We are given the function \( f(x) = \frac{(2^x + 2^{-x}) \tan x \sqrt{\tan^{-1}(x^2 - x + 1)}}{(7x^2 + 3x + 1)^{3}} \) and we need to find the value of \( f'(0) \).
To solve this, we need to understand that we will apply the rules of differentiation to find \( f'(x) \) and then evaluate it at \( x = 0 \). We should also simplify the expression wherever possible before differentiating.
**Step 1: Understand the components of the function at \( x = 0 \).**
Plugging these values into the function at \( x = 0 \), we find that:
\( f(0) = \frac{2 \cdot 0 \cdot \frac{\sqrt{\pi}}{2}}{1} = 0 \).
This confirms that initially the entire expression evaluates to zero.
**Step 2: Differentiate the expression using the product and quotient rules.**
The given function is a quotient of two functions. According to the quotient rule:
\( \left( \frac{u}{v} \right)' = \frac{u'v - uv'}{v^2} \)
Let:
Evaluate derivatives \( u'(x) \) and \( v'(x) \):
\( f'(0) = \text{depends primarily on the high-order effects of the term derivations}\), and thus the only non-zero influence locally about zero is from the derivative component residing partially from \( \frac{\sqrt{\pi}}{2} \). Therefore, the calculated effect due to simplification leads directly to:
**Conclusion**: The calculated derivative indicates the form \(\sqrt{\pi}\), matching the identity of calculated form upon organize elimination of proximate zeroes.
Thus, the answer is \(\sqrt\pi\).
\[ f'(0) = \lim_{h \to 0} \frac{f(h) - f(0)}{h} \]
Substitute \(x = h\) and \(x = 0\) into \(f(x)\):
\[ f'(0) = \lim_{h \to 0} \frac{\left(2^h + 2^{-h}\right) \tan h \sqrt{\tan^{-1}(h^2 - h + 1)} - 0}{(7h^2 + 3h + 1)^3 \cdot h} \]
Using the limit properties, we get:
\[ f'(0) = \sqrt{\pi} \]
So, the correct answer is: \(\sqrt{\pi}\)
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:
