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A far off planet is estimated to be at a...

A far off planet is estimated to be at a distance D from the earth. If its diametrically opposite extremes subtend an angle `theta` at an observatory situated on the earth, the approximate diameter of the planet is

A

`theta/D`

B

`D/theta`

C

`D theta`

D

`1/(D theta)`

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The correct Answer is:
To solve the problem of finding the approximate diameter of a far-off planet that subtends an angle \( \theta \) at an observatory on Earth, we can follow these steps: ### Step 1: Understand the Geometry We have an observatory on Earth and a planet at a distance \( D \). The planet's diametrically opposite extremes subtend an angle \( \theta \) at the observatory. We can visualize this scenario as a triangle formed by the observatory and the two extremes of the planet. ### Step 2: Define the Variables Let: - \( D \) = distance from the observatory to the planet - \( d \) = diameter of the planet - The angle subtended at the observatory is \( \theta \). ### Step 3: Consider Half of the Angle Since the diameter subtends the angle \( \theta \), each half of the diameter subtends an angle of \( \frac{\theta}{2} \). ### Step 4: Use Trigonometric Relationships In the triangle formed (let's label the observatory point as \( O \), one extreme of the planet as \( A \), and the other extreme as \( C \)), we can use the tangent function: \[ \tan\left(\frac{\theta}{2}\right) = \frac{\text{opposite}}{\text{adjacent}} = \frac{\frac{d}{2}}{D} \] Where \( \frac{d}{2} \) is the opposite side (half the diameter of the planet) and \( D \) is the adjacent side (distance from the observatory to the planet). ### Step 5: Approximate for Small Angles For small angles (which is the case here), we can use the approximation: \[ \tan\left(\frac{\theta}{2}\right) \approx \frac{\theta}{2} \] Thus, we can rewrite the equation as: \[ \frac{\theta}{2} = \frac{\frac{d}{2}}{D} \] ### Step 6: Solve for the Diameter \( d \) Rearranging the equation gives: \[ \frac{d}{2} = D \cdot \frac{\theta}{2} \] Multiplying both sides by 2: \[ d = D \cdot \theta \] ### Conclusion The approximate diameter of the planet is: \[ d \approx D \cdot \theta \] ### Final Answer Thus, the approximate diameter of the planet is \( d = D \cdot \theta \). ---
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