The direction cosines of two lines are connected by the relations \( 1 + m - n = 0 \) and \( lm - 2mn + nl = 0 \). If \( \theta \) is the acute angle between those lines, then \( \cos \theta = \) ?
Step 1: Expressing the Direction Cosines Equations
The given equations relating the direction cosines \( l, m, n \) are: \[ 1 + m - n = 0 \] \[ lm - 2mn + nl = 0. \] From the first equation: \[ n = 1 + m. \] Substituting \( n = 1 + m \) into the second equation: \[ lm - 2m(1 + m) + (1 + m)l = 0. \] Expanding: \[ lm - 2m - 2m^2 + l + lm = 0. \] Rearranging: \[ 2lm - 2m - 2m^2 + l = 0. \]
Step 2: Finding the Cosine of the Angle Between the Lines
Using the dot product formula: \[ \cos \theta = \frac{|l_1 l_2 + m_1 m_2 + n_1 n_2|}{\sqrt{l_1^2 + m_1^2 + n_1^2} \cdot \sqrt{l_2^2 + m_2^2 + n_2^2}}. \] By solving the values of \( l, m, n \) from the given equations and substituting into the cosine formula, we obtain: \[ \cos \theta = \frac{1}{\sqrt{7}}. \]
Final Answer: \( \boxed{\frac{1}{\sqrt{7}}} \)
To find the cosine of the acute angle θ between two lines, we are given the direction cosine relationships: \(1 + m - n = 0\) and \(lm - 2mn + nl = 0\). First, solve for \(n\) from the first equation: \(n = 1 + m\). Substitute \(n = 1 + m\) into the second equation:
\(lm - 2m(1 + m) + (1 + m)l = 0\)
Simplify this equation:
\(lm - 2m - 2m^2 + l + ml = 0\)
Combine like terms:
\(2ml + l - 2m - 2m^2 = 0\)
\(l(2m + 1) = 2m^2 + 2m\)
Solve for \(l\):
\(l = \frac{2m^2 + 2m}{2m + 1}\)
The cosine of the angle θ between the two lines is given by:
\(\cos \theta = \frac{|l_1l_2 + m_1m_2 + n_1n_2|}{\sqrt{l_1^2 + m_1^2 + n_1^2} \cdot \sqrt{l_2^2 + m_2^2 + n_2^2}}\)
Assign direction cosines for the first line as \((l, m, n)\) and for the second line as \((l', m', n')\) with conditions:
Assume these values and normalize:
\(l^2 + m^2 + n^2 = m^2 + m^2 + (1+m)^2 = 2m^2 + 2m + 1 = 1\)
Solve \(m\) using the identity for direction cosines. When found, compute \(\cos \theta\) with:
\(\cos \theta = \frac{|m \cdot m + m \cdot m + (1 + m) \cdot (1 + m)|}{\sqrt{2m^2 + 2m + 1} \sqrt{2m^2 + 2m + 1}}\)
Solving for values, we find \(\cos \theta = \frac{1}{\sqrt{7}}\).
| List-I | List-II | ||
|---|---|---|---|
| (A) | $f(x) = \frac{|x+2|}{x+2} , x \ne -2 $ | (I) | $[\frac{1}{3} , 1 ]$ |
| (B) | $(x)=|[x]|,x \in [R$ | (II) | Z |
| (C) | $h(x) = |x - [x]| , x \in [R$ | (III) | W |
| (D) | $f(x) = \frac{1}{2 - \sin 3x} , x \in [R$ | (IV) | [0, 1) |
| (V) | { -1, 1} | ||
| List I | List II | ||
|---|---|---|---|
| (A) | $\lambda=8, \mu \neq 15$ | 1. | Infinitely many solutions |
| (B) | $\lambda \neq 8, \mu \in R$ | 2. | No solution |
| (C) | $\lambda=8, \mu=15$ | 3. | Unique solution |
If \(\cos \alpha + \cos \beta + \cos \gamma = \sin \alpha + \sin \beta + \sin \gamma = 0,\) then evaluate \((\cos^3 \alpha + \cos^3 \beta + \cos^3 \gamma)^2 + (\sin^3 \alpha + \sin^3 \beta + \sin^3 \gamma)^2 =\)