An a.c. source of angular frequency \( \omega \) is connected across a resistor \( R \) and a capacitor \( C \) in series. The current is observed as \( I \). Now the frequency of the source is changed to \( \omega/4 \) (keeping the voltage unchanged) the current is found to be \( I/3 \). The ratio of resistance to reactance at frequency \( \omega \) is