To solve this problem, we need to determine the value of \( 2 (\alpha + \beta + \gamma + \delta) \) given the conditions of the parallelogram.
The points \( A(\alpha, \beta) \) and \( C(\gamma, \delta) \) both lie on the line described by the equation \( 3y = 2x + 1 \). Therefore, we can write down the following equations for these points:
We know that the distance \( AB = \sqrt{10} \). For points \( A(\alpha, \beta) \) and \( B(1, 0) \), the distance formula gives:
\(AB = \sqrt{(\alpha - 1)^2 + (\beta - 0)^2} = \sqrt{10}\)
Squaring both sides, we get:
\((\alpha - 1)^2 + \beta^2 = 10\)
In a parallelogram, opposite sides are equal and parallel. Thus, vectors \( \overrightarrow{AB} \) and \( \overrightarrow{CD} \) are equal, and vectors \( \overrightarrow{AD} \) and \( \overrightarrow{BC} \) are also equal. Calculate the vectors:
From these equations, it simplifies to:
We now have the following equations:
Substituting from equation 4 into 1 and 2:
If \(\beta = 1\), then \(\delta = 1\).
Substitute into either line equation: \(3(1) = 2\alpha + 1 \Rightarrow \alpha = 1\).
With \(\alpha = 1\), \(\beta = 1\), \(\gamma = 1\), \(\delta = 1\), compute the required expression:
\(2(\alpha + \beta + \gamma + \delta) = 2(1 + 1 + 1 + 1) = 8\)
The calculated result is 8. This corresponds to the given correct answer.
Let \( E \) be the midpoint of the diagonals. By the midpoint formula: \[ \frac{\alpha + \gamma}{2} = \frac{1 + 1}{2} = 1 \quad \implies \quad \alpha + \gamma = 2 \] Similarly: \[ \frac{\beta + \delta}{2} = \frac{2 + 0}{2} = 1 \quad \implies \quad \beta + \delta = 2 \] Therefore: \[ 2(\alpha + \beta + \gamma + \delta) = 2(2 + 2) = 8 \]
Consider the following sequence of reactions : 
Molar mass of the product formed (A) is ______ g mol\(^{-1}\).
In a Young's double slit experiment, three polarizers are kept as shown in the figure. The transmission axes of \( P_1 \) and \( P_2 \) are orthogonal to each other. The polarizer \( P_3 \) covers both the slits with its transmission axis at \( 45^\circ \) to those of \( P_1 \) and \( P_2 \). An unpolarized light of wavelength \( \lambda \) and intensity \( I_0 \) is incident on \( P_1 \) and \( P_2 \). The intensity at a point after \( P_3 \), where the path difference between the light waves from \( S_1 \) and \( S_2 \) is \( \frac{\lambda}{3} \), is:
