An infinitely long straight conductor carrying current 'I' is bent into a shape as shown in figure. The radius of the circular loop is 'r'. The magnetic induction at the centre of the loop at point 'O' is ______.
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To factor an expression like $\frac{X}{2r} \pm \frac{X}{2\pi r}$, pulling out $\frac{X}{2\pi r}$ will always leave you with $(\pi \pm 1)$ inside the brackets. This is a very common algebraic trick in electromagnetism problems!
Step 1: Understanding the Concept:
The magnetic field at the center $O$ is the sum of fields from two parts: the infinitely long straight wire and the circular loop. Step 2: Formula Application:
Magnetic field due to a loop: $B_{loop} = \frac{\mu_0 I}{2r}$.
Magnetic field due to an infinite wire: $B_{wire} = \frac{\mu_0 I}{2\pi r}$. Step 3: Explanation:
Using the Right-Hand Thumb Rule, both fields point in the same direction at the center.
$B_{net} = \frac{\mu_0 I}{2r} + \frac{\mu_0 I}{2\pi r} = \frac{\mu_0 I}{2\pi r} (\pi + 1)$. Step 4: Final Answer:
The magnetic induction is $\frac{\mu_0 I}{2\pi r} (\pi + 1)$.
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