| Preface |
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xiii | |
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Signal Integrity Is in Your Future |
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1 | (40) |
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What Is Signal Integrity? |
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2 | (3) |
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Signal Quality on a Single Net |
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5 | (3) |
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8 | (2) |
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10 | (3) |
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Electromagnetic Interference (EMI) |
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13 | (2) |
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Two Important Signal Integrity Generalizations |
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15 | (1) |
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Trends in Electronic Products |
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16 | (5) |
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The Need for a New Design Methodology |
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21 | (1) |
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A New Product Design Methodology |
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22 | (1) |
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23 | (4) |
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27 | (2) |
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Creating Circuit Models from Calculation |
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29 | (5) |
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Three Types of Measurements |
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34 | (3) |
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37 | (2) |
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39 | (2) |
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Time and Frequency Domains |
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41 | (38) |
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42 | (2) |
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Sine Waves in the Frequency Domain |
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44 | (2) |
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Shorter Time to a Solution in the Frequency Domain |
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46 | (1) |
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47 | (2) |
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49 | (2) |
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The Spectrum of a Repetitive Signal |
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51 | (2) |
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The Spectrum of an Ideal Square Wave |
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53 | (2) |
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From the Frequency Domain to the Time Domain |
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55 | (1) |
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Effect of Bandwidth on Rise Time |
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56 | (3) |
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59 | (2) |
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What Does ``Significant'' Mean? |
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61 | (3) |
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Bandwidth of Real Signals |
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64 | (2) |
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Bandwidth and Clock Frequency |
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66 | (2) |
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Bandwidth of a Measurement |
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68 | (2) |
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70 | (1) |
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Bandwidth of an Interconnect |
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71 | (5) |
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76 | (3) |
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Impedance and Electrical Models |
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79 | (30) |
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Describing Signal-Integrity Solutions in Terms of Impedance |
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80 | (2) |
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82 | (2) |
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Real vs. Ideal Circuit Elements |
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84 | (2) |
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Impedance of an Ideal Resistor in the Time Domain |
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86 | (1) |
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Impedance of an Ideal Capacitor in the Time Domain |
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87 | (3) |
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Impedance of an Ideal Inductor in the Time Domain |
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90 | (2) |
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Impedance in the Frequency Domain |
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92 | (5) |
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Equivalent Electrical Circuit Models |
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97 | (2) |
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99 | (4) |
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103 | (5) |
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108 | (1) |
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The Physical Basis of Resistance |
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109 | (14) |
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Translating Physical Design into Electrical Performance |
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110 | (1) |
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The Only Good Approximation for the Resistance of Interconnects |
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111 | (3) |
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114 | (1) |
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115 | (2) |
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117 | (4) |
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121 | (2) |
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The Physical Basis of Capacitance |
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123 | (24) |
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Current Flow in Capacitors |
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124 | (2) |
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The Capacitance of a Sphere |
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126 | (1) |
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Parallel Plate Approximation |
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127 | (2) |
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129 | (1) |
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Power and Ground Planes and Decoupling Capacitance |
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130 | (4) |
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134 | (5) |
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139 | (3) |
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Effective Dielectric Constant |
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142 | (4) |
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146 | (1) |
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The Physical Basis of Inductance |
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147 | (58) |
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147 | (1) |
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Inductance Principle #1: There Are Circular Magnetic-Field Line Loops Around All Currents |
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148 | (2) |
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Inductance Principle #2: Inductance Is the Number of Webers of Field Line Loops Around a Conductor per Amp of Current Through It |
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150 | (2) |
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Self-Inductance and Mutual Inductance |
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152 | (2) |
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Inductance Principle #3: When the Number of Field Line Loops Around a Conductor Changes, There Will Be a Voltage Induced Across the Ends of the Conductor |
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154 | (3) |
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157 | (6) |
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Effective, Total, or Net Inductance and Ground Bounce |
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163 | (6) |
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Loop Self- and Mutual Inductance |
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169 | (5) |
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The Power-Distribution System (PDS) and Loop Inductance |
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174 | (5) |
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Loop Inductance per Square of Planes |
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179 | (2) |
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Loop Inductance of Planes and Via Contacts |
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181 | (2) |
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Loop Inductance of Planes with a Field of Clearance Holes |
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183 | (2) |
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185 | (1) |
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185 | (2) |
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187 | (2) |
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Current Distributions and Skin Depth |
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189 | (9) |
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High-Permeability Materials |
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198 | (2) |
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200 | (2) |
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202 | (3) |
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The Physical Basis of Transmission Lines |
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205 | (72) |
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206 | (1) |
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207 | (1) |
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Uniform Transmission Lines |
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208 | (2) |
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The Speed of Electrons in Copper |
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210 | (1) |
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The Speed of a Signal in a Transmission Line |
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211 | (4) |
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Spatial Extent of the Leading Edge |
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215 | (1) |
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216 | (4) |
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The Instantaneous Impedance of a Transmission Line |
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220 | (3) |
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Characteristic Impedance and Controlled Impedance |
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223 | (2) |
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Famous Characteristic Impedances |
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225 | (3) |
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The Impedance of a Transmission Line |
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228 | (5) |
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Driving a Transmission Line |
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233 | (3) |
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236 | (4) |
