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.
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,