To solve the problem, let's consider the given conditions regarding the angles a line makes with the axes. Denoting large capital angles: \( \alpha \) with the x-axis, \( \beta \) with the y-axis, and \( \gamma \) with the z-axis.
According to the problem statement:
The direction cosines of the line with respect to the x-, y-, and z-axes are given by:
According to the identity involving direction cosines, we have:
\(\cos^2 \alpha + \cos^2 \beta + \cos^2 \gamma = 1\)Substitute the known relations into the equation:
This simplifies to:
\(\cos^2 \alpha + 2 \cos^2 \frac{\alpha}{2} = 1\)Using the double angle identity: \( \cos^2 \frac{\alpha}{2} = \frac{1 + \cos \alpha}{2} \), we substitute and get:
\(\cos^2 \alpha + 2 \times \frac{1 + \cos \alpha}{2} = 1\)This further simplifies to:
\(\cos^2 \alpha + 1 + \cos \alpha = 1\)Or, reorganizing terms:
\(\cos^2 \alpha + \cos \alpha = 0\)Factor the quadratic equation:
\(\cos \alpha (\cos \alpha + 1) = 0\)This gives us two solutions:
Substituting back, we find the possible values of \( \beta \):
The sum of all possible values of \( \beta \) is then:
\(\frac{\pi}{4} + \frac{\pi}{2} = \frac{3\pi}{4}\)Therefore, the sum of all possible values of the angle \( \beta \) is \(\frac{3\pi}{4}\).
Let the angle with the positive x-axis be \( \alpha \).
\(\text{Given, } \beta = \frac{\alpha}{2} \text{ and } \gamma = \frac{\alpha}{2}. \)
\(\text{We know that } \cos^2 \alpha + \cos^2 \beta + \cos^2 \gamma = 1. \)
\(\text{Substituting the values of } \beta \text{ and } \gamma: \)
\(\cos^2 \alpha + \cos^2 \left( \frac{\alpha}{2} \right) + \cos^2 \left( \frac{\alpha}{2} \right) = 1 \)
\(\Rightarrow \cos^2 \alpha + 2 \cos^2 \left( \frac{\alpha}{2} \right) = 1 \)
\(\text{Using the identity } \cos \alpha = 2 \cos^2 \left( \frac{\alpha}{2} \right) - 1, \text{ we get } \)
\(2 \cos^2 \left( \frac{\alpha}{2} \right) = \cos \alpha + 1 \)
\(\text{So,} \)
\(\cos^2 \alpha + \cos \alpha + 1 = 1 \)
\(\Rightarrow \cos^2 \alpha + \cos \alpha = 0 \)
\(\Rightarrow \cos \alpha (\cos \alpha + 1) = 0 \)
\(\text{This gives } \cos \alpha = 0 \text{ or } \cos \alpha = -1. \)
Case 1:
\(\cos \alpha = 0 \)
\(\Rightarrow \alpha = \frac{\pi}{2} \text{ or } \alpha = \frac{3\pi}{2} \)
\(\text{Since the angles are with the positive axes, } 0 \le \alpha, \beta, \gamma \le \pi. \)
\(\text{If } \alpha = \frac{\pi}{2}, \text{ then } \beta = \frac{\pi}{4} \)
\(\text{If } \alpha = \frac{3\pi}{2}, \text{ this is not possible as } \beta = \frac{3\pi}{4} \text{ and } \gamma = \frac{3\pi}{4}, \)
\(\text{leading to } \cos^2 \alpha + \cos^2 \beta + \cos^2 \gamma = 0 + \frac{1}{2} + \frac{1}{2} = 1. \)
Case 2:
\(\cos \alpha = -1 \)
\(\Rightarrow \alpha = \pi \)
\(\Rightarrow \beta = \frac{\pi}{2}, \quad \gamma = \frac{\pi}{2} \)
\(\Rightarrow \cos^2 \pi + \cos^2 \frac{\pi}{2} + \cos^2 \frac{\pi}{2} = 1 + 0 + 0 = 1 \)
\(\text{Possible values of } \beta \text{ are } \frac{\pi}{4} \text{ and } \frac{\pi}{2}. \)
\(\text{Sum of possible values of } \beta = \frac{\pi}{4} + \frac{\pi}{2} = \frac{3\pi}{4}. \)
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,