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Exercise 3.10 · Q16

Q.Suppose that a satellite in space, an earth station and the centre of the earth all lie in the same plane. Let rr be the radius of the earth and RR be the distance from the centre of the earth to the satellite. Let dd be the distance from the earth station to the satellite. Let 30∘30^\circ be the angle of elevation from the earth station to the satellite. If the line segment connecting the earth station and the satellite subtends angle α\alpha at the centre of the earth, then prove that d=R1+(rR)2−2rRcos⁡αd = R\sqrt{1+\left(\dfrac{r}{R}\right)^2 - 2\dfrac{r}{R}\cos\alpha}.

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The centre of the earth OO, the earth station EE, and the satellite SS form a triangle with OE=rOE=r, OS=ROS=R, and included angle ∠EOS=α\angle EOS=\alpha at the centre. Applying the cosine rule for the side ES=dES=d and then factoring R2R^2 out of the square root gives exactly the stated formula.

Step 1. Set up the triangle. Let OO be the centre of the earth, EE the earth station on the earth's surface (so OE=rOE=r, the earth's radius), and SS the satellite (so OS=ROS=R, the distance from the earth's centre to the satellite). The angle subtended at the centre by the segment joining EE and SS is ∠EOS=α\angle EOS = \alpha. The required distance is d=ESd = ES.

Step 2. Apply the cosine rule in △OES\triangle OES, for the side opposite the known angle α\alpha.

d2=OE2+OS2−2(OE)(OS)cos⁡α=r2+R2−2rRcos⁡α.d^2 = OE^2+OS^2-2(OE)(OS)\cos\alpha = r^2+R^2-2rR\cos\alpha.

Step 3. Factor R2R^2 out from inside the square root.

d=r2+R2−2rRcos⁡α=R2[(rR)2+1−2(rR)cos⁡α].d = \sqrt{r^2+R^2-2rR\cos\alpha} = \sqrt{R^2\left[\left(\frac{r}{R}\right)^2+1-2\left(\frac{r}{R}\right)\cos\alpha\right]}.

Step 4. Pull RR (positive, since it is a distance) outside the square root. …

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