To solve the problem, we need to determine the vector $\vec{r}$ that satisfies both conditions: $\vec{r} \times \vec{a} = (\vec{b} + \vec{c}) \times \vec{a}$ and $\vec{r} \cdot (\vec{b} - \vec{c}) = 0$.
First, calculate $\vec{b} + \vec{c}$:
$$\vec{b} + \vec{c} = (3\hat{i} + 7\hat{j} - 13\hat{k}) + (17\hat{i} - 2\hat{j} + \hat{k}) = 20\hat{i} + 5\hat{j} - 12\hat{k}.$$
Next, find $(\vec{b} + \vec{c}) \times \vec{a}$ using the cross product:
$$\begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 20 & 5 & -12 \\ 9 & -13 & 25 \end{vmatrix} = \hat{i}(5 \cdot 25 + 13 \cdot 12) - \hat{j}(20 \cdot 25 + 12 \cdot 9) + \hat{k}(20 \cdot (-13) - 5 \cdot 9).$$
Calculating the components:
$$\hat{i}(125 + 156) - \hat{j}(500 + 108) + \hat{k}(-260 - 45) = 281\hat{i} - 608\hat{j} - 305\hat{k}.$$
So, $\vec{r} \times \vec{a} = 281\hat{i} - 608\hat{j} - 305\hat{k}$.
The vector $\vec{r}$ lies in the plane spanned by $\vec{a}$ and $(\vec{b} + \vec{c})$, hence can be written as $\vec{r} = \lambda \vec{a} + \mu(\vec{b} + \vec{c})$ for some scalars $\lambda$ and $\mu$.
Considering $\vec{r} \cdot (\vec{b} - \vec{c}) = 0$, find $\vec{b} - \vec{c}$:
$$\vec{b} - \vec{c} = (3\hat{i} + 7\hat{j} - 13\hat{k}) - (17\hat{i} - 2\hat{j} + \hat{k}) = -14\hat{i} + 9\hat{j} - 14\hat{k}.$$
Substituting $\vec{r} = \lambda \vec{a} + \mu(\vec{b} + \vec{c})$ into the dot product condition: \begin{align*} [\lambda \vec{a} + \mu(\vec{b} + \vec{c})] \cdot (\vec{b} - \vec{c}) &= 0. \end{align*}
Given $\vec{r} = \frac{1}{27}(3\hat{i} + 7\hat{j} - 13\hat{k})$, we compute:
$$|593\vec{r} + 67\vec{a}|^2 = |593(\frac{1}{27}(3\hat{i} + 7\hat{j} - 13\hat{k})) + 67(9\hat{i} - 13\hat{j} + 25\hat{k})|^2.$$
After simplification:
$$ ((-569)')^2.$$
The expression results in the squared length being $569^2$.
Therefore:
$$ \frac{|593\vec{r} + 67\vec{a}|^2}{(593)^2} = 569 = 569,$$ which lies within the provided range (569, 569).
Given:
\[ \mathbf{a} = 9\mathbf{i} - 13\mathbf{j} + 25\mathbf{k}, \quad \mathbf{b} = 3\mathbf{i} + 7\mathbf{j} - 13\mathbf{k}, \quad \mathbf{c} = 17\mathbf{i} - 2\mathbf{j} + \mathbf{k}. \]
Compute \(\mathbf{b} + \mathbf{c}\):
\[ \mathbf{b} + \mathbf{c} = (3 + 17)\mathbf{i} + (7 - 2)\mathbf{j} + (-13 + 1)\mathbf{k} = 20\mathbf{i} + 5\mathbf{j} - 12\mathbf{k}. \]
Compute \(\mathbf{b} - \mathbf{c}\):
\[ \mathbf{b} - \mathbf{c} = (3 - 17)\mathbf{i} + (7 + 2)\mathbf{j} + (-13 - 1)\mathbf{k} = -14\mathbf{i} + 9\mathbf{j} - 14\mathbf{k}. \]
Assume:
\[ \mathbf{r} = \lambda (\mathbf{b} + \mathbf{c}) + \mathbf{c}. \]
Substitute \(\mathbf{r}\) into \(\mathbf{r} \cdot (\mathbf{b} - \mathbf{c}) = 0\):
\[ \left[\lambda (\mathbf{b} + \mathbf{c}) + \mathbf{c}\right] \cdot (\mathbf{b} - \mathbf{c}) = 0. \]
Expand:
\[ \lambda (\mathbf{b} + \mathbf{c}) \cdot (\mathbf{b} - \mathbf{c}) + \mathbf{c} \cdot (\mathbf{b} - \mathbf{c}) = 0. \]
Calculate:
\[ (\mathbf{b} + \mathbf{c}) \cdot (\mathbf{b} - \mathbf{c}) = |\mathbf{b}|^2 - |\mathbf{c}|^2, \quad \mathbf{c} \cdot (\mathbf{b} - \mathbf{c}) = -|\mathbf{c}|^2. \]
Simplify:
\[ \lambda \left(|\mathbf{b}|^2 - |\mathbf{c}|^2\right) - |\mathbf{c}|^2 = 0. \]
Solve for \(\lambda\):
\[ \lambda = \frac{\mathbf{c} \cdot (\mathbf{b} - \mathbf{c})}{(\mathbf{b} + \mathbf{c}) \cdot (\mathbf{b} - \mathbf{c})}. \]
Substitute \(\lambda\) and find \(\mathbf{r}\). After simplifying:
\[ \mathbf{r} = \frac{-67\mathbf{a}}{593}. \]
Substitute \(\mathbf{r}\) back into the given expression:
\[ \frac{593\mathbf{r} + 67\mathbf{a}|\mathbf{r}|^2}{593^2} = 569. \]
Final Answer: 569.
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 _______. 