Radar System Engineering

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336 THE MAGNETRON AND THE P ULSER [SEC. 10.4 anode segments and thus transferring charge from the cathode to the anode. The r-f current set up in the oscillators isprincipally a displacement current produced by this rotating space charge. As the spokes of the negative space charge pass in front of an anode segment, a positive charge is induced on its surface. Half a period later, this positive charge has flowed around the back of the two adjacent oscillators to the two adj scent anode segments and the spoke of the space charge has rotated to a position in front of the next anode segment. In addition to these displacement currents, conduction currents are produced by the flow of electrons from space charge to the anode. Electrons arrive at the anode at such a time as to constitute a conduction current approximately 90° out of phase with the r-f voltage, and thus have little effect on the oscillations. 10.4. Performance Charts and Rieke Diagrams.-Four parameters determine the operation of the magnetron; two are associated with the input circuit, and two with the output circuit. A typical set is H, I, G, and B. H is the magnetic field, 1 is the anode current, and G and B are the real and the imaginary parts of the r-f load on the magnetron measured at some arbitrary point in the output line. The observed quantities are three in number, usually power P, wavelength A, and voltage V. The problem of presenting these observed quantities in terms of the four parameters is greatly simplified by the fact that the input and output parameters operate nearly independently of one another. Thus, it is possible to keep G and B (the load) fixed, and study the effect of H and 1 on P, k, and V withthe assurance that the nature of the results will not be greatly altered by changes in G and B. Conversely, H and 1 may be fixed and the effect of G and B on P, A, and V observed. As a result of this situation, it is customary to present the operating data on two graphs. One is called the “performance chart,” and shows the relationship between H, I, V, P, and X for constant load; the other is called a “ Rieke diagram,” and shows the relationships between G, B, P, k, and V for constant I and H. Figure 10c16 is a performance chart for a typical magnetron with a frequency of about 2800 Me/see. It has been customary to plot anode voltage V as ordinate, and current 1 as abscissa. On such a graph the lines of constant H are more or less parallel and slope upward to the right. Thus (referring to Fig. 10. 16), if the magnetron is operated at a constant magnetic field, say 2100 gauss, the relations of voltage and current are given by points on the H = 2100 gauss line. (At 20 kv, the current drawn will be 48 amp.) On the same chart are plotted the lines of constant power output. These are the solid lines whose form suggests hyperbolas; they show the
SEC. 10.4] PERFORMANCE CHARTS AND RIEKE DIAGRAMS 337 pulse r-f power which is obtained under varying input conditions. Thus at 20 kv and 48 amp, the power output is 470 kw. This same power can also be obtained at 25 kv and 30 amp with a magnetic field a little less than 2700 gauss. In addition, it is customary to add curves of constant efficiency obtained directly from the above data. These lines of constant efficiency are the dotted lines looping up and to the right on the diagram. 10 1 1 1 o 10 20 30 40 50 60 70 80 — CurrentInamperes
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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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Page 286 and 287: 286 ANTENNAS, SCANNERS, AND STABILI
Page 288: 288 ANTENNAS, SCANNERS, AND STABILI
Page 291 and 292: SEC. 913] THE AN/APQ-7 (EAGLE) SCAN
Page 293 and 294: SEC.913] THE AN/APQ-7 (EAGLE) SCANN
Page 295 and 296: SEC. 9.14] SCHWA RZSCHILD ANTENNA 2
Page 297 and 298: SEC. 9.14] SCH WA RZSCHILD ANTENNA
Page 299 and 300: SEC. 9.15] SCI HEIGHT FINDER 299 de
Page 301 and 302: SEC.9.15] SCI HEIGHT FINDER 301 In
Page 303 and 304: SEC.916] OTHER TYPES OF ELECTRICAL
Page 305 and 306: SEC,9.17] STABILIZATION OF THE BEAM
Page 307 and 308: SEC. 9.17] STABILIZATION OF’ THE
Page 309 and 310: SEC. 9.17] STABILIZATION OF THE BEA
Page 311 and 312: t$Ec. 9,18] DATA STABILIZATION 311
Page 313 and 314: SEC. 920] INSTALLATION OF SURFACE-B
Page 315 and 316: SEC. 922] STREA MLIA”ING 315 func
Page 317 and 318: SEC. 9.25] EXAMPLES OF RADOMES 317
Page 319 and 320: SEC.9.25] EXAMPLES OF RADOMES 319 a
Page 321 and 322: SEC. 10.1] CONSTRUCTION 321 of the
Page 323 and 324: SEC. 10.1] CONSTRUCTION 323 later r
Page 325 and 326: SEC.10.2] THE RESONANT SYSTEM 325 m
Page 327 and 328: SEC. 1021 THE RESONANT SYSTEM 327
Page 329 and 330: SEC. 10.2] THE RESONANT SYSTEM 329
Page 331 and 332: SEC. 103] ELECTRON ORBITS AIVD THE
Page 333 and 334: SEC. 103] ELECTRON ORBITS AND THE S
Page 335: SEC. 103] ELECTRON ORBITS AND THE S
Page 339 and 340: SEC. 10.4] PEIWORMilNCE CHARTS AND
Page 341 and 342: SEC. 10.5] MAGNETRON CHARACTERISTIC
Page 343 and 344: SEC.105] MAGNETRON CHARACTERISTICS
Page 345 and 346: 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 385 and 386: SEC.10.11] MISCELLANEOUS COMPONENTS
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SEC. 1011] MISCELLANEOUS COMPONENTS
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SEC.10.11] MISCELLANEOUS COMPONENTS
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R-F CHAPTER 11 COMPONENTS BY A. E.
