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in Physics by (51.8k points)
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Let δ1 and δ2 be the angle fo dip in any two vertical planes (other than the magnetic meridian) that are at right angles to each other. If, δ is the true value of the angle of dip, we would have

(1) tan2 δ1 + tan2 δ= tan2δ

(2) \(\frac{tan^2δ_1}{tan^2δ_2}=cot^2δ\)

(3) cot2 δ1 + cot2 δ2 = 1

(4) cot2 δ = cot2 δ1 + cot2 δ2

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(4) cot2 δ = cot2 δ1 + cot2 δ2

Let the vertical plane, in which angle of dip is δ1 subtends an angle θ with the magnetic meridian. Their other plane then subteneds an angle (π/2 - θ) with the magnetic meridian.

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