Given the parabola:
\[ y^2 = 12x \]
The length of a focal chord is given by:
\[ \text{Length of focal chord} = 4a \csc^2 \theta = 15 \]
For this parabola, \(4a = 12\), so: \[ 12 \csc^2 \theta = 15 \]
Solving for \(\csc^2 \theta\):
\[ \csc^2 \theta = \frac{15}{12} = \frac{5}{4} \]
Thus: \[ \sin^2 \theta = \frac{4}{5} \]
Using the trigonometric identity \(\tan^2 \theta = \frac{\sin^2 \theta}{1 - \sin^2 \theta}\):
\[ \tan^2 \theta = \frac{\frac{4}{5}}{1 - \frac{4}{5}} = 4 \implies \tan \theta = 2 \]
The slope of the focal chord PQ is \(\tan \theta = 2\).
The equation of the chord passing through the focus \((3, 0)\) is given by: \[ y - 0 = 2(x - 3) \]
Simplifying: \[ y = 2x - 6 \implies 2x - y - 6 = 0 \]
To find the perpendicular distance of this line from the origin \((0, 0)\), use the formula:
\[ p = \frac{|2 \times 0 - 0 - 6|}{\sqrt{2^2 + (-1)^2}} = \frac{6}{\sqrt{5}} \]
Calculating \(10p^2\):
\[ 10p^2 = 10 \left(\frac{6}{\sqrt{5}}\right)^2 = 10 \times \frac{36}{5} = 72 \]
A body of mass 1000 kg is moving horizontally with a velocity of 6 m/s. If 200 kg extra mass is added, the final velocity (in m/s) is: