Step 1: Velocity equation The velocity of the particle is given as:
\( v = \alpha \sqrt{x}. \)
At \( x = 0 \), the velocity is:
\( v = 0. \)
At \( x = d \), the velocity becomes:
\( v = \alpha \sqrt{d}. \)
Step 2: Work-Energy Theorem The work done by all forces is equal to the change in kinetic energy:
\( W.D = K_f - K_i, \)
where:
\( K = \frac{1}{2} mv^2. \)
Substitute the velocities:
\( W.D = \frac{1}{2} m (\alpha \sqrt{d})^2 - \frac{1}{2} m (0)^2. \)
Simplify:
\( W.D = \frac{1}{2} m (\alpha^2 d) - 0. \)
\( W.D = \frac{m \alpha^2 d}{2}. \)
Final Answer: \( \frac{m \alpha^2 d}{2}. \)
The acceleration of a particle which moves along the positive \( x \)-axis varies with its position as shown in the figure. If the velocity of the particle is \( 0.8 \, \text{m/s} \) at \( x = 0 \), then its velocity at \( x = 1.4 \, \text{m} \) is:
A force of \( (6x^2 - 4x + 3) \, \text{N} \) acts on a body of mass 0.75 kg and displaces it from \( x = 5 \, \text{m} \) to \( x = 2 \, \text{m} \). The work done by the force is
If \[ \frac{dy}{dx} + 2y \sec^2 x = 2 \sec^2 x + 3 \tan x \cdot \sec^2 x \] and
and \( f(0) = \frac{5}{4} \), then the value of \[ 12 \left( y \left( \frac{\pi}{4} \right) - \frac{1}{e^2} \right) \] equals to: