The bounce diagram and the voltages 9L1 and 9L2 are sketched as shown. b Since the load end of one of the Ω interconnects point A is now an open circuit i. Bounce diagram and 9L1 , and 9L2 versus t. This process continues on. The bounce diagram and the variation of the voltages 9L1 and 9L2 are as shown. This process continues on until the 2 reflections die out. The variation of the voltages 91 , 92 and 93 are shown in Figure 2. The voltages 91 , 92 and 93 are sketched up to 5 ns as shown in Figure 2. Again, at steady-state, all the voltages reach 1. Bounce diagram and 91 , and 92 versus t.

Thus, the parasitic effects cause extra time delay before the voltages reach their steady-state values. The bounce diagram and the voltages 9s and 9L for this case are shown in Figure 2. As a result, no reflections from the source end occurs for the time interval 5. a Bounce diagram b 9s , 9J , and 9L versus t. b In this case,. Using a similar approach, we can generate the bounce diagram and the voltage plots shown in Figure 2. reflects back toward the source and a voltage wave of amplitude 0. The bounce diagram and the variation of the load voltage 9L t are as shown in Figure 2. Bounce diagram and 9L versus t. on the interconnect traveling toward the driver gate. As seen from the bounce diagram and the sketch of the load-end voltage 9L versus t, the load gate turns on permanently i. However, the steady-state voltages are different from one another. In the parallel termination network however, a steady-state current flows through the circuit at HIGH state given by. In the parallel termination network, no reflections occur.

Therefore, the parallel termination network provides a faster overall speed because all of the three load gates reach steady state earlier. The two voltage waves transmitted on lines 2 and 3 each with 2. Using the above values, the bounce diagram and the variation of the voltage 91 and 92 versus t are as shown in Figure 2. Bounce diagram,91 versus t and 92 versus t. a Let the two interconnects connected to each driver gate be driver interconnects D1 and D2 and the third one connected to the load gate be the load interconnect. The bounce diagram and the sketch of the load-end voltage 9L versus t are as shown in Figure 2. is launched at the driver end of the driver interconnect D1. At the same time, when driver gate 2 switches to HIGH state, a voltage wave of amplitude V0 2 is launched at the driver end of the driver interconnect D2. Therefore, in this case, as shown in Figure 2.

The transmitted voltage wave reaches the 5 pF capacitor at. a Bounce diagram and 9L versus t. b 9L versus t. Initially the capacitor is uncharged and appears like a short circuit, i. The sketch of 91 t versus t is as shown in Figure 2. Reading from the TDR waveform, the amplitude of the initial voltage wave launched on the Z01 transmission line is. b Based on the TDR waveform, we can identify the unknown elements, as shown in Figure 2. From Figure 2. Therefore, there are no reflections from the source end. Based on Figure 2. Let these two elements be represented as L and R. is transmitted to line 2 heading toward the capacitive load. Note that this expression represents the reflected voltage wave at the load position. The plot of 9L versus t is shown in Figure 2. The plot 9s versus t is also shown in Figure 2. Considering the above results, we can make the sketches seen in Figure 2.

a 9s t versus t. b 9L t versus t. Following steps similar to Example 2. where the K1 and K2 constants are to be determined using the initial and final conditions. Note that the reflected voltage wave at the load end must vary exponentially from 2. The source- and load-end voltage waveforms are shown in Figure 2. Equivalent circuit at the load end of the transmission line at steady state. We begin by calculating the reflection coefficient ΓJ at the junction. The total reflection coefficient at the junction for a voltage wave approaching from the 50Ω line is therefore is launched down the 50Ω transmission line.

Initially, the capacitor is discharged and represents a short circuit. Noting the series 25Ω load resistor, the capacitive load is initially matched and the initial reflection coefficient is 0. At this time, the reflection coefficient at the capacitive load is 1. Noting that the two Ω lines have matched terminations, and the parallel network seen by the 25Ω line is also matched, the bounce diagram in Figure 2. Page 22 Page 23 Page 24 Page 25 Page 26 Page 27 Page 28 Page 29 Page 30 Page 31 Page 32 Page 33 Page 34 Page 35 Page 36 Page 37 Page 38 Page 39 Page 40 Page 41 Page 42 Page 43 Page 44 Page 45 Page 46 Page 47 Page 48 Page 49 Page 50 Page 51 Page 52 Page 53 Page 54 Page 55 Page 56 Page 57 Page 58 Page 59 Page 60 Page 61 Page 62 Page 63 Page 64 Page 65 Page 66 Page 67 Page 68 Page 69 Page 70 Page 71 Page 72 Page 73 Page 74 Page 75 Page 76 Page 77 Page 78 Page 79 Page 80 Page 81 Page 82 Page 83

You will find Field and Wave Electromagnetics, 2nd Edition PDF which can be downloaded for FREE on this page. Field and Wave Electromagnetics, 2nd Edition is useful when preparing for COE course exams. Field and Wave Electromagnetics, 2nd Edition written by David cheng was published in the year and uploaded for level Engineering students of Federal University of Technology, Owerri FUTO offering COE course. Field and Wave Electromagnetics, 2nd Edition can be used to learn Electromagnetic Model, Vector analysis, Static electric field, Electrostatics, steady electric current, static magnetic fields, Varying Fields, Maxwell's Equations, Plane Electromagnetic Waves, Theory and Applications of Transmission Lines, Waveguides, Cavity resonators, Antennas, Radiating system.

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