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A ring of radius R carries a linear charge density $$\lambda$$ . It is rotating with angular speed $$\omega$$ . The magnetic field at its center is
$$ \frac{3 \mu_{0} \lambda \omega}{2}$$
$$\frac{\mu_{0} \lambda \omega}{2}$$
$$\frac{\mu_{0} \lambda \omega}{\pi}$$
$$\mu_{0} \lambda \omega$$
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