Radar System Engineering

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536 THE RECEIVING SYSTEM—INDICATORS [SEC.13.16 The first method involves the use of clamps m switches in the secondary circuit to force the potential or the current to zero in the interval between sweeps. So long as the sweep component has a given polarity, this can be very simply accomplished in the potential case by a d-c rest orer (See. 13“9), and in the current case by a selenium rectifier in series with the secondary circuit. In cases where the scanning is confined to 90° or less, these variations of the first method are the most satisfactory of all. If the scan covers more than 90°, one of the diodes must be switched in polarity from time to timefor example, by a cam arrangement on the scanner. If the scan covers more than 180° both of them must be so switched. Although it is difficult to switch quickly and smoothly enough to avoid aest heti call y displeasing display irregularities, this method is quite satisfactory and is probably the simplest for the case of resolved currents, providing the scanning rate is not too high. A better and only slightly more expensive method of voltage restoration involves the use of a double clamp (Fig. 13.25) which connects the secondary to a point of proper potential between sweeps but releases it when the sweep begins. This is the most widely used method in the voltage case when polarity reversal is involved. No satisfactory series switches exist for analogous use with resolved currents. In the second method of correcting the sweep-origin difficulty, the positive and negative waveforms are “balanced” about the sweep origin either by introducing a precisely controlled negative waveform in the primary circuit between sweeps, or by arranging to trigger the transmitter automatically at the precise time when the secondary current or voltage passes through zero. Both variations involve a good deal of precision and are more costly than the switched clamps mentioned in the last paragraph as usable when voltage is involved. However, the present methods have been widely used in connection with resolved currents, since they require no switching elements in the low-impedance secondary circuit. Applications of these various methods will be described in connection with the following specific examples. Magnetic PPI Using A mplijiers.-Figure 13.46 shows the secondary circuit of a magnetic PPI of the resolved–time-base type using the method of clamping between sweeps. It is supposed that the synchro is preceded by the sweep generator and amplifier of Fig. 13.44, except that the circuit of V6 is changed as indicated so that the feedback voltage is that across the synchro itself. The clamps on each of the amplifier grids of Fig. 13.46 are of the double-triode variety illustrated in Fig. 13.25a. They are switched by the same flip-flop (rectangular-wave generator) that controls the sawtooth generator and are thus closed during the entire interval between
SEC. 13.16] RESOLVED mi? TIME BASE 537 ‘“’’*”’’” vh,v%~ i%?. 13.44 ‘\ I r F lli!J H!$w! K T II ..- . . I L M G I L L 1 10 cathcde of v= — $● -’ --- _- From V’ ~ (Fig.13.44) I I 1 1 1 Trigger~––––––––– -------~ W~-—---––---– ““”’’(”~--------------MM ‘“’”” --~ (G) Bias . . pot. M d –--––--ll_tuuI Azimuth angle J 9b” 1!40” 2;0” 6“ Fm. 13.46.—Resolved-e.weepPPI using amplifiers.
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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
Page 64 and 65:
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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Page 88 and 89:
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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Page 168 and 169:
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
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SEC. 10.5] MAGNETRON CHARACTERISTIC
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SEC. 10.6] MAQNETRON CHARACTERISTIC
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L%C. 10.6] MAGNETRON CHARACTERISTIC
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SEC. 10.7] PULSER CIRCUITS 357 and
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SEC. 10.7] PULSER CIRCUITS 359 tude
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SEC. 10.7] PULSER CIRCUITS 361 cen~
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SEC. 108] LOAD REQUIREMENTS 363 TAB
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SEC. 10.8] LOAD REQUIREMENTS 365 to
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SEC. 109] THE HARD-TUBE P ULSEh? 36
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SEC. 10.9] THE HARD-TUBE P ULSER 36
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SEC 10.9] THE HARD-lUBE PULSER 371
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Sl?lc.10.91 LINE-TYPE PULSERS 373 D
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SEC. 10,10] LINE-TYPE PULSERS 375 i
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SEC. 10.10] LINE-TYPE PULSERS 377 I
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SEC. 10.10] LINE-T YPE PULSERS 379
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SEC. 10.10] LINE-TYPE PULSERS 381 T
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SEC.10.11] MISCELLANEOUS COMPONENTS
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SEC. 1011] 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
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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
Page 485 and 486: SEC. 13.3] SELECTION OF THE CATHODE
Page 487 and 488: SEC. 13.4] ANGLE-DATA TRANSMITTERS
Page 489 and 490: SEC.13.4] ANGLE-DATA TRANSMITTERS 4
Page 491 and 492: SEC. 13.5] ELECTROMECHANICAL REPEAT
Page 493 and 494: SEC. 13.6] AMPLIFIERS 493 whence th
Page 495 and 496: SEC. 13.6] AMPLIFIERS 495 by using
Page 497 and 498: SEC. 13.7] GENERA TION OF RECTANGUL
Page 499 and 500: SEC. 13.7] GENERATION OF RECTANGULA
Page 501 and 502: . SEC. 13.8] GENERA TION OF SHARP P
Page 503 and 504: SEC. 139] ELECTRONIC SWITCHES 503 T
Page 505 and 506: SEC. 13.9] ELECTRONIC SWITCHES 505
Page 507 and 508: SEC. 13.9] ELECTRO.VIC ISWI TCHES 5
Page 509 and 510: SEC. 13.9] ELECTRONIC SWITCHES 509
Page 511 and 512: SEC. 1310] SAWTOOTH GENERATORS 511
Page 513 and 514: SEC.13.10] SAWTOOTH GE,VBliATOh?S 5
Page 515 and 516: SEC. 1311] ANGLE INDICES 515 bright
Page 517 and 518: SEC. 13.11] ANGLE INDICES 517 the s
Page 519 and 520: . . “4 100k.lw $4.7k-lw .& t, T 0
Page 521 and 522: SEC.K3.121 RANGE AND HEIGIiT INDICE
Page 523 and 524: i%C.13121 RANGE AND HEIGHT INDICES;
Page 525 and 526: SEC. 13.13] DESIGN OF A-SCOPES 525
Page 527 and 528: SEC. 1313] DESIGN OF A-SCOPES 527 f
Page 529 and 530: SEC.1314] B-SCOPE DESIGN 529 \
Page 531 and 532: SEC. 13.14] B-SCOPE DESIG.V 531 wil
Page 533 and 534: Trigger I I I (CT)Sawtooth —. (A)
Page 535: SEC.1316] RESOLVED TIME BASE PPI 53
Page 539 and 540: SEC. 13.17] RESOLVED-CURRENT PPI 53
Page 541 and 542: SEC. 13.17] RESOLVED-CURRENT PPI 54
Page 543 and 544: + 200V— — — J 60k . Llk )k 60
Page 545 and 546: SEC. 13.19] 1’HE RANGB-ll EIGII1
Page 547 and 548: SEL!. 13.19] THE RANGE-HEIGHT INDIC
Page 549 and 550: SEC. 13.20] RESOLUTION AND CONTRAST
Page 551: SEC. 13.211 SPECIAL RECEIVING TECHN
Page 554 and 555: 554 THE RECEIVING SYSTEM-INDICATORS
Page 556 and 557: 556 PRIME POWER SUPPLIES FOR RADAR
Page 558 and 559: . . . 0.9 P~- 860-’CPS CF over 2
Page 562 and 563: 562 PRIME POWER SLTPPLIES FOR RADAR
Page 572: 572 PRIME POWER SUPPLIES FOR RADAR
Page 575 and 576: SEC. 14.6] SPEED REGULATORS 575 ‘
Page 577 and 578: 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
Page 585 and 586: SEC. 14.13] ULTRAPORTABLE UNITS 585
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SEC. l’k~~] SHIP RADAR SYSTEMS 58
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SEC. 151] INTRODCCTIO,\- 589 the pr
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SEC, 152] NEED FOR SYSTEM TESTING 5
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SEC, 153] INITIAL PLANNING AND OBJE
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SEC. 15.4] THE RANGE EQUATION 595 n
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SEC. 15.5] CHOICE OF PULSE LENGTH 5
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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
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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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. 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
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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
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726 RADAR RELAY [SEC. 17.15 RADAR R
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728 RADAR RELAY [SEC. 17.15 Modulat
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730 RADAR RELAY [SEC. 17.15 the sec
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732 RADAR RELAY [SEC. 17.10 pulses
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734 RADAR RELAY [f+iEc.17.16 The vi
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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
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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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