Step 1: Represent the lines in vector form
The parametric equations of the first line can be written as:
\[ \mathbf{r_1} = \langle -\sqrt{6}, \sqrt{6}, 0 \rangle + t \langle 2, 4, 5 \rangle. \]
The parametric equations of the second line can be written as:
\[ \mathbf{r_2} = \langle \lambda, 2\sqrt{6}, -2\sqrt{6} \rangle + s \langle 3, 4, 5 \rangle. \]
Step 2: Find the direction vector for the shortest distance
The shortest distance between two skew lines is given by the perpendicular distance between the two lines:
\[ d = \frac{|(\mathbf{a_2} - \mathbf{a_1}) \cdot (\mathbf{b_1} \times \mathbf{b_2})|}{|\mathbf{b_1} \times \mathbf{b_2}|}. \]
Here:
\[ \mathbf{a_1} = \langle -\sqrt{6}, \sqrt{6}, 0 \rangle, \quad \mathbf{a_2} = \langle \lambda, 2\sqrt{6}, -2\sqrt{6} \rangle, \] \[ \mathbf{b_1} = \langle 2, 4, 5 \rangle, \quad \mathbf{b_2} = \langle 3, 4, 5 \rangle. \]
Step 3: Compute \( \mathbf{b_1} \times \mathbf{b_2} \)
The cross product is calculated as:
\[ \mathbf{b_1} \times \mathbf{b_2} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 2 & 4 & 5 \\ 3 & 4 & 5 \end{vmatrix} = \langle 0, 5, -4 \rangle. \]
Step 4: Compute \( \mathbf{a_2} - \mathbf{a_1} \)
The difference between the vectors is:
\[ \mathbf{a_2} - \mathbf{a_1} = \langle \lambda + \sqrt{6}, \sqrt{6}, -2\sqrt{6} \rangle. \]
Step 5: Apply the formula for distance
Substitute into the distance formula:
\[ d = \frac{|(\mathbf{a_2} - \mathbf{a_1}) \cdot (\mathbf{b_1} \times \mathbf{b_2})|}{|\mathbf{b_1} \times \mathbf{b_2}|}. \]
The numerator is:
\[ (\mathbf{a_2} - \mathbf{a_1}) \cdot (\mathbf{b_1} \times \mathbf{b_2}) = \langle \lambda + \sqrt{6}, \sqrt{6}, -2\sqrt{6} \rangle \cdot \langle 0, 5, -4 \rangle = 5\sqrt{6} + 8\sqrt{6} = \lambda + 13\sqrt{6}. \]
The denominator is:
\[ |\mathbf{b_1} \times \mathbf{b_2}| = \sqrt{0^2 + 5^2 + (-4)^2} = \sqrt{41}. \]
We are given that \( d = 6 \), so:
\[ \frac{| \lambda + 13\sqrt{6} |}{\sqrt{41}} = 6 \quad \Rightarrow \quad | \lambda + 13\sqrt{6} | = 6\sqrt{41}. \]
Step 6: Solve for \( \lambda \)
We now solve for \( \lambda \) by considering both cases:
\[ \lambda + 13\sqrt{6} = 6\sqrt{41}, \quad \lambda + 13\sqrt{6} = -6\sqrt{41}. \]
Thus, we have two solutions for \( \lambda \):
\[ \lambda = -13\sqrt{6} + 6\sqrt{41}, \quad \lambda = -13\sqrt{6} - 6\sqrt{41}. \]
Step 7: Square the sum of all possible \( \lambda \)
We now compute the square of the sum of the two values of \( \lambda \):
\[ \lambda^2 = (-13\sqrt{6} + 6\sqrt{41})^2 + (-13\sqrt{6} - 6\sqrt{41})^2 = 624. \]
Let \( \alpha = \dfrac{-1 + i\sqrt{3}}{2} \) and \( \beta = \dfrac{-1 - i\sqrt{3}}{2} \), where \( i = \sqrt{-1} \). If
\[ (7 - 7\alpha + 9\beta)^{20} + (9 + 7\alpha - 7\beta)^{20} + (-7 + 9\alpha + 7\beta)^{20} + (14 + 7\alpha + 7\beta)^{20} = m^{10}, \] then the value of \( m \) is ___________.
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,
A Complex Number is written in the form
a + ib
where,
The Complex Number consists of a symbol “i” which satisfies the condition i^2 = −1. Complex Numbers are mentioned as the extension of one-dimensional number lines. In a complex plane, a Complex Number indicated as a + bi is usually represented in the form of the point (a, b). We have to pay attention that a Complex Number with absolutely no real part, such as – i, -5i, etc, is called purely imaginary. Also, a Complex Number with perfectly no imaginary part is known as a real number.