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Example · Example 3

Q.State the expression for the magnetic field intensity on the axial line of a short bar magnet of dipole moment mm at distance dd from its centre, and briefly outline how it is obtained by treating the magnet as two point poles ±qm\pm q_m a distance 2l2l apart.

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Model the magnet as two poles +qm+q_m (N) and −qm-q_m (S), separated by 2l2l, centred at OO. At an axial point PP beyond the N pole, at distance dd from OO: the N pole (distance d−ld-l) gives field BN=(μ0/4π)qm/(d−l)2B_N=(\mu_0/4\pi)q_m/(d-l)^2 pointing away from the magnet, and the S pole (distance d+ld+l) gives BS=(μ0/4π)qm/(d+l)2B_S=(\mu_0/4\pi)q_m/(d+l)^2 pointing toward it. Both lie along the axis, and since PP is nearer NN, the resultant points away from the magnet:

Baxial=μ0qm4π[1(d−l)2−1(d+l)2]=μ04π⋅2m d(d2−l2)2B_{\text{axial}} = \frac{\mu_0q_m}{4\pi}\left[\frac{1}{(d-l)^2}-\frac{1}{(d+l)^2}\right] = \frac{\mu_0}{4\pi}\cdot\frac{2m\,d}{(d^2-l^2)^2}

For a short magnet (d≫ld\gg l), (d2−l2)2≈d4(d^2-l^2)^2\approx d^4, giving

Baxial≈μ04π⋅2md3B_{\text{axial}} \approx \frac{\mu_0}{4\pi}\cdot\frac{2m}{d^3}

✓Final answer

Baxial≈μ04π⋅2md3B_{\text{axial}} \approx \dfrac{\mu_0}{4\pi}\cdot\dfrac{2m}{d^3}, along the axis, in the direction of m⃗\vec{m}.

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