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When Return Paths Switch Reference Planes |
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240 | (12) |
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A First-Order Model of a Transmission Line |
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252 | (5) |
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Calculating Characteristic Impedance with Approximations |
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257 | (4) |
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Calculating the Characteristic Impedance with a 2D Field Solver |
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261 | (5) |
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An n-Section Lumped Circuit Model |
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266 | (7) |
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Frequency Variation of the Characteristic Impedance |
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273 | (2) |
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275 | (2) |
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Transmission Lines and Reflections |
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277 | (56) |
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Reflections at Impedance Changes |
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278 | (2) |
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Why Are There Reflections? |
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280 | (3) |
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Reflections from Resistive Loads |
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283 | (3) |
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286 | (2) |
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288 | (1) |
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Simulating Reflected Waveforms |
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289 | (3) |
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Measuring Reflections with a TDR |
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292 | (3) |
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Transmission Lines and Unintentional Discontinuities |
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295 | (2) |
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297 | (3) |
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The Most Common Termination Strategy for Point-to-Point Topology |
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300 | (2) |
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Reflections from Short Series Transmission Lines |
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302 | (3) |
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Reflections from Short-Stub Transmission Lines |
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305 | (2) |
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Reflections from Capacitive End Terminations |
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307 | (3) |
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Reflections from Capacitive Loads in the Middle of a Trace |
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310 | (3) |
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313 | (2) |
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Effects of Corners and Vias |
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315 | (5) |
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320 | (3) |
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Reflections from Inductive Discontinuities |
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323 | (5) |
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328 | (2) |
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330 | (3) |
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Lossy Lines, Rise-Time Degradation, and Material Properties |
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333 | (68) |
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Why Worry About Lossy Lines |
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334 | (2) |
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Losses in Transmission Lines |
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336 | (2) |
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Sources of Loss: Conductor Resistance and Skin Depth |
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338 | (4) |
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Sources of Loss: The Dielectric |
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342 | (5) |
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347 | (3) |
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The Real Meaning of Dissipation Factor |
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350 | (5) |
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Modeling Lossy Transmission Lines |
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355 | (8) |
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Characteristic Impedance of a Lossy Transmission Line |
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363 | (2) |
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Signal Velocity in a Lossy Transmission Line |
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365 | (2) |
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367 | (5) |
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Attenuation in Lossy Lines |
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372 | (9) |
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Measured Properties of a Lossy Line in the Frequency Domain |
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381 | (5) |
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The Bandwidth of an Interconnect |
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386 | (6) |
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Time-Domain Behavior of Lossy Lines |
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392 | (4) |
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Improving the Eye Diagram of a Transmission Line |
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396 | (2) |
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Pre-emphasis and Equalization |
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398 | (1) |
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399 | (2) |
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Cross Talk in Transmission Lines |
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401 | (70) |
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402 | (1) |
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Origin of Coupling: Capacitance and Inductance |
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403 | (2) |
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Cross Talk in Transmission Lines: NEXT and FEXT |
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405 | (2) |
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407 | (2) |
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The SPICE Capacitance Matrix |
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409 | (4) |
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The Maxwell Capacitance Matrix and 2D Field Solvers |
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413 | (6) |
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419 | (2) |
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Cross Talk in Uniform Transmission Lines and Saturation Length |
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421 | (5) |
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Capacitively Coupled Currents |
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426 | (4) |
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Inductively Coupled Currents |
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430 | (3) |
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433 | (3) |
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436 | (7) |
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Decreasing Far-End Cross Talk |
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443 | (2) |
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445 | (7) |
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452 | (7) |
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Cross Talk and Dielectric Constant |
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459 | (1) |
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460 | (4) |
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464 | (4) |
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Summary of Reducing Cross Talk |
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468 | (1) |
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468 | (3) |
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Differential Pairs and Differential Impedance |
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471 | (80) |
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472 | (4) |
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476 | (2) |
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Differential Impedance with No Coupling |
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478 | (4) |
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482 | (6) |
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Calculating Differential Impedance |
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488 | (4) |
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The Return-Current Distribution in a Differential Pair |
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492 | (6) |
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498 | (5) |
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Differential Impedance and Odd-Mode Impedance |
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503 | (1) |
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Common Impedance and Even-Mode Impedance |
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504 | (3) |
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Differential and Common Signals and Odd- and Even-Mode Voltage Components |
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507 | (2) |
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Velocity of Each Mode and Far-End Cross Talk |
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509 | (6) |
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Ideal Coupled Transmission-Line Model or an Ideal Differential Pair |
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515 | (1) |
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Measuring Even- and Odd-Mode Impedance |
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516 | (2) |
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Terminating Differential and Common Signals |
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518 | (7) |
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Conversion of Differential to Common Signals |
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525 | (5) |
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530 | (5) |
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Cross Talk in Differential Pairs |
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535 | (2) |
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Crossing a Gap in the Return Path |
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537 | (3) |
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To Tightly Couple or Not to Tightly Couple |
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540 | (2) |
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Calculating Odd and Even Modes from Capacitance- and Inductance-Matrix Elements |
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542 | (4) |
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The Characteristic Impedance Matrix |
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546 | (3) |
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549 | (2) |
| Appendix A |
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551 | (8) |
| Appendix B |
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559 | (12) |
| Appendix C |
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571 | (2) |
| Index |
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573 | (14) |
| About the Author |
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587 | |