Given that the body moves under the influence of a constant power source, we aim to find the relation between the displacement \( s \) and the time \( t \).
Step 1: Understanding the Relationship Between Power and Velocity
Power \( P \) delivered to the body is constant and is given by:
\[ P = Fv, \]
where:
- \( F \) is the force acting on the body,
- \( v \) is the velocity of the body.
Using Newton’s second law \( F = ma \), where \( m \) is the mass and \( a \) is the acceleration, we have:
\[ P = mav. \]
Since power is constant, we can write:
\[ P = mv \frac{dv}{dt}. \]
Step 2: Integrating the Equation
Rearranging:
\[ P \, dt = mv \, dv. \]
Integrating both sides:
\[ \int P \, dt = \int mv \, dv. \]
This yields:
\[ Pt = \frac{mv^2}{2} \implies v^2 = \frac{2Pt}{m}. \]
Taking the square root:
\[ v = \sqrt{\frac{2Pt}{m}}. \]
Step 3: Finding the Displacement
Velocity is the derivative of displacement with respect to time:
\[ v = \frac{ds}{dt} = \sqrt{\frac{2Pt}{m}}. \]
Rearranging and integrating:
\[ ds = \sqrt{\frac{2P}{m}} \, t^{1/2} \, dt. \]
Integrating both sides:
\[ s \propto t^{3/2}. \]
Therefore, the displacement \( s \) is proportional to \( t^{3/2} \).
A force \( \vec{f} = x^2 \hat{i} + y \hat{j} + y^2 \hat{k} \) acts on a particle in a plane \( x + y = 10 \). The work done by this force during a displacement from \( (0,0) \) to \( (4m, 2m) \) is Joules (round off to the nearest integer).
Which one of the following graphs accurately represents the plot of partial pressure of CS₂ vs its mole fraction in a mixture of acetone and CS₂ at constant temperature?

Let \( \alpha = \dfrac{-1 + i\sqrt{3}}{2} \) and \( \beta = \dfrac{-1 - i\sqrt{3}}{2} \), where \( i = \sqrt{-1} \). If
\[ (7 - 7\alpha + 9\beta)^{20} + (9 + 7\alpha - 7\beta)^{20} + (-7 + 9\alpha + 7\beta)^{20} + (14 + 7\alpha + 7\beta)^{20} = m^{10}, \] then the value of \( m \) is ___________.