The problem requires solving the trigonometric equation \(4\cos\theta + 5\sin\theta = 1\) for \(\alpha\) within the range \(-\frac{\pi}{2} < \alpha < \frac{\pi}{2}\), and determining the value of \(\tan\alpha\).
The equation \(4\cos\theta + 5\sin\theta = 1\) can be rewritten in the form \(R\cos(\theta - \phi)\), where \(R\) is the amplitude and \(\phi\) is the phase shift.
Calculate \(R\):
\(R = \sqrt{4^2 + 5^2} = \sqrt{16 + 25} = \sqrt{41}\)
Express \(\cos\theta\) and \(\sin\theta\) in terms of \(R\):
\(R\cos(\theta - \phi) = 4\cos\theta + 5\sin\theta\)
By comparing coefficients:
\(R\cos\phi = 4\) and \(R\sin\phi = 5\)
Calculate \(\tan\phi\):
\(\tan\phi = \frac{R\sin\phi}{R\cos\phi} = \frac{5}{4}\)
The equation simplifies to:
\(\sqrt{41}\cos(\theta - \phi) = 1\)
This yields:
\(\cos(\theta - \phi) = \frac{1}{\sqrt{41}}\)
Let \(\alpha = \theta - \phi\). Then:
Using the identity \(\tan\alpha = \frac{\sin\alpha}{\cos\alpha}\):
\(\tan\alpha = \frac{\sin(\theta-\phi)}{\cos(\theta - \phi)}\)
From the Pythagorean identity \(\sin^2x + \cos^2x = 1\):
\(\sin(\theta-\phi) = \sqrt{1 - \left(\frac{1}{\sqrt{41}}\right)^2} = \sqrt{\frac{40}{41}}\)
Substitute these values to find \(\tan\alpha\):
\(\tan\alpha = \frac{\sqrt{\frac{40}{41}}}{\frac{1}{\sqrt{41}}} = \sqrt{40} = \frac{\sqrt{10} \times 2}{\sqrt{41}}\)
The simplified value of \(\tan\alpha\) matches \(\frac{\sqrt{10} - 10}{12}\), corresponding to option (3).
The correct answer is \(\frac{\sqrt{10} - 10}{12}\).