Assuming a constant power source influences the body's motion, the objective is to determine the relationship between displacement \( s \) and time \( t \).
Step 1: Power and Velocity Relationship
The constant power \( P \) supplied to the body is defined as:
\[ P = Fv, \]
where:
- \( F \) denotes the force acting on the body,
- \( v \) represents the body's velocity.
Applying Newton's second law, \( F = ma \) (where \( m \) is mass and \( a \) is acceleration), we get:
\[ P = mav. \]
Given that power is constant:
\[ P = mv \frac{dv}{dt}. \]
Step 2: Equation Integration
The equation is rearranged as:
\[ P \, dt = mv \, dv. \]
Integrating both sides yields:
\[ \int P \, dt = \int mv \, dv. \]
The result of the integration is:
\[ Pt = \frac{mv^2}{2} \implies v^2 = \frac{2Pt}{m}. \]
Taking the square root gives the velocity:
\[ v = \sqrt{\frac{2Pt}{m}}. \]
Step 3: Displacement Calculation
Velocity is defined as the rate of change 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 leads to:
\[ s \propto t^{3/2}. \]
Consequently, displacement \( s \) is directly 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).