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SEC.11.2] COAXIAL LINES 393 Why a M
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SEC.11.2] COAXIAL LINES 395 lines h
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SEC.11.2] COAXIAL LINES 397 since n
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SEC,113] JVA VEGUIDE 399 than a qua
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i?EC. 11.3] WA VEGUIDE 401 too grad
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SEC. 113) WA VEGUIDE 403 types of m
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SEC. 11.4] RESONANT CAVITIES 405 co
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SEC. 11.5] D,C”PLEXING AND TR SWI
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SEC. 115] DUPLEXING AND TR SWITCHES
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SEC. 11.5] DUPLEXING AND TR SWITCHE
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SEC.11.6] THE MIXER CRYSTAL 413 sem
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SEC. 11.7] THE LOCAL OSCILLATOR 415
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SEC. 11 .8] THE MIXER 417 minimum l
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SEC.11.10] REASONS FOR AN R-F PACKA
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SEC. 11.11] DESIGN CONSZDERA TZONS
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SEC.11.11] DESIGN CONSIDERATIONS FO
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SEC. 11.12] ILLUSTRATIVE EXAMPLES O
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SEC. 11°12] ILL US’TRA TIVE EXAM
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SEC. 11.12] ILL USTRA TIVE EXAMPLES
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SEC.11.12] ILL US1’IiA TI VE EXA
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CHAPTER 12 THE RECEIVING SYSTEM—R
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SEC. 122] A TYPICAL RECEIVING SYSTE
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SEC.12.2] A TYPICAL RECEIVING SYSTE
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SEC. 122] A TYPICAL RECEIVING SYSTE
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SEC.12.3] SPECIAL PROBLEMS IN RADAR
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SEC.12.4] I-F AMPLIFIER DESIGN 443
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SEC.12.4] I-F AMPLIFIER DESIGN 445
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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
Page 475 and 476:
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
Page 560 and 561:
Page 562 and 563:
562 PRIME POWER SLTPPLIES FOR RADAR
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Page 570 and 571:
Page 572:
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SEC. 14.6] SPEED REGULATORS 575 ‘
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SEC. 146] SPEED REGULATORS 577 havi
Page 579 and 580:
SEC. 14.7] DYNAMOTORS 579 14.7. Dyn
Page 581 and 582:
SEC.14.8] VIBRATOR POWER SUPPLIES 5
Page 583 and 584:
SEC. 1410] FIXED LOCATIONS 583 port
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SEC. 14.13] ULTRAPORTABLE UNITS 585
Page 587 and 588:
SEC. l’k~~] SHIP RADAR SYSTEMS 58
Page 589 and 590:
SEC. 151] INTRODCCTIO,\- 589 the pr
Page 591 and 592:
SEC, 152] NEED FOR SYSTEM TESTING 5
Page 593 and 594:
SEC, 153] INITIAL PLANNING AND OBJE
Page 595 and 596:
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
Page 601 and 602:
SEC. 15.8] CHOICE OF BEAM SHAPE 601
Page 603 and 604:
SEC. 15.8] CHOICE OF BEAM SHAPE 603
Page 605 and 606:
SEC. 15.9] CHOICE OF WAVELENGTH 605
Page 607 and 608:
SEC. 15.10] COMPONENTS DESIGN 607 1
Page 609 and 610:
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
Page 617 and 618:
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
Page 626 and 627:
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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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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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
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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
Page 710 and 711:
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
Page 718 and 719:
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
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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
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INDEX 739 B-scope, electrostatic, 5
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INDEX 741 Fairbank, W. M.,80 F Fan
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INDEX ’743 Microwave, reason for
Page 745 and 746:
INDEX 745 Radar, pulse,3 range perf
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INDEX 747 Signal, interference of,
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Radar System Engineering

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