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The propagation constant of a transmission line is 0.15├Ч10тАУ┬│ + j1.5├Ч10тАУ┬│. The wavelength of the traveling wave is
2╧А15├Ч10тИТ3тАЛ
1.5├Ч10тИТ32╧АтАЛ
╧А15├Ч10тИТ3тАЛ
15├Ч10тИТ3╧АтАЛ
1.5├Ч10тИТ32╧АтАЛ
The propagation constant of a transmission line is defined as ╬│=╬▒+j╬▓, where ╬▒ is the attenuation constant and ╬▓ is the phase constant. The wavelength ╬╗ of the traveling wave is related to the phase constant ╬▓ by the expression ╬╗=╬▓2╧АтАЛ.
The propagation constant of a transmission line is defined as ╬│=╬▒+j╬▓, where ╬▒ is the attenuation constant and ╬▓ is the phase constant. The wavelength ╬╗ of the traveling wave is related to the phase constant ╬▓ by the expression ╬╗=╬▓2╧АтАЛ.
╬│=╬▒+j╬▓ тАФ Propagation constant definition
╬╗=╬▓2╧АтАЛ тАФ Relationship between wavelength and phase constant
As an electromagnetic wave propagates down a transmission line, it undergoes a phase shift determined by the phase constant ╬▓. The distance required for the wave to complete one full cycle (a phase shift of 2╧А radians) is defined as the wavelength ╬╗. Since ╬▓ represents the phase shift per unit length (radians/meter), ╬╗ is simply the inverse proportion of ╬▓.
The propagation constant is a complex quantity where the imaginary part ╬▓ dictates the wave's phase velocity.
The units of ╬▓ are radians per meter (rad/m) and ╬▒ are nepers per meter (Np/m).
Wavelength is inversely proportional to the phase constant: higher frequency signals generally correspond to higher ╬▓ values and shorter wavelengths.
Provides a simple mathematical relation for wave analysis
Essential for calculating line impedance matching
Assumes a linear, time-invariant transmission line
Does not account for non-uniform line geometry
Designing impedance matching networks
Determining signal propagation delays in power and communication lines
Given ╬│=0.15├Ч10тИТ3+j(1.5├Ч10тИТ3), the imaginary part ╬▓=1.5├Ч10тИТ3.
Substituting ╬▓ into the formula ╬╗=╬▓2╧АтАЛ yields 1.5├Ч10тИТ32╧АтАЛ.
B is correct тАФ The wavelength is defined by ╬╗=╬▓2╧АтАЛ, where ╬▓ is the imaginary part of the propagation constant.
Always ensure you extract the imaginary part (╬▓) for phase calculations, as the real part (╬▒) only affects signal amplitude/attenuation.