\(\frac{\pi}{6}\)
\(\frac{5\pi}{12}\)
\(\frac{\pi}{3}\)
\(\frac{\pi}{4}\)
For the hyperbola, the eccentricity is given by:
\[ e_h = \sqrt{1 + \sin^2 \theta} \]
For the ellipse, the eccentricity is given by:
\[ e_e = \sqrt{1 - \sin^2 \theta} \]
We are given that the eccentricity of the hyperbola is \(\sqrt{7}\) times the eccentricity of the ellipse:
\[ e_h = \sqrt{7} \cdot e_e \]
Substituting the expressions for \(e_h\) and \(e_e\):
\[ \sqrt{1 + \sin^2 \theta} = \sqrt{7} \cdot \sqrt{1 - \sin^2 \theta} \]
Squaring both sides:
\[ 1 + \sin^2 \theta = 7(1 - \sin^2 \theta) \]
Expanding:
\[ 1 + \sin^2 \theta = 7 - 7 \sin^2 \theta \]
Simplifying:
\[ 1 + \sin^2 \theta + 7 \sin^2 \theta = 7 \]
\[ 8 \sin^2 \theta = 6 \]
\[ \sin^2 \theta = \frac{3}{4} \]
Thus:
\[ \sin \theta = \frac{\sqrt{3}}{2} \]
Therefore:
\[ \theta = \frac{\pi}{3} \]
For \( 0 < \theta < \frac{\pi}{2} \), given that the eccentricity of the hyperbola \( x^2 - y^2 \csc^2 \theta = 5 \) is \( \sqrt{7} \) times the eccentricity of the ellipse \( x^2 \csc^2 \theta + y^2 = 5 \), find \( \theta \).
For a hyperbola \( \frac{x^2}{a^2} - \frac{y^2}{b^2} = 1 \), eccentricity \( e_h = \sqrt{1 + \frac{b^2}{a^2}} \).
For an ellipse \( \frac{x^2}{a^2} + \frac{y^2}{b^2} = 1 \) (with \( a > b \)), eccentricity \( e_e = \sqrt{1 - \frac{b^2}{a^2}} \).
Step 1: Write both equations in standard form.
Hyperbola: \( x^2 - y^2 \csc^2 \theta = 5 \)
Divide by 5: \( \frac{x^2}{5} - \frac{y^2}{5 \sin^2 \theta} = 1 \).
So \( a_h^2 = 5 \), \( b_h^2 = 5 \sin^2 \theta \).
Ellipse: \( x^2 \csc^2 \theta + y^2 = 5 \)
Divide by 5: \( \frac{x^2}{5 \sin^2 \theta} + \frac{y^2}{5} = 1 \).
Here, denominator of \( x^2 \) is \( 5 \sin^2 \theta \), of \( y^2 \) is 5.
Since \( 0 < \theta < \frac{\pi}{2} \), \( 0 < \sin \theta < 1 \), so \( 5 \sin^2 \theta < 5 \).
Thus \( a_e^2 = 5 \) (semi-major axis along y-axis), \( b_e^2 = 5 \sin^2 \theta \).
Step 2: Find eccentricities.
Hyperbola: \( e_h = \sqrt{1 + \frac{b_h^2}{a_h^2}} = \sqrt{1 + \frac{5 \sin^2 \theta}{5}} = \sqrt{1 + \sin^2 \theta} \).
Ellipse: \( e_e = \sqrt{1 - \frac{b_e^2}{a_e^2}} = \sqrt{1 - \frac{5 \sin^2 \theta}{5}} = \sqrt{1 - \sin^2 \theta} = \sqrt{\cos^2 \theta} = \cos \theta \) (since \( \cos \theta > 0 \) in given domain).
Step 3: Use given condition.
Given: \( e_h = \sqrt{7} \, e_e \)
So \( \sqrt{1 + \sin^2 \theta} = \sqrt{7} \cos \theta \).
Step 4: Solve for \( \sin^2 \theta \).
Square both sides: \( 1 + \sin^2 \theta = 7 \cos^2 \theta \).
But \( \cos^2 \theta = 1 - \sin^2 \theta \), so:
\( 1 + \sin^2 \theta = 7(1 - \sin^2 \theta) \)
\( 1 + \sin^2 \theta = 7 - 7 \sin^2 \theta \)
\( 8 \sin^2 \theta = 6 \)
\( \sin^2 \theta = \frac{3}{4} \).
Step 5: Find \( \theta \).
\( \sin \theta = \frac{\sqrt{3}}{2} \) (since \( \sin \theta > 0 \))
So \( \theta = \frac{\pi}{3} \).
Therefore, the value of \( \theta \) is \( \mathbf{\frac{\pi}{3}} \).
In the given figure, the blocks $A$, $B$ and $C$ weigh $4\,\text{kg}$, $6\,\text{kg}$ and $8\,\text{kg}$ respectively. The coefficient of sliding friction between any two surfaces is $0.5$. The force $\vec{F}$ required to slide the block $C$ with constant speed is ___ N.
(Given: $g = 10\,\text{m s}^{-2}$) 
Two circular discs of radius \(10\) cm each are joined at their centres by a rod, as shown in the figure. The length of the rod is \(30\) cm and its mass is \(600\) g. The mass of each disc is also \(600\) g. If the applied torque between the two discs is \(43\times10^{-7}\) dyne·cm, then the angular acceleration of the system about the given axis \(AB\) is ________ rad s\(^{-2}\).
