To solve the given problem, we start by analyzing the condition \(\vec{b} \times \vec{a} = \vec{c} \times \vec{a}\). Given the vectors: \(\vec{a} = \hat{i} + \hat{j} + \hat{k}\), \(\vec{b} = -\hat{i} - 8\hat{j} + 2\hat{k}\), and \(\vec{c} = 4\hat{i} + c_2\hat{j} + c_3\hat{k}\), the condition implies that \((\vec{b} - \vec{c}) \times \vec{a} = \vec{0}\). This means \(\vec{b} - \vec{c}\) is parallel to \(\vec{a}\).
Calculating \(\vec{b} - \vec{c}\):
\(\vec{b} - \vec{c} = (-1 - 4)\hat{i} + (-8 - c_2)\hat{j} + (2 - c_3)\hat{k} = -5\hat{i} + (-8 - c_2)\hat{j} + (2 - c_3)\hat{k}\).
Since \(\vec{b} - \vec{c}\) is parallel to \(\vec{a}\), it must be a scalar multiple: \(-5\hat{i} + (-8 - c_2)\hat{j} + (2 - c_3)\hat{k} = \lambda(\hat{i} + \hat{j} + \hat{k})\).
Equating components, we get:
- \(-5 = \lambda\)
- \(-8 - c_2 = \lambda\)
- \(2 - c_3 = \lambda\)
Solving these equations:
- From \(-5 = \lambda\), we have \(\lambda = -5\).
- Plugging \(\lambda = -5\) into \(-8 - c_2 = \lambda\):
\(-8 - c_2 = -5 \Rightarrow c_2 = -3\).
- Plugging \(\lambda = -5\) into \(2 - c_3 = \lambda\):
\(2 - c_3 = -5 \Rightarrow c_3 = 7\).
Thus, \(\vec{c} = 4\hat{i} - 3\hat{j} + 7\hat{k}\).
Next, consider the angle \(\theta\) between \(\vec{c}\) and \(3\hat{i} + 4\hat{j} + \hat{k}\).
The cosine of the angle is given by the formula:
\[\cos \theta = \frac{\vec{c} \cdot (3\hat{i} + 4\hat{j} + \hat{k})}{|\vec{c}||3\hat{i} + 4\hat{j} + \hat{k}|}\]
Calculating the dot product \(\vec{c} \cdot (3\hat{i} + 4\hat{j} + \hat{k})\):
\(= (4 \cdot 3) + (-3 \cdot 4) + (7 \cdot 1) = 12 - 12 + 7 = 7\).
Finding the magnitudes:
- \(|\vec{c}| = \sqrt{4^2 + (-3)^2 + 7^2} = \sqrt{16 + 9 + 49} = \sqrt{74}\).
- \(|3\hat{i} + 4\hat{j} + \hat{k}| = \sqrt{3^2 + 4^2 + 1^2} = \sqrt{9 + 16 + 1} = \sqrt{26}\).
Thus, \(\cos \theta = \frac{7}{\sqrt{74} \cdot \sqrt{26}} = \frac{7}{\sqrt{1924}}\).
Using \(\cos^2 \theta + \sin^2 \theta = 1\), find \(\sin^2 \theta\):
\(\sin^2 \theta = 1 - \cos^2 \theta = 1 - \left(\frac{7^2}{1924}\right) = 1 - \frac{49}{1924} = \frac{1924 - 49}{1924} = \frac{1875}{1924}\).
Then calculate \(\tan^2 \theta = \frac{\sin^2 \theta}{\cos^2 \theta}\):
\(\tan^2 \theta = \frac{\frac{1875}{1924}}{\frac{49}{1924}} = \frac{1875}{49} \approx 38.2653\).
The greatest integer less than or equal to \(\tan^2 \theta\) is \(38\), which matches the expected range (38,38).
Calculate $\vec{b} \times \vec{a}$:
\(\vec{b} \times \vec{a}\) = \(\begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \ -1 & -8 & 21 \ 1 & 1 & 1 \end{vmatrix} = -10\hat{i} + 3\hat{j} + 7\hat{k}\)
Since \(\vec{b} \times \vec{a} = \vec{c} \times \vec{a},\) we have:
$-10\hat{i} + 3\hat{j} + 7\hat{k} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \ c_1 & c_2 & c_3 \ 1 & 1 & 1 \end{vmatrix}$
Expanding the determinant, we get:
$-10\hat{i} + 3\hat{j} + 7\hat{k} = (c_2 - c_3)\hat{i} - (c_1 - c_3)\hat{j} + (c_1 - c_2)\hat{k}$
Comparing the coefficients, we get:
$c_2 - c_3 = -10$
$-c_1 + c_3 = -3$
$c_1 - c_2 = 7$
Solving these equations, we find:
$c_2 = -3$
$c_3 = 7$
$c_1 = 4$
So, $\vec{c} = 4\hat{i} - 3\hat{j} + 7\hat{k}$.
Let $\theta$ be the angle between the two vectors. We can use the dot product formula:
$(3\hat{i} + 4\hat{j} + \hat{k}) \cdot \vec{c} = |\vec{c}||3\hat{i} + 4\hat{j} + \hat{k}| \cos \theta$
Calculating the dot product and magnitudes:
$(4,-3,7) \cdot (3,4,1) = \sqrt{74}\sqrt{26} \cos \theta$
Simplifying:
$12 - 12 + 7 = \sqrt{74}\sqrt{26} \cos \theta$
$7 = \sqrt{74}\sqrt{26} \cos \theta$
Solving for $\cos \theta$:
$\cos \theta = \frac{7}{\sqrt{74}\sqrt{26}}$
Using the identity $\sin^2 \theta + \cos^2 \theta = 1$, we can find $\sin \theta$:
$\sin \theta = \sqrt{1 - \cos^2 \theta} = \sqrt{1 - \frac{49}{1924}} = \frac{\sqrt{1875}}{1924}$
Now, we can calculate $\tan^2 \theta$:
$\tan^2 \theta = \frac{\sin^2 \theta}{\cos^2 \theta} = \frac{1875}{49}$
The greatest integer less than or equal to $\frac{1875}{49}$ is 38.
Therefore, the correct answer is 38.
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 _______. 