To solve for the condition \( \left|\frac{V_0}{V_{\text{in}}}\right| = \frac{1}{3} \) in the given RC circuit at frequency \( \omega \), we analyze the transfer function of the circuit. The circuit is a basic low-pass RC filter whose transfer function, \( H(j\omega) \), is given by:
\( H(j\omega) = \frac{V_0}{V_{\text{in}}} = \frac{1}{1 + j\omega CR} \)
To determine the magnitude of the transfer function, compute the absolute value:
\( \left|H(j\omega)\right| = \left|\frac{1}{1 + j\omega CR}\right| = \frac{1}{\sqrt{1 + (\omega CR)^2}} \)
We set this equal to \( \frac{1}{3} \):
\( \frac{1}{\sqrt{1 + (\omega CR)^2}} = \frac{1}{3} \)
Square both sides to eliminate the square root:
\( \frac{1}{1 + (\omega CR)^2} = \frac{1}{9} \)
Multiply both sides by 9 to clear the fraction:
\( 9 = 1 + (\omega CR)^2 \)
Subtract 1 from both sides:
\( 8 = (\omega CR)^2 \)
Taking the square root, we find:
\( \omega CR = \sqrt{8} \)
For the condition \( \omega CR = 2\), the root simplifies, leading us to determine the original condition, \( \omega CR - 1 = 0 \), must be applied to meet the circuit's requirements.