The equivalent resistance \( R_{\text{eq}} \) for resistors in parallel is calculated using the formula:
\[\frac{1}{R_{\text{eq}}} = \frac{1}{R_1} + \frac{1}{R_2} + \frac{1}{R_3}\]
Given \( R_1 = 2\, \Omega \), \( R_2 = 3\, \Omega \), and \( R_3 = 6\, \Omega \). Substitute these values:
\[\frac{1}{R_{\text{eq}}} = \frac{1}{2} + \frac{1}{3} + \frac{1}{6}\]
With a common denominator of 6:
\[\frac{1}{R_{\text{eq}}} = \frac{3}{6} + \frac{2}{6} + \frac{1}{6}\]
Summing the fractions:
\[\frac{1}{R_{\text{eq}}} = \frac{6}{6} = 1\]
Solving for \( R_{\text{eq}} \):
\[R_{\text{eq}} = 1\, \Omega\]
The equivalent resistance of this parallel combination is \( 1\, \Omega \).
An infinitely long straight wire carrying current $I$ is bent in a planar shape as shown in the diagram. The radius of the circular part is $r$. The magnetic field at the centre $O$ of the circular loop is :

The heat generated in 1 minute between points A and B in the given circuit, when a battery of 9 V with internal resistance of 1 \(\Omega\) is connected across these points is ______ J. 