(Solved): Using a Function Generator, Agilent DMM, 100mH inductor, 47nF ceramic capacitor, \( 1 \mathrm{k} ...

Using a Function Generator, Agilent DMM, 100mH inductor, 47nF ceramic capacitor, \( 1 \mathrm{k} \) and \( 10 \mathrm{Ohm} \) resistors, draw this configuration in the space below: - \( 2 \mathrm{~V}_{\mathrm{RMS}} \) source voltage from function generator - \( 100 \mathrm{mH} \) inductor, \( 47 \mathrm{nF} \) capacitor and a \( 1 \mathrm{k} \) resistor form a RLC Series circuit - The DMM is used to measure \( V_{R} \) and indicate when the frequency on the function generator is the resonant frequency of the circuit - The \( 10 \mathrm{Ohm} \) resistor will be used as a source resistor to show the phase angle of \( I_{T} \) when the circuit is at resonance. - This will be known as Figure 1 Procedure A: Using Multisim, connect the circuit in Figure 1. Adjust the frequency on the function generator until the circuit is at resonance. Record your DMM measurements in Table \( 1 . \) - . Procedure B: Move the frequency \( 200 \mathrm{~Hz} \) above and below your measured value of \( f_{R} \). What happens to \( V_{R} \) and the phase angle of \( I_{T} \) when you move the frequency above and below the measured value of \( f_{R} \) ? Why does this happen?