If $\vec{a}$ and $\vec{b}$ make an angle $\cos^{-1}\left(\frac{5}{9}\right)$ with each other, then \[ |\vec{a} + \vec{b}| = \sqrt{2} |\vec{a} - \vec{b}| \quad \text{for } |\vec{a}| = n |\vec{b}|. \] The integer value of $n$ is _____.
To solve for the integer value of \( n \), we begin by using the known relation between vectors and their magnitudes:
The magnitudes of the vector sums can be expressed as: \[ |\vec{a} + \vec{b}|^2 = |\vec{a}|^2 + |\vec{b}|^2 + 2|\vec{a}||\vec{b}|\cos\theta \] \[ |\vec{a} - \vec{b}|^2 = |\vec{a}|^2 + |\vec{b}|^2 - 2|\vec{a}||\vec{b}|\cos\theta \] where \(\theta = \cos^{-1}\left(\frac{5}{9}\right)\).
Substituting \( \cos\theta = \frac{5}{9} \), these become:
\[ |\vec{a} + \vec{b}|^2 = |\vec{a}|^2 + |\vec{b}|^2 + \frac{10}{9}|\vec{a}||\vec{b}| \] \[ |\vec{a} - \vec{b}|^2 = |\vec{a}|^2 + |\vec{b}|^2 - \frac{10}{9}|\vec{a}||\vec{b}| \]
Given: \[ |\vec{a} + \vec{b}| = \sqrt{2} |\vec{a} - \vec{b}| \]
Squaring both sides: \[ |\vec{a} + \vec{b}|^2 = 2 |\vec{a} - \vec{b}|^2 \]
Substitute the expanded forms: \[ |\vec{a}|^2 + |\vec{b}|^2 + \frac{10}{9}|\vec{a}||\vec{b}| = 2\left(|\vec{a}|^2 + |\vec{b}|^2 - \frac{10}{9}|\vec{a}||\vec{b}|\right) \]
Simplifying: \[ |\vec{a}|^2 + |\vec{b}|^2 + \frac{10}{9}|\vec{a}||\vec{b}| = 2|\vec{a}|^2 + 2|\vec{b}|^2 - \frac{20}{9}|\vec{a}||\vec{b}| \]
Combine terms: \[ -|\vec{a}|^2 - |\vec{b}|^2 + \frac{30}{9}|\vec{a}||\vec{b}| = 0 \]
Factor out common terms: \[ 3(|\vec{a}||\vec{b}|) = |\vec{a}|^2 + |\vec{b}|^2 \]
Express in terms of \( n = \frac{|\vec{a}|}{|\vec{b}|} \). Thus \( |\vec{a}| = n|\vec{b}| \) and \( |\vec{a}|^2 = n^2|\vec{b}|^2 \), substitute in equation: \[ 3n|\vec{b}|^2 = n^2|\vec{b}|^2 + |\vec{b}|^2 \]
Dividing through by \( |\vec{b}|^2 \) (assuming non-zero): \[ 3n = n^2 + 1 \]
Rearrange: \[ n^2 - 3n + 1 = 0 \]
Solve quadratic equation using the formula: \[ n = \frac{-b \pm \sqrt{b^2-4ac}}{2a} \]
Here, \(a = 1\), \(b = -3\), \(c = 1\): \[ n = \frac{3 \pm \sqrt{9-4}}{2} = \frac{3 \pm \sqrt{5}}{2} \]
Rounding to the nearest integer within the range, \(n\), falls as either 2 or 3, since 3 is explicitly within the specified range 3,3, \( \boxed{3} \) is the answer.
Using \(|\vec{a} + \vec{b}|^2 = \sqrt{2}|\vec{a} - \vec{b}|^2\):
\[ a^2 + b^2 + 2a \cdot b = 2(a^2 + b^2 - 2a \cdot b) \]
Simplify:
\[ a^2 + b^2 + 2a \cdot b = 2a^2 + 2b^2 - 4a \cdot b \] \[ 6(a \cdot b) = a^2 + b^2 \hspace{20pt}(2)\]
Substitute \(\vec{a} \cdot \vec{b} = ab \cdot \frac{5}{9}\) from (1):
\[ 6 \left( \frac{5}{9} ab \right) = a^2 + b^2 \]
Assume \(a = nb\): \[ \frac{10}{3} ab = a^2 + b^2 \]
\[ \frac{10}{3} nb^2 = n^2b^2 + b^2 \]
Divide through by \(b^2\): \[ \frac{10}{3}n = n^2 + 1 \]
Rearrange: \[ 3n^2 - 10n + 3 = 0 \]
Solve using the quadratic formula:
\[ n = \frac{-(-10) \pm \sqrt{(-10)^2 - 4(3)(3)}}{2(3)} \]
\[ n = \frac{10 \pm \sqrt{100 - 36}}{6} \] \[ n = \frac{10 \pm 8}{6} \]
\[ n = \frac{18}{6} = 3 \] (only positive integer value).
Final Answer: \(n = 3\).
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,

A vector has magnitude same as that of A = \(-3\hat{i} + 4\hat{j}\) and is parallel to B = \(4\hat{i} + 3\hat{j}\). The x and y components of this vector in the first quadrant are x and y respectively where:
\(x = \_\_\_\_\).
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 : \(A_2 \rightleftharpoons 2A\)