Step 1: Use the relation between power, force, and velocity
Power \(P = F \cdot v = ma \cdot v = m \cdot \frac{dv}{dt} \cdot v\)
Step 2: Rearranging and integrating
\[ P = m v \frac{dv}{dt} \Rightarrow \frac{P}{m} dt = v dv \] \[ \int v dv = \int \frac{P}{m} dt \Rightarrow \frac{v^2}{2} = \frac{P}{m} t + C \Rightarrow v \propto \sqrt{t} \] Step 3: Use \(v = \frac{ds}{dt}\)
\[ \frac{ds}{dt} \propto t^{1/2} \Rightarrow ds \propto t^{1/2} dt \Rightarrow \int ds \propto \int t^{1/2} dt \Rightarrow s \propto t^{3/2} \] Step 4: Identify the exponent \(x\)
So, \(x = \frac{3}{2}\)
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:
