The given problem asks us to find the sum of the solutions \( x \in \mathbb{R} \) of the equation:
\(\frac{3 \cos 2x + \cos^3 2x}{\cos^6 x - \sin^6 x} = x^3 - x^2 + 6\)
We will solve this equation step-by-step:
Conclusively, the sum of the solutions is:
Therefore, the correct answer is -1.
The given equation is: \(\frac{3\cos 2x + \cos^3 2x}{\cos^6 x - \sin^6 x} = x^3 - x^2 + 6\)
Step 1. Simplify the denominator: Using the identity \( \cos^6 x - \sin^6 x = (\cos^2 x - \sin^2 x)(\cos^4 x + \cos^2 x \sin^2 x + \sin^4 x) \) and substituting \( \cos^2 x - \sin^2 x = \cos 2x \), we get:
\(\cos^6 x - \sin^6 x = \cos 2x \cdot (1 - \sin^2 x \cos^2 x)\)
Step 2. Rewrite the equation: Substitute this into the left side:
\(\frac{\cos 2x(3 + \cos^2 2x)}{\cos 2x(1 - \sin^2 x \cos^2 x)} = x^3 - x^2 + 6\)
Simplifying further, we get:
\(\frac{4(3 + \cos^2 2x)}{(4 - \sin^2 2x)} = x^3 - x^2 + 6\)
which simplifies to:
\(\frac{4(3 + \cos^2 2x)}{(3 + \cos^2 2x)} = x^3 - x^2 + 6\)
Step 3. Solve the resulting polynomial equation: Expanding and rearranging terms, we get: \(x^3 - x^2 + 2 = 0\)
Factorizing gives:
\((x + 1)(x^2 - 2x + 2) = 0\)
So the real root is \( x = -1 \).
Step 4. Calculate the sum of real solutions: Since \( x = -1 \) is the only real solution, the sum of real solutions is: -1
The Correct Answer is: -1
A conducting bar moves on two conducting rails as shown in the figure. A constant magnetic field \( B \) exists into the page. The bar starts to move from the vertex at time \( t = 0 \) with a constant velocity. If the induced EMF is \( E \propto t^n \), then the value of \( n \) is _____. 