\(\frac{1}{2}\)
To solve the problem, we need to equate the range and the maximum height of the projectile. We start by understanding the formulas used for range and maximum height when a ball is projected with an initial velocity \(u\) at an angle \(\theta\) from the horizontal:
Given that the range and maximum height are equal, we have:
\(\frac{u^2 \sin(2\theta)}{g} = \frac{u^2 \sin^2(\theta)}{2g}\)
By cancelling common terms and simplifying, we get:
\(2 \sin(2\theta) = \sin^2(\theta)\)
Using the trigonometric identity \(\sin(2\theta) = 2\sin(\theta)\cos(\theta)\), we substitute:
\(4 \sin(\theta)\cos(\theta) = \sin^2(\theta)\)
Divide both sides by \(\sin(\theta)\) (assuming \(\sin(\theta)\) is not zero):
\(4 \cos(\theta) = \sin(\theta)\)
This simplifies to:
\(\tan(\theta) = 4\)
Therefore, the value of \(\tan(\theta)\) is 4. Thus, the correct answer is the option
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