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Conquer Radio Frequency

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CHAPTER 2 - Conveying Power at Radio Frequency 70 2.7 Standing waves and resonance Whenever there is a mismatch of impedance between transmission line and load, reflections will occur. If the incident signal is a continuous AC waveform, these reflections will mix with more of the oncoming incident waveform to produce stationary waveforms called standing waves. Figure 2.7-1 shows how a triangle-shaped incident waveform turns into a mirror-image reflection upon reaching the line's unterminated end. The transmission line in this illustrative sequence is shown as a single, dotted line rather than a pair of wires, for simplicity. The incident wave is shown travelling from left to right, while the reflected wave travels from right to left. After the incident signal hits the end of the line, the overall voltage observed on the line will be the sum of incident and reflected voltages. Figure 2.7-1 shows the step by step transients of the total voltage along the line up until the reflected voltage reaches the source end. After this transient time, what we observe on the line is the standing wave shown in Figure 2.7-2. This is representative of the steady-state voltage along the line, i.e. the sum of incident and reflected voltage waves. This standing wave oscillates in instantaneous magnitude, but does not propagate down the cable's length like the incident or reflected waveforms causing it. Note that the "zero" points of the standing wave, where the incident and reflected waves cancel each other, never change position (Figure 2.7-2). In the next section we will examine these phenomena in more detail for a range of terminations. Conquer Radio Frequency 70 www.cadence.com/go/awr

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