Transmission Line Properties The physical characteristics geometry and

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Transmission Line Properties The physical characteristics, geometry, and materials determine the electrical properties of

Transmission Line Properties The physical characteristics, geometry, and materials determine the electrical properties of a transmission line. The primary properties are Capacitance, Conductance, Resistance, and Inductance per unit length: C 0 (f/m), G 0 (s/m), R 0 (W/m), and L 0 (h/m) respectively. For well designed transmission lines, R 0 and G 0 are very small and can be neglected in a first order analysis (lossless case). When a differential length (dx) of lossless transmission line is analyzed using Kirchhoff's Laws, the resulting differential equations yield a solution for the complex voltage function having the following form. . .

The coefficient A is a complex constant representing a voltage amplitude, including a possible

The coefficient A is a complex constant representing a voltage amplitude, including a possible phase shift determined by the boundary (termination) conditions. The + wt parameter in the exponential indicates that when the line is driven by a source having radian frequency w, there will exist complex conjugate solutions assuring a real valued sinusoidal voltage function. For simplicity, we will only consider the positive frequency solution. The + bx parameter in the exponential indicates that there will exist solutions representing traveling waves moving in both the positive and negative x directions, supporting our previous deduction. We will use the following forms for the forward and reflected line voltages:

Transmission Line Properties (cont) In addition to the form of the voltage waveform, the

Transmission Line Properties (cont) In addition to the form of the voltage waveform, the analysis also yields the following fundamental transmission line properties: Characteristic Impedance: Phase Velocity: For many simple geometries, the expression for phase velocity reduces to:

Phase Velocity and Wavelength Consider the expression derived for the forward voltage: The term

Phase Velocity and Wavelength Consider the expression derived for the forward voltage: The term in the parentheses represents the instantaneous phase of the traveling wave. We can examine the motion of a point of fixed phase (e. g. , a peak, valley, or zero crossing) by setting the phase term equal to a constant, and solving for x: The term in parentheses represents the speed at which the point of constant phase is moving in the positive x direction, thus:

Phase Velocity and Wavelength (cont) The point of constant phase, moving at velocity vp,

Phase Velocity and Wavelength (cont) The point of constant phase, moving at velocity vp, will move one wavelength, l , in one period of the source frequency: Or, alternatively, b is referred to as the “wave number” and has units of radians/meter.