Given that the midpoint of the chord is \( \left( \sqrt{2}, \frac{4}{3} \right) \), and the length of the chord is \( \frac{2\sqrt{\alpha}}{3} \).
The equation of the chord is derived using the midpoint formula, and we compute the length of the chord: \[ \sqrt{2x + 3y} = 6 \Rightarrow y = \frac{6 - \sqrt{2x}}{3} \quad {(put in ellipse form)} \] \[ {So, } \frac{x^2}{9} + \left( \frac{6 - \sqrt{2x}}{9 \times 4} \right)^2 = 1 \] \[ 4x^2 + 36 + 2x^2 - 12 \sqrt{2x} = 36 \] \[ 6x^2 - 12 \sqrt{2x} = 0 \] \[ 6x(x - \sqrt{2}) = 0 \] \[ x = 0 \quad {or} \quad x = \sqrt{2} \] So, \( y = 2 \) or \( y = \frac{2}{3} \) \[ {Length of chord} = \sqrt{\left( 2\sqrt{2} - 0 \right)^2 + \left( \frac{2}{3} - 2 \right)^2} \] \[ = \sqrt{8 + \frac{16}{9}} = \sqrt{\frac{88}{9}} = \frac{2}{3} \sqrt{22} \] \[ \Rightarrow \alpha = 22 \] Thus, \( \alpha = 22 \).
The value of current \( I \) in the electrical circuit as given below, when the potential at \( A \) is equal to the potential at \( B \), will be _____ A.
Two light beams fall on a transparent material block at point 1 and 2 with angle \( \theta_1 \) and \( \theta_2 \), respectively, as shown in the figure. After refraction, the beams intersect at point 3 which is exactly on the interface at the other end of the block. Given: the distance between 1 and 2, \( d = \frac{4}{3} \) cm and \( \theta_1 = \theta_2 = \cos^{-1} \left( \frac{n_2}{2n_1} \right) \), where \( n_2 \) is the refractive index of the block and \( n_1 \) is the refractive index of the outside medium, then the thickness of the block is …….. cm.