To find the equivalent resistance \( R_{\text{eq}} \) of resistors connected in parallel, we use the formula:
\[\frac{1}{R_{\text{eq}}} = \frac{1}{R_1} + \frac{1}{R_2} + \frac{1}{R_3}\]
where \( R_1 = 2\, \Omega \), \( R_2 = 3\, \Omega \), and \( R_3 = 6\, \Omega \).
Substituting the given values into the formula:
\[\frac{1}{R_{\text{eq}}} = \frac{1}{2} + \frac{1}{3} + \frac{1}{6}\]
Finding a common denominator (6) for the fractions:
\[\frac{1}{2} = \frac{3}{6}, \quad \frac{1}{3} = \frac{2}{6}, \quad \frac{1}{6} = \frac{1}{6}\]
Adding the fractions:
\[\frac{1}{R_{\text{eq}}} = \frac{3}{6} + \frac{2}{6} + \frac{1}{6} = \frac{6}{6} = 1\]
Thus:
\[R_{\text{eq}} = \frac{1}{1} = 1\, \Omega\]
Therefore, the equivalent resistance of the combination is \( 1\, \Omega \).
Two cells of emf 1V and 2V and internal resistance 2 \( \Omega \) and 1 \( \Omega \), respectively, are connected in series with an external resistance of 6 \( \Omega \). The total current in the circuit is \( I_1 \). Now the same two cells in parallel configuration are connected to the same external resistance. In this case, the total current drawn is \( I_2 \). The value of \( \left( \frac{I_1}{I_2} \right) \) is \( \frac{x}{3} \). The value of x is 1cm.