Acceleration (\( a \)) is the rate of change of velocity with respect to time, which can be expressed as:
\[ a = \frac{dv}{dt} = \frac{dv}{dx} \cdot \frac{dx}{dt} = v \cdot \frac{dv}{dx}. \]
Given \( v = 10 \sqrt{x} \), differentiate \( v \) with respect to \( x \):
\[ \frac{dv}{dx} = \frac{d}{dx} (10 \sqrt{x}) = 10 \cdot \frac{1}{2 \sqrt{x}} = \frac{5}{\sqrt{x}}. \]
Now substitute \( v = 10 \sqrt{x} \) and \( \frac{dv}{dx} = \frac{5}{\sqrt{x}} \) into the formula for acceleration:
\[ a = v \cdot \frac{dv}{dx} = 10 \sqrt{x} \cdot \frac{5}{\sqrt{x}} = 50 \, \text{m/s}^2. \]
Using Newton’s second law, the force (\( F \)) is given by:
\[ F = m \cdot a. \]
Substitute \( m = 0.5 \, \text{kg} \) and \( a = 50 \, \text{m/s}^2 \):
\[ F = 0.5 \cdot 50 = 25 \, \text{N}. \]
The force acting on the body is \( 25 \, \text{N} \).
The motion of an airplane is represented by the velocity-time graph as shown below. The distance covered by the airplane in the first 30.5 seconds is km.



For the circuit shown above, the equivalent gate is:
Let \( f : \mathbb{R} \to \mathbb{R} \) be a twice differentiable function such that \[ (\sin x \cos y)(f(2x + 2y) - f(2x - 2y)) = (\cos x \sin y)(f(2x + 2y) + f(2x - 2y)), \] for all \( x, y \in \mathbb{R}. \)
If \( f'(0) = \frac{1}{2} \), then the value of \( 24f''\left( \frac{5\pi}{3} \right) \) is: