To solve this problem, we need to determine the distance between two cars when they come to rest after braking. Let's break it down step by step:
We use the kinematic equation for constant acceleration:
\(v^2 = u^2 + 2as\)
Apply the equation separately for each car:
The combined distance covered by both cars is \(100 \, \text{m} + 100 \, \text{m} = 200 \, \text{m}\). Since the initial distance between the cars was \(300 \, \text{m}\), the distance remaining between the two cars when they stop is:
\(300 \, \text{m} - 200 \, \text{m} = 100 \, \text{m}\)
Therefore, the distance between the cars when they come to rest is 100 m.
Let the distance between the cars when they come to rest be \( d \). Each car has an initial speed of 20 m/s. The deceleration \( a \) is \(-2 \, \text{m/s}^2\).
Using the equation of motion:
\( v^2 = u^2 + 2ad, \)
where \( v = 0 \) (final speed), \( u = 20 \, \text{m/s} \) (initial speed), and \( a = -2 \, \text{m/s}^2 \), we get:
\( 0 = 20^2 + 2(-2)d \quad \Rightarrow \quad 0 = 400 - 4d \quad \Rightarrow \quad d = 100 \, \text{m}. \)
Since the two cars are moving towards each other, the total distance covered by both cars is \( 100 + 100 = 200 \, \text{m} \), so the distance between them when they come to rest is 100 m.
Let one focus of the hyperbola \( H : \dfrac{x^2}{a^2} - \dfrac{y^2}{b^2} = 1 \) be at \( (\sqrt{10}, 0) \) and the corresponding directrix be \( x = \dfrac{9}{\sqrt{10}} \). If \( e \) and \( l \) respectively are the eccentricity and the length of the latus rectum of \( H \), then \( 9 \left(e^2 + l \right) \) is equal to:
