Let $ \vec{a} = \hat{i} + 2\hat{j} + \hat{k} $, $ \vec{b} = 3\hat{i} - 3\hat{j} + 3\hat{k} $, $ \vec{c} = 2\hat{i} - \hat{j} + 2\hat{k} $ and $ \vec{d} $ be a vector such that $ \vec{b} \times \vec{d} = \vec{c} \times \vec{d} $ and $ \vec{a} \cdot \vec{d} = 4 $. Then $ |\vec{a} \times \vec{d}|^2 $ is equal to _______
The problem asks for the value of \(|\vec{a} \times \vec{d}|^2\), given the vectors \(\vec{a}\), \(\vec{b}\), \(\vec{c}\) and two conditions that define the vector \(\vec{d}\).
This problem utilizes several fundamental properties of vector algebra:
Step 1: Simplify the first condition involving vector \(\vec{d}\).
The first condition is \(\vec{b} \times \vec{d} = \vec{c} \times \vec{d}\). We can rearrange this equation:
\[ \vec{b} \times \vec{d} - \vec{c} \times \vec{d} = \vec{0} \]Using the distributive property of the cross product:
\[ (\vec{b} - \vec{c}) \times \vec{d} = \vec{0} \]This implies that the vector \(\vec{d}\) is parallel to the vector \((\vec{b} - \vec{c})\). Therefore, \(\vec{d}\) can be written as a scalar multiple of \((\vec{b} - \vec{c})\).
\[ \vec{d} = \lambda (\vec{b} - \vec{c}) \quad \text{for some scalar } \lambda \]Step 2: Calculate the vector \((\vec{b} - \vec{c})\).
Given \(\vec{b} = 3\hat{i} - 3\hat{j} + 3\hat{k}\) and \(\vec{c} = 2\hat{i} - \hat{j} + 2\hat{k}\):
\[ \vec{b} - \vec{c} = (3 - 2)\hat{i} + (-3 - (-1))\hat{j} + (3 - 2)\hat{k} \] \[ \vec{b} - \vec{c} = 1\hat{i} - 2\hat{j} + 1\hat{k} \]Step 3: Use the second condition to find the scalar \(\lambda\).
We now have \(\vec{d} = \lambda (\hat{i} - 2\hat{j} + \hat{k})\). The second condition is \(\vec{a} \cdot \vec{d} = 4\). We are given \(\vec{a} = \hat{i} + 2\hat{j} + \hat{k}\).
\[ \vec{a} \cdot \vec{d} = (\hat{i} + 2\hat{j} + \hat{k}) \cdot (\lambda\hat{i} - 2\lambda\hat{j} + \lambda\hat{k}) = 4 \] \[ (1)(\lambda) + (2)(-2\lambda) + (1)(\lambda) = 4 \] \[ \lambda - 4\lambda + \lambda = 4 \] \[ -2\lambda = 4 \implies \lambda = -2 \]Step 4: Determine the vector \(\vec{d}\).
Substitute the value of \(\lambda = -2\) back into the expression for \(\vec{d}\):
\[ \vec{d} = -2(\hat{i} - 2\hat{j} + \hat{k}) = -2\hat{i} + 4\hat{j} - 2\hat{k} \]Step 5: Calculate the cross product \(\vec{a} \times \vec{d}\).
\[ \vec{a} \times \vec{d} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 1 & 2 & 1 \\ -2 & 4 & -2 \end{vmatrix} \] \[ = \hat{i}((2)(-2) - (1)(4)) - \hat{j}((1)(-2) - (1)(-2)) + \hat{k}((1)(4) - (2)(-2)) \] \[ = \hat{i}(-4 - 4) - \hat{j}(-2 + 2) + \hat{k}(4 + 4) \] \[ = -8\hat{i} - 0\hat{j} + 8\hat{k} = -8\hat{i} + 8\hat{k} \]Step 6: Calculate the final value \(|\vec{a} \times \vec{d}|^2\).
The squared magnitude of the vector \(-8\hat{i} + 8\hat{k}\) is:
\[ |\vec{a} \times \vec{d}|^2 = (-8)^2 + (0)^2 + (8)^2 \] \[ = 64 + 0 + 64 = 128 \]The value of \(|\vec{a} \times \vec{d}|^2\) is 128.
Given
\( \vec{b} \times \vec{d} = \vec{c} \times \vec{d} \).
\( \vec{b} \times \vec{d} - \vec{c} \times \vec{d} = \vec{0} \)
\( (\vec{b} - \vec{c}) \times \vec{d} = \vec{0} \)
This implies that \( \vec{d} \) is parallel to \( \vec{b} - \vec{c} \).
\( \vec{b} - \vec{c} = (3\hat{i} - 3\hat{j} + 3\hat{k}) - (2\hat{i} - \hat{j} + 2\hat{k}) = (3 - 2)\hat{i} + (-3 - (-1))\hat{j} + (3 - 2)\hat{k} = \hat{i} - 2\hat{j} + \hat{k} \)
So, \( \vec{d} = \lambda (\vec{b} - \vec{c}) = \lambda (\hat{i} - 2\hat{j} + \hat{k}) \)
for some scalar \( \lambda \). Given \( \vec{a} \cdot \vec{d} = 4 \).
\( (\hat{i} + 2\hat{j} + \hat{k}) \cdot (\lambda (\hat{i} - 2\hat{j} + \hat{k})) = 4 \)
\( \lambda ((\hat{i} + 2\hat{j} + \hat{k}) \cdot (\hat{i} - 2\hat{j} + \hat{k})) = 4 \)
\( \lambda (1(1) + 2(-2) + 1(1)) = 4 \) \( \lambda (1 - 4 + 1) = 4 \) \( \lambda (-2) = 4 \) \( \lambda = -2 \)
Now we can find \( \vec{d} \): \( \vec{d} = -2 (\hat{i} - 2\hat{j} + \hat{k}) = -2\hat{i} + 4\hat{j} - 2\hat{k} \)
We need to find \( |\vec{a} \times \vec{d}|^2 \). First, calculate \( \vec{a} \times \vec{d} \): \[ \vec{a} \times \vec{d} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} 1 & 2 & 1 -2 & 4 & -2 \end{vmatrix} = \hat{i}(2(-2) - 1(4)) - \hat{j}(1(-2) - 1(-2)) + \hat{k}(1(4) - 2(-2)) \] \[ \vec{a} \times \vec{d} = \hat{i}(-4 - 4) - \hat{j}(-2 + 2) + \hat{k}(4 + 4) = -8\hat{i} - 0\hat{j} + 8\hat{k} = -8\hat{i} + 8\hat{k} \] Now, find the magnitude squared: \[ |\vec{a} \times \vec{d}|^2 = (-8)^2 + (0)^2 + (8)^2 = 64 + 0 + 64 = 128 \]
Alternatively, using the identity \( |\vec{a} \times \vec{d}|^2 + (\vec{a} \cdot \vec{d})^2 = |\vec{a}|^2 |\vec{d}|^2 \):
\( |\vec{a}|^2 = 1^2 + 2^2 + 1^2 = 1 + 4 + 1 = 6 \) \( |\vec{d}|^2 = (-2)^2 + (4)^2 + (-2)^2 = 4 + 16 + 4 = 24 \) \( (\vec{a} \cdot \vec{d})^2 = (4)^2 = 16 \) \( |\vec{a} \times \vec{d}|^2 = |\vec{a}|^2 |\vec{d}|^2 - (\vec{a} \cdot \vec{d})^2 = 6 \times 24 - 16 = 144 - 16 = 128 \)
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,