTARGET INDICATION [SEC.
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672 MOVING TARGET INDICATION [SEC.1
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674 MOVING- TARGET INDICATION [SEC.
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676 MOVING-TARGET INDICATION ~SEC.
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Page 680 and 681:
CHAPTER 17 RADAR RELAY BY L. J. HAW
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682 RADAR RELAY [SEC. 172 transmitt
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684 RADAR RELAY [SEC. 17.3 staggeri
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686 RADAR RELAY [SEC. 17.4 excluded
Page 688 and 689:
688 RADAR RELAY [SEC. 174 long sign
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h Video I 1 I Angle marks RADAR REL
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692 [SEC. 175 ḇ 1 1 1 I ~ LKal tr
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694 RADAR RELAY [SEC. 17.5 generato
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696 RADAR RELAY [SEC. 17.6 station
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698 RADAR RELAY [SEC. 17.6 Video si
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700 RADAR RELAY [SEC. 176 train. Th
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702 RADAR RELAY [SEC.17.7 be obtain
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704 RADAR RELAY @EC. 17.7 illustrat
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[11 1 Bas,c pulse I %e pulse i ~--.
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708 RADAR ltELA Y [SEC. 1743 wave f
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710 RADAR RELAY [SEC. 17.8 actual m
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. 712 RADAR RELAY [SEC. 17.9 Such a
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714 RADAR RELAY [SEC. 17.10 between
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716 RADAR RELAY [SEC. 17.10 signal
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718 RADAR RELAY [SEC. 17.11 suppres
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720 RADAR RELAY [SEC. 17.12 provide
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722 RADAR RELAY [SEC. 17.13 relay l
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724 RADAR RELAY [SEC. 17.14 TaLE 17
Page 726 and 727:
726 RADAR RELAY [SEC. 17.15 RADAR R
Page 728 and 729:
728 RADAR RELAY [SEC. 17.15 Modulat
Page 730 and 731:
730 RADAR RELAY [SEC. 17.15 the sec
Page 732 and 733:
732 RADAR RELAY [SEC. 17.10 pulses
Page 734 and 735:
734 RADAR RELAY [f+iEc.17.16 The vi
Page 737 and 738:
Index A Absorbent materials, 69 Abs
Page 739 and 740:
INDEX 739 B-scope, electrostatic, 5
Page 741 and 742:
INDEX 741 Fairbank, W. M.,80 F Fan
Page 743 and 744:
INDEX ’743 Microwave, reason for
Page 745 and 746:
INDEX 745 Radar, pulse,3 range perf
Page 747 and 748:
INDEX 747 Signal, interference of,
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Radar System Engineering

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