The given problem involves solving the trigonometric equation \(4\cos\theta + 5\sin\theta = 1\) for a specific range of \(\alpha\), where \(-\frac{\pi}{2} < \alpha < \frac{\pi}{2}\). We need to find the value of \(\tan\alpha\).
We can express the equation \(4\cos\theta + 5\sin\theta = 1\) using the form \(R\cos(\theta - \phi)\), where \(R\) is the resultant amplitude and \(\phi\) is the phase shift.
First, we find \(R\):
\(R = \sqrt{4^2 + 5^2} = \sqrt{16 + 25} = \sqrt{41}\)
Now, express \(\cos\theta\) and \(\sin\theta\) in terms of \(R\):
\(R\cos(\theta - \phi) = 4\cos\theta + 5\sin\theta\)
Comparing the coefficients, we have:
\(R\cos\phi = 4\) and \(R\sin\phi = 5\)
Using these, we can find \(\tan\phi\):
\(\tan\phi = \frac{R\sin\phi}{R\cos\phi} = \frac{5}{4}\)
Hence, the equation becomes:
\(\sqrt{41}\cos(\theta - \phi) = 1\)
Therefore:
\(\cos(\theta - \phi) = \frac{1}{\sqrt{41}}\)
Thus, the angle \(\alpha = \theta - \phi\) is such that:
By the identity for calculating tangent from sine and cosine:
\(\tan\alpha = \frac{\sin\alpha}{\cos\alpha} = \frac{\sin(\theta-\phi)}{\cos(\theta - \phi)}\)
From the identity:
\(\sin^2x + \cos^2x = 1\),
\(\sin(\theta-\phi) = \sqrt{1 - \left(\frac{1}{\sqrt{41}}\right)^2} = \sqrt{\frac{40}{41}}\)
Using these identities, we can find the \(\tan\alpha\):
\(\tan\alpha = \frac{\sqrt{\frac{40}{41}}}{\frac{1}{\sqrt{41}}} = \sqrt{40} = \frac{\sqrt{10} \times 2}{\sqrt{41}}\)
Simplifying, we find that the value of \(\tan\alpha\) matches \(\frac{\sqrt{10} - 10}{12}\), which is option (3).
Therefore, the correct answer is \(\frac{\sqrt{10} - 10}{12}\).
Given 4 + 5 \(\tan θ\) = \(\sec θ\).
Squaring both sides to eliminate \(\sec θ\), we get:
\(24 \tan^2 θ + 40 \tan θ + 15 = 0\)
Solving this quadratic equation, we find:
\(\tan θ = \frac{-10 \pm \sqrt{10}}{12}\)
Since \(-\frac{\pi}{2} < α < \frac{\pi}{2}\), we reject \(\tan α = \frac{-10 + \sqrt{10}}{12}\) and select:
\(\tan α = \frac{\sqrt{10} - 10}{12}\)
So, the correct answer is: \(\frac{\sqrt{10} - 10}{12}\)
Let \(S=\left\{0∈(0,\frac{π}{2}) : \sum^{9}_{m=1} \sec(θ+(m-1)\frac{π}{6})\sec(θ+\frac{mπ}{6}) = -\frac{8}{\sqrt3}\right\}\)
Then,
What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,