We are given two equations to solve for \( \theta \) in the interval \([0, 2\pi]\):
Let's analyze each equation:
Equation (1): \( 2\sin^2\theta = \cos 2\theta \)
We know \(\cos 2\theta = 1-2\sin^2\theta\) from the double angle identity. Substitute it into the equation:
\( 2\sin^2\theta = 1 - 2\sin^2\theta \)
Add \( 2\sin^2\theta \) to both sides:
\( 4\sin^2\theta = 1 \)
Divide by 4:
\( \sin^2\theta = \frac{1}{4} \)
Taking the square root yields:
\( \sin\theta = \frac{1}{2} \) or \( \sin\theta = -\frac{1}{2} \)
Values are \(\theta = \frac{\pi}{6}, \frac{5\pi}{6}\) for \( \sin\theta = \frac{1}{2} \) and \(\theta = \frac{7\pi}{6}, \frac{11\pi}{6}\) for \(\sin\theta = -\frac{1}{2}\).
Equation (2): \( 2\cos^2\theta = 3\sin\theta \)
Substituting \(\cos^2\theta = 1-\sin^2\theta\) gives:
\( 2(1-\sin^2\theta) = 3\sin\theta \)
\( 2 - 2\sin^2\theta = 3\sin\theta \)
Rearrange:
\( 2\sin^2\theta + 3\sin\theta - 2 = 0 \)
Let \( x = \sin\theta \), then:
\( 2x^2 + 3x - 2 = 0 \)
Solve using the quadratic formula \( x = \frac{-b \pm \sqrt{b^2-4ac}}{2a} \):
\( x = \frac{-3 \pm \sqrt{3^2 - 4\cdot2\cdot(-2)}}{2\cdot2} = \frac{-3 \pm \sqrt{9 + 16}}{4} = \frac{-3 \pm 5}{4} \)
Thus, \( x = \frac{1}{2} \) or \( x = -2 \). Since \(\sin\theta\) cannot be -2, only \(\sin\theta = \frac{1}{2}\) is valid.
Intersection of Solutions:
From both equations, valid solutions for \(\sin\theta = \frac{1}{2}\) are \(\theta = \frac{\pi}{6}\) and \(\theta = \frac{5\pi}{6}\).
Sum of all solutions:
\(\frac{\pi}{6} + \frac{5\pi}{6} = \frac{6\pi}{6} = \pi\)
Thus, the sum of all solutions is \(\pi\).
Step 1: Simplify the first equation.
Using \( \cos 2\theta = 1 - 2\sin^2\theta \), the equation \[ 2\sin^2\theta = \cos 2\theta \] becomes \[ 2\sin^2\theta = 1 - 2\sin^2\theta \;\Longrightarrow\; 4\sin^2\theta = 1 \;\Longrightarrow\; \sin\theta = \pm \tfrac{1}{2}. \]
Step 2: Simplify the second equation.
From \( \cos^2\theta = 1 - \sin^2\theta \), the equation \[ 2\cos^2\theta = 3\sin\theta \] gives \[ 2(1 - \sin^2\theta) = 3\sin\theta \;\Longrightarrow\; 2 - 2\sin^2\theta = 3\sin\theta. \] Let \( s = \sin\theta \). Then \[ 2s^2 + 3s - 2 = 0 \;\Longrightarrow\; s = \frac{-3 \pm \sqrt{9 + 16}}{4} = \frac{-3 \pm 5}{4}. \] Hence \( s = \tfrac{1}{2} \) or \( s = -2 \). Since \( \sin\theta \in [-1,1] \), the only admissible solution is \[ \sin\theta = \tfrac{1}{2}. \]
Step 3: Common solutions to both equations.
From Step 1, \( \sin\theta = \pm \tfrac{1}{2} \), and from Step 2, \( \sin\theta = \tfrac{1}{2} \).
Therefore, the common solutions satisfy \( \sin\theta = \tfrac{1}{2} \) in \( [0, 2\pi] \): \[ \theta = \frac{\pi}{6},\; \frac{5\pi}{6}. \]
Step 4: Sum of all solutions.
\[ \frac{\pi}{6} + \frac{5\pi}{6} = \pi. \]
\[ \boxed{\pi} \]
If $ \theta \in [-2\pi,\ 2\pi] $, then the number of solutions of $$ 2\sqrt{2} \cos^2\theta + (2 - \sqrt{6}) \cos\theta - \sqrt{3} = 0 $$ is:
The number of solutions of the equation $ \cos 2\theta \cos \left( \frac{\theta}{2} \right) + \cos \left( \frac{5\theta}{2} \right) = 2 \cos^3 \left( \frac{5\theta}{2} \right) $ in the interval \(\left[ -\frac{\pi}{2}, \frac{\pi}{2} \right ]\) is:
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 _____. 