Step 1: State the formula for the input impedance of a transmission line.\[ Z_{in} = Z_0 \frac{Z_L + jZ_0 \tan(\beta l)}{Z_0 + jZ_L \tan(\beta l)} \]
Step 2: Calculate \(\tan(\beta l)\).Given a line length of \(l = \lambda/8\) and a phase constant of \(\beta = 2\pi/\lambda\):\[ \beta l = \frac{2\pi}{\lambda} \cdot \frac{\lambda}{8} = \frac{\pi}{4} \]\[ \tan(\beta l) = \tan(\pi/4) = 1 \]
Step 3: Substitute the given values into the input impedance formula.With \(Z_0 = 50\Omega\) and \(Z_L = R + j30\):\[ Z_{in} = 50 \frac{(R + j30) + j50(1)}{50 + j(R + j30)(1)} = 50 \frac{R + j80}{50 + jR - 30} = 50 \frac{R + j80}{20 + jR} \]
Step 4: Determine the value of \(R\) that makes \(Z_{in}\) real.To eliminate the imaginary component of \(Z_{in}\), multiply the numerator and denominator by the complex conjugate of the denominator:\[ Z_{in} = 50 \frac{(R + j80)(20 - jR)}{(20 + jR)(20 - jR)} = 50 \frac{(20R + 80R) + j(1600 - R^2)}{400 + R^2} \]For the input impedance to be real, the imaginary part must be zero.\[ 1600 - R^2 = 0 \]\[ R^2 = 1600 \implies R = 40 \, \Omega \]