We are given:
We know the formula for the latus rectum of an ellipse is:
\[ L = \frac{2b^2}{a} \]
From the problem, we are given \( L = \sqrt{14} \), so:
\[ \frac{2b^2}{a} = \sqrt{14} \]
Thus,
\[ 2b^2 = a \sqrt{14} \tag{1} \]
Next, use the relationship for the eccentricity \( e \) of an ellipse:
\[ e = \sqrt{1 - \frac{b^2}{a^2}} = \frac{1}{\sqrt{2}} \]
Squaring both sides:
\[ e^2 = 1 - \frac{b^2}{a^2} = \frac{1}{2} \]
This implies:
\[ \frac{b^2}{a^2} = \frac{1}{2} \]
Substitute this into equation (1):
\[ 2 \left(\frac{a^2}{2}\right) = a \sqrt{14} \] \[ a^2 = a \sqrt{14} \]
Thus:
\[ a = \sqrt{14} \] 1
Substitute \( a = \sqrt{14} \) into \( b^2 = \frac{a^2}{2} \):
\[ b^2 = \frac{14}{2} = 7 \]
Now, compute the square of the eccentricity:
\[ e^2 = 1 - \frac{b^2}{a^2} = 1 - \frac{7}{14} = \frac{7}{14} = \frac{1}{2} \]
Thus, the square of the eccentricity is \( \frac{3}{2} \).
Two cells of emf 1V and 2V and internal resistance 2 \( \Omega \) and 1 \( \Omega \), respectively, are connected in series with an external resistance of 6 \( \Omega \). The total current in the circuit is \( I_1 \). Now the same two cells in parallel configuration are connected to the same external resistance. In this case, the total current drawn is \( I_2 \). The value of \( \left( \frac{I_1}{I_2} \right) \) is \( \frac{x}{3} \). The value of x is 1cm.
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 term independent of $ x $ in the expansion of $$ \left( \frac{x + 1}{x^{3/2} + 1 - \sqrt{x}} \cdot \frac{x + 1}{x - \sqrt{x}} \right)^{10} $$ for $ x>1 $ is:
Consider the following reaction occurring in the blast furnace. \[ {Fe}_3{O}_4(s) + 4{CO}(g) \rightarrow 3{Fe}(l) + 4{CO}_2(g) \] ‘x’ kg of iron is produced when \(2.32 \times 10^3\) kg \(Fe_3O_4\) and \(2.8 \times 10^2 \) kg CO are brought together in the furnace.
The value of ‘x’ is __________ (nearest integer).