The function given is \(f(x) = \frac{x}{x^2 - 6x - 16}\). To determine where this function increases or decreases, we first need to find its derivative.
This is a quotient of two functions, so we apply the quotient rule:
\(\frac{d}{dx}\left(\frac{u(x)}{v(x)}\right) = \frac{u'(x) v(x) - u(x) v'(x)}{(v(x))^2}\)
For \(f(x) = \frac{x}{x^2 - 6x - 16}\), let:
Now, apply the quotient rule:
\(f'(x) = \frac{1 \cdot (x^2 - 6x - 16) - x \cdot (2x - 6)}{(x^2 - 6x - 16)^2}\)
Simplify the numerator:
\(= \frac{x^2 - 6x - 16 - (2x^2 - 6x)}{(x^2 - 6x - 16)^2}\)
\(= \frac{x^2 - 6x - 16 - 2x^2 + 6x}{(x^2 - 6x - 16)^2}\)
\(= \frac{-x^2 - 16}{(x^2 - 6x - 16)^2}\)
The critical points are determined by setting the numerator equal to zero. However, \(-x^2 - 16 = 0\) has no real roots (as the equation simplifies to \(x^2 = -16\), which is not possible in real numbers).
Next, examine the sign of \(f'(x)\):
Therefore, \(f'(x)\) is negative for all intervals where the function is defined, indicating that the function \(f(x)\) is decreasing in those intervals.
Thus, the correct answer is that the function decreases in \((-\infty, -2) \cup (-2, 8) \cup (8, \infty)\).
The given function is: \(f(x) = \frac{x}{x^2 - 6x - 16}\)
Step 1. Calculate the derivative \( f'(x) \):\(f'(x) = \frac{-(x^2 + 16)}{(x^2 - 6x - 16)^2}\)
Step 2. Since \( f'(x) < 0 \), the function \( f(x) \) is decreasing in all intervals where it is defined.**
Step 3. Therefore, \( f(x) \) is decreasing in \( (-\infty, -2) \cup (-2, 8) \cup (8, \infty) \).**
The Correct Answer is:\( (-\infty, -2) \cup (-2, 8) \cup (8, \infty) \)
Consider the following sequence of reactions : 
Molar mass of the product formed (A) is ______ g mol\(^{-1}\).
In a Young's double slit experiment, three polarizers are kept as shown in the figure. The transmission axes of \( P_1 \) and \( P_2 \) are orthogonal to each other. The polarizer \( P_3 \) covers both the slits with its transmission axis at \( 45^\circ \) to those of \( P_1 \) and \( P_2 \). An unpolarized light of wavelength \( \lambda \) and intensity \( I_0 \) is incident on \( P_1 \) and \( P_2 \). The intensity at a point after \( P_3 \), where the path difference between the light waves from \( S_1 \) and \( S_2 \) is \( \frac{\lambda}{3} \), is:
