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Conquer Radio Frequency

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2.5 Reflection of DC voltage in Transmission lines 47 Figure 2.5-2 The switch is closed and the voltage wave starts propagating down the transmission line Since Z s = Z 0 , one-half of the applied voltage (E/2) will appear across the internal battery impedance, Z s , and one-half across the impedance of the line, Z 0 . This voltage "wave" applies a potential of E/2 across the first inductor-capacitor section and hence a current I flows through the inductor to charge the respective capacitor up to a voltage equal to E/2 volts. This is again shown in Figure 2.5-2. Once the first capacitor is charged, no further current will flow through it and, as the voltage wave advances, the current I will flow through second inductor to charge the second capacitor up to a E/2 volts (Figure 2.5-3). Figure 2.5-3 As the voltage wave advances, it charges up the second capacitor This process continues as the voltage wave continues to travel down the line charging each capacitor through the preceding inductor (Figure 2.5-4). Figure 2.5-4 The voltage wave continues to travel down the line E/2 E I E/2 Zero Z s E E/2 I E/2 E/2 E E/2 I E/2 E/2 E/2 Conquer Radio Frequency 47 www.cadence.com/go/awr

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