\( \frac{3 - \sqrt{3}}{1 + 3\sqrt{3}}, \frac{3 + \sqrt{3}}{1 - 3\sqrt{3}} \)
To find the possible slopes of lines that make a 60° angle with the given line, we follow these steps:
1. Determine Original Slope:
Given line equation: $y - 3x + 18 = 0$
Convert to slope-intercept form:
$y = 3x - 18$ → Slope $m_1 = 3$
2. Angle Between Lines Formula:
For two lines with slopes $m_1$ and $m_2$ making angle θ:
$\tanθ = \left|\frac{m_1 - m_2}{1 + m_1m_2}\right|$
Given θ = 60° and $\tan60° = \sqrt{3}$:
$\sqrt{3} = \left|\frac{3 - m_2}{1 + 3m_2}\right|$
3. Solve for Possible Slopes:
This absolute value equation gives two cases:
Case 1:
$\sqrt{3} = \frac{3 - m_2}{1 + 3m_2}$
Solving yields:
$m_2 = \frac{3 - \sqrt{3}}{1 + 3\sqrt{3}}$
Case 2:
$\sqrt{3} = -\frac{3 - m_2}{1 + 3m_2}$
Solving yields:
$m_2 = \frac{3 + \sqrt{3}}{1 - 3\sqrt{3}}$
Final Answer:
The possible slopes are:
$m_2 = \frac{3 - \sqrt{3}}{1 + 3\sqrt{3}}$ and $\frac{3 + \sqrt{3}}{1 - 3\sqrt{3}}$
To find the slope of lines making an angle of \(60^\circ\) with the given line \(y - 3x + 18 = 0\), we start by identifying the slope \(m_1\) of the given line. By rewriting the equation in the form \(y = mx + c\), we get:
\(y = 3x - 18\)
Thus, the slope \(m_1\) of this line is 3.
We know the formula for the tangent of the angle \(\theta\) between two lines with slopes \(m_1\) and \(m_2\):
\(\tan\theta = \left|\frac{m_2 - m_1}{1 + m_1m_2}\right|\)
Given \(\theta = 60^\circ\), we have \(\tan 60^\circ = \sqrt{3}\). Therefore:
\(\sqrt{3} = \left|\frac{m_2 - 3}{1 + 3m_2}\right|\)
This equation splits into two cases:
Case 1:
\(\frac{m_2 - 3}{1 + 3m_2} = \sqrt{3}\)
Cross-multiplying:
\(m_2 - 3 = \sqrt{3}(1 + 3m_2)\)
\(m_2 - 3 = \sqrt{3} + 3\sqrt{3}m_2\)
Rearranging gives:
\(m_2 - 3\sqrt{3}m_2 = 3 + \sqrt{3}\)
\(m_2(1 - 3\sqrt{3}) = 3 + \sqrt{3}\)
\(m_2 = \frac{3 + \sqrt{3}}{1 - 3\sqrt{3}}\)
Case 2:
\(\frac{m_2 - 3}{1 + 3m_2} = -\sqrt{3}\)
Cross-multiplying:
\(m_2 - 3 = -\sqrt{3}(1 + 3m_2)\)
\(m_2 - 3 = -\sqrt{3} - 3\sqrt{3}m_2\)
Rearranging gives:
\(m_2 + 3\sqrt{3}m_2 = -\sqrt{3} + 3\)
\(m_2(1 + 3\sqrt{3}) = 3 - \sqrt{3}\)
\(m_2 = \frac{3 - \sqrt{3}}{1 + 3\sqrt{3}}\)
Thus, the possible slopes of the lines that make an angle of \(60^\circ\) with the line \(y - 3x + 18 = 0\) are:
\(m_2 = \frac{3 - \sqrt{3}}{1 + 3\sqrt{3}}, \quad m_2 = \frac{3 + \sqrt{3}}{1 - 3\sqrt{3}}\)
Let \( F_1, F_2 \) \(\text{ be the foci of the hyperbola}\) \[ \frac{x^2}{a^2} - \frac{y^2}{b^2} = 1, a > 0, \, b > 0, \] and let \( O \) be the origin. Let \( M \) be an arbitrary point on curve \( C \) and above the X-axis and \( H \) be a point on \( MF_1 \) such that \( MF_2 \perp F_1 F_2, \, M F_1 \perp OH, \, |OH| = \lambda |O F_2| \) with \( \lambda \in (2/5, 3/5) \), then the range of the eccentricity \( e \) is in:
Let the line $\frac{x}{4} + \frac{y}{2} = 1$ meet the x-axis and y-axis at A and B, respectively. M is the midpoint of side AB, and M' is the image of the point M across the line $x + y = 1$. Let the point P lie on the line $x + y = 1$ such that $\Delta ABP$ is an isosceles triangle with $AP = BP$. Then the distance between M' and P is:
A solid cylinder of mass 2 kg and radius 0.2 m is rotating about its own axis without friction with angular velocity 5 rad/s. A particle of mass 1 kg moving with a velocity of 5 m/s strikes the cylinder and sticks to it as shown in figure.
The angular velocity of the system after the particle sticks to it will be: