TABLES THE DEVICES ‘igi @ 1.1 1.2 Approximate Component Weights, Approximate Component Weights, ek ww wee « 1-26 1-29 1.4 Approximate Component Weights, ee ew 1-35 1.3 1.5 1.6 1.7 .1.8 1.9 Approximate Component Weights, ~ Approximate Component Weights, . Approximate Component Weighta, | gi a Approximate Componsnt Weights, Approximate Component Weights, Approximate Component Weights, 1.13 Integral of pdR -Integral of pdR -- Integral of pdR -, we ee 1.16 Integral of pdR - 7a Sue 1-38 {3 1HAL .. 1-39 es LH wee ee we wee ee we ww LAS big ee we we ew ew we LHD 1-50 te ee ew ee ee «1-52 eee ew Integral of pdR -j ew ew ee ft LAT 1AK8 beg ee ee ee 61K Be i” ee 3h - og r *s ure THE MZASUREMENTS 2.1 2.2 2.3 2.4 Expected Gamma-ray Levela ... , ee eee we Cross Sections for Tuballoy (T™-M7). we ew ee Predicted Lighting Times of Neutron Mean Freg Paths tion Times coud on 2-67 ees Pg os £ 2-80 \. . 2.5 2.6 (Qe hot Spots... . Interface Radii, Materi 233 HKG , Transmissio® and Thermal Flux Received as Function of Field of View for Conditions Similar to Those Existing on Mike Shot... .....2.56266046-4- ro? 2-106 ig [33 te bug 2-119 SSAPIER 3 MISCELLANEOUS DATA 3.4 .......226 00.2. ... eee we ee Ivy Neutron Intersitiea es Seen by Various. Threshold Detectors ... we ee ee we Predicted Neutron Intensities as Seen by Various Threshold Detectors .......2-2-e-+- + i+ 3-le 7 bos JT 5HK8 ae 6 se i: .§ eit Bek J790 y 3.5 J-1l Threshold Detectora J-12 Thresnold Detectors ......... 3 iy P 3,2 3.3 Ivy Mike Peak Fall-out Intensity RT gs MARTY vl FS gana 3.1 jis? mrkyLetAIR aN CHAPTER 2 . | 1.15 es ee ee L-32 7 ST ke 1S DELETED 1.14 Integral of pdR - .. . we ew 1.10 Integral of pdR - 1.11 1.12 “a «© « ice [oh Sen ; CHAPTER 1 «410 a top. y sod Sea, gut Poy wren x wet Coplegoe LAN

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