We are given the force as a function of time and need to calculate the velocity and power of the object:
The force acting on the object is given by:
\(\vec{F} = 2t \hat{i} + 3 t^2 \hat{j}\)
According to Newton's second law, the force is related to the rate of change of velocity:
\(m \frac{d \vec{v}}{dt} = 2 t \hat{i} + 3 t^2 \hat{j}\)
Where: - \( m = 1 \, \text{kg} \) (mass of the object), - \( \vec{v} \) is the velocity of the object, - \( t \) is time.
We now integrate the equation with respect to time to find the velocity. The equation becomes:
\(\int\limits^{\hat{v}}_0 d \vec{v} = \int\limits^t_0 (2t \hat{i} + 3 t^2 \hat{j}) \, dt\)
Performing the integration, we get:
\(\vec{v} = t^2 \hat{i} + t^3 \hat{j}\)
This gives the velocity of the object as a function of time:
\(\vec{v} = t^2 \hat{i} + t^3 \hat{j}\)
The power \( P \) delivered by the force is the dot product of the force and velocity vectors:
\(P = \vec{F} \cdot \vec{v}\)
Substitute the expressions for \( \vec{F} \) and \( \vec{v} \):
\(P = (2 t \hat{i} + 3 t^2 \hat{j}) \cdot (t^2 \hat{i} + t^3 \hat{j})\)
Now compute the dot product:
\(P = (2 t^3 + 3 t^5) \, \text{W}\)
The power delivered by the force as a function of time is:
\(P = 2 t^3 + 3 t^5 \, \text{W}\)
In a Vernier caliper, \(N+1\) divisions of vernier scale coincide with \(N\) divisions of main scale. If 1 MSD represents 0.1 mm, the vernier constant (in cm) is: