Let \(\vec{u} = \hat{i}\) and \(\vec{OQ} = \hat{j}\). Since R is the midpoint of the arc PQ, \(\vec{OR}\) bisects the right angle \(\vec{POQ}\). We can express \(\vec{v}\) in terms of \(\vec{u}\) and \(\vec{OQ}\) (which we’ve set as \(\hat{i}\) and \(\hat{j}\) respectively).
Since R is the midpoint of the arc PQ, the vector \(\vec{OR}\) is given by:
\( \vec{v} = \frac{1}{\sqrt{2}} \hat{i} + \frac{1}{\sqrt{2}} \hat{j} \)
Given that \( \vec{OQ} = \alpha \vec{u} + \beta \vec{v} \), we have:
\( \hat{j} = \alpha \hat{i} + \beta \left( \frac{1}{\sqrt{2}} \hat{i} + \frac{1}{\sqrt{2}} \hat{j} \right) \)
\( \hat{j} = \left( \alpha + \frac{\beta}{\sqrt{2}} \right) \hat{i} + \frac{\beta}{\sqrt{2}} \hat{j} \)
Comparing the coefficients of \(\hat{i}\) and \(\hat{j}\) on both sides, we get:
\( \alpha + \frac{\beta}{\sqrt{2}} = 0 \quad \text{and} \quad \frac{\beta}{\sqrt{2}} = 1 \)
From the second equation, \( \beta = \sqrt{2} \). Substituting this into the first equation gives:
\( \alpha + \frac{\sqrt{2}}{\sqrt{2}} = 0 , \quad \text{so} \quad \alpha = -1 \)
We are given that \(\alpha\) and \(\beta^2\) are the roots of a quadratic equation.
Since \(\alpha = -1\) and \(\beta = \sqrt{2}\), then \( \beta^2 = 2 \).
Let the quadratic equation be \( x^2 + bx + c = 0 \).
The sum of the roots is \( -b = \alpha + \beta^2 = -1 + 2 = 1 \), so \( b = -1 \).
The product of the roots is \( c = \alpha \cdot \beta^2 = (-1)(2) = -2 \).
Therefore, the quadratic equation is \( x^2 - x - 2 = 0 \).
What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,