KCET · Physics · Motion In Two Dimensions
The maximum height attained by a projectile when thrown at an angle \(\theta\) with the horizontal is found to be half the horizontal range. Then \(\theta\) is equal to
- A \(\tan ^{-1}\) (2)
- B \(\frac{\pi}{6}\)
- C \(\frac{\pi}{4}\)
- D \(\tan ^{-1}\left(\frac{1}{2}\right)\)
Answer & Solution
Correct Answer
(A) \(\tan ^{-1}\) (2)
Step-by-step Solution
Detailed explanation
Maximum height, \(H_{0}=\frac{u^{2} \sin _{2} \theta}{2 g}\)
Range, \(R=\frac{u^{2} \sin 2 \theta}{g}\)
Given, \(H_{0}=\frac{R}{2}\)
\(\therefore \frac{u^{2} \sin ^{2} \theta}{2 g} =\frac{u^{2} 2 \sin \theta \cos \theta}{2 g} \)
\(\Rightarrow \sin \theta =2 \cos \theta \)
\(\Rightarrow \tan \theta =2 \)
\(\therefore \theta =\tan ^{-1}(2)\)
Range, \(R=\frac{u^{2} \sin 2 \theta}{g}\)
Given, \(H_{0}=\frac{R}{2}\)
\(\therefore \frac{u^{2} \sin ^{2} \theta}{2 g} =\frac{u^{2} 2 \sin \theta \cos \theta}{2 g} \)
\(\Rightarrow \sin \theta =2 \cos \theta \)
\(\Rightarrow \tan \theta =2 \)
\(\therefore \theta =\tan ^{-1}(2)\)
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