To solve the given problem, we need to evaluate the expression for \( f'(x) \) at \( x = 0 \) and find \( \frac{1}{5} f'(0) \).
The function given is:
| \( f(x) = \begin{vmatrix} 2 \cos^4 x & 2 \sin^4 x & 3 + \sin^2 2x \\ 3 + 2 \cos^4 x & 2 \sin^4 x & \sin^2 2x \\ 2 \cos^4 x & 3 + 2 \sin^4 x & \sin^2 2x \end{vmatrix} \) |
We need to differentiate this determinant with respect to \( x \) and find the value at \( x = 0 \).
Let's breakdown \( \sin^2 2x \) and \( \cos^4 x \) as:
First, substitute \( x = 0 \) into \( f(x) \) to find \( f(0) \):
Thus, the matrix at \( x = 0 \) becomes:
| \( f(0) = \begin{vmatrix} 2 & 0 & 3 \\ 5 & 0 & 0 \\ 2 & 3 & 0 \end{vmatrix} \) |
Calculate the determinant at \( x = 0 \):
Now we need \( f'(0) \). For this, differentiate each function inside the determinant with respect to \( x \) and substitute \( x = 0 \):
Using Leibniz rule for the derivative of the determinant, which is quite complicated, we notice that:
Thus, at \( x = 0 \), it leads to a stable determinant even after differentiations considering levels of polynomial multiplication by terms having no linear variations at that instant \( x \). Hence, \( f'(0) = 0 \).
Finally, calculate \( \frac{1}{5} f'(0) \). Since \( f'(0) = 0 \), we have:
\(\frac{1}{5} f'(0) = \frac{1}{5} \times 0 = 0\).
Therefore, the correct answer is: 0
By simplifying the determinant using row operations:
\( R_2 \rightarrow R_2 - R_1 \), \( R_3 \rightarrow R_3 - R_1 \)
we find that \( f(x) \) is constant. Therefore, \( f'(x) = 0 \).
Thus,
\[ \frac{1}{5} f'(0) = 0 \]
If $ A = \begin{pmatrix} 2 & 2 + p & 2 + p + q \\ 4 & 6 + 2p & 8 + 3p + 2q \\ 6 & 12 + 3p & 20 + 6p + 3q \end{pmatrix} $, then the value of $ \det(\text{adj}(\text{adj}(3A))) = 2^m \cdot 3^n $, then $ m + n $ is equal to:
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,