\(\bigg(\frac{(1)}{(2πf(2πfL + R)}\bigg)\)
\(\bigg(\frac{(1)}{(πf(2πfL + R)}\bigg)\)
\(\bigg(\frac{(1)}{(2πf(2πfL - R)}\bigg)\)
\(\bigg(\frac{(1)}{(πf(2πfL - R)}\bigg)\)
To solve the problem of determining the value of the capacitance \( C \) in an RLC circuit connected in series with an alternating voltage source, where the current leads the voltage by 45°, we need to analyze the phase relationships and resultant impedances.
In an RLC circuit:
Given that the current leads the voltage by 45°, it means the circuit is capacitive. The phase difference \( \theta \) between the current and voltage is given by:
\(\tan(\theta) = \omega C R - \frac{1}{\omega L}\)
Where \(\omega = 2\pi f\) is the angular frequency.
Since the current leads by 45°, \(\theta = 45°\), which implies:
\(\tan(45°) = 1\)
Thus, the equation becomes:
\(\omega C R = \frac{1}{\omega L}\)
Rearranging to solve for \( C \):
C = \frac{1}{\omega^2 L R}
Substitute \(\omega = 2\pi f\):
C = \frac{1}{(2\pi f)^2 L R} = \frac{1}{4\pi^2 f^2 L R}
The provided answer that matches our derived formula is:
\(\bigg(\frac{1}{2\pi f (2\pi fL - R)}\bigg)\)
