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: \(2 + \sqrt{2}\).
A substance 'X' (1.5 g) dissolved in 150 g of a solvent 'Y' (molar mass = 300 g mol$^{-1}$) led to an elevation of the boiling point by 0.5 K. The relative lowering in the vapour pressure of the solvent 'Y' is $____________ \(\times 10^{-2}\). (nearest integer)
[Given : $K_{b}$ of the solvent = 5.0 K kg mol$^{-1}$]
Assume the solution to be dilute and no association or dissociation of X takes place in solution.
Inductance of a coil with \(10^4\) turns is \(10\,\text{mH}\) and it is connected to a DC source of \(10\,\text{V}\) with internal resistance \(10\,\Omega\). The energy density in the inductor when the current reaches \( \left(\frac{1}{e}\right) \) of its maximum value is \[ \alpha \pi \times \frac{1}{e^2}\ \text{J m}^{-3}. \] The value of \( \alpha \) is _________.
\[ (\mu_0 = 4\pi \times 10^{-7}\ \text{TmA}^{-1}) \]
A small block of mass \(m\) slides down from the top of a frictionless inclined surface, while the inclined plane is moving towards left with constant acceleration \(a_0\). The angle between the inclined plane and ground is \(\theta\) and its base length is \(L\). Assuming that initially the small block is at the top of the inclined plane, the time it takes to reach the lowest point of the inclined plane is _______. 