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Stated another way, it is the ratIO of the voltage in the forward- traveling voltage wave to the current in the forward traveling current wave. Although the characteristic impedance of a waveguide has the dimensions and some of the properties of an impedance, it is important to note that these properties are not physically equivalent to the impedance properties of a single-port circuit. For example, although it has a real and an imaginary part, its real part, per se, does not dissipate energy nor does its imaginary part store energy.

5 SURGE IMPEDANCE The input impedance that the forward traveling electromagnetic wave encounters as it propagates along a uniform waveguide is called the surge impedance or the initial sending-end impedance. In the case of a uniform waveguide it is called, specifically, the characteristic impedance. The input impedance has, initially, a constant value independent of position along the waveguide. Its magnitude is independent of the magnitude or of the phase angle of the load reflection coefficient, it being assumed 11 that in this briefinterval the forward-traveling electromagnetic wave has not yet arrived at the load terminals.

Measure with horizontal axis scale, and tabulate voltage vector lengths o-a), O-@, O-@, etc. to o-@. (a) What is the magnitude and angle of the voltage reflection coefficient at the minimum point (CD) of the voltage standing wave? 5L180 (b) What is the magnitude and angle of the current reflection coefficient at the same point (maximum point (®) of the current standing wave)? 6 ETC. 66 0 - ® I. 06 o - @ I. 40 o - @ I. 50 - ® I. 40 o - (i) I. 66 0 o o 1/16 2/16 3/16 4/16 5/16 6/16 WAVELENGTHS FROM E min TOWARD LOAD Fig.

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