To solve the problem, let's start by analyzing the given condition:
\[\frac{| \vec{a} + \vec{b} | + | \vec{a} - \vec{b} |}{| \vec{a} + \vec{b} | - | \vec{a} - \vec{b} |} = \sqrt{2} + 1\]The vectors \(\vec{a}\) and \(\vec{b}\) have the same magnitude, so \(|\vec{a}| = |\vec{b}| = a\)\). Using the identity for the magnitudes:
\[|\vec{a} + \vec{b}| = \sqrt{|\vec{a}|^2 + |\vec{b}|^2 + 2\vec{a} \cdot \vec{b}} = \sqrt{2a^2 + 2a^2\cos\theta}\]\[|\vec{a} - \vec{b}| = \sqrt{|\vec{a}|^2 + |\vec{b}|^2 - 2\vec{a} \cdot \vec{b}} = \sqrt{2a^2 - 2a^2\cos\theta}\]Let us denote:
Then, applying the identity, we have:
\[x + y = \sqrt{2a^2(1 + \cos\theta)} + \sqrt{2a^2(1 - \cos\theta)} \] \] \] \] \] \] \[ x - y = \sqrt{2a^2(1 + \cos\theta)} - \sqrt{2a^2(1 - \cos\theta)} \] \] \] \] \]\]Now, consider the given condition again:
\[\frac{x + y}{x - y} = \sqrt{2} + 1 \] \] \] \] \] \] \[ \Rightarrow x + y = (\sqrt{2} + 1)(x - y) \] \] \] \] \]\]Substituting \(x = ka\)\)and \(y = ma\)\)in value where \(k\)\)and \(m\)\)are unknown constants, we solve for:
\[k + m = (\sqrt{2} + 1)(k - m) \] \] \] \] \] \] \[ \Rightarrow k + m = (\sqrt{2} + 1)(k - m) \] \] \] \] \]\]Cross-multiplying and simplifying, we arrive at \(\cos\theta = \frac{1}{\sqrt{2}}\). Consequently, \(|\vec{a} + \vec{b}|^2 = 2a^2 + 2a^2\frac{1}{\sqrt{2}}\)\) can be endeavored:
\[\Rightarrow |\vec{a} + \vec{b}|^2 = 2a^2 + \sqrt{2}a^2\]Thus,
\[\frac{|\vec{a} + \vec{b}|^2}{|\vec{a}|^2} = 2 + \sqrt{2}\]Hence, the given expression evaluates to: \(2 + \sqrt{2}\).
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,