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: \[ 2(\alpha + \beta + \gamma + \delta) = 2(2 + 2) = 8 \]
In the figure, triangle ABC is equilateral. 
Two positively charged particles \(m_1\) and \(m_2\) have been accelerated across the same potential difference of 200 keV. Given mass of \(m_1 = 1 \,\text{amu}\) and \(m_2 = 4 \,\text{amu}\). The de Broglie wavelength of \(m_1\) will be \(x\) times that of \(m_2\). The value of \(x\) is _______ (nearest integer). 