To analyze the situation, let's apply the basic principles of physics, specifically concepts from kinematics and dynamics.
When a constant force is exerted on an object, the acceleration of that object can be determined using Newton's second law, \( F = ma \). The acceleration \( a \) will depend on the force applied \( F \) and the mass \( m \) of the cart.
Experiment 1: Cart at Rest
- Initially, the cart is at rest, so its initial speed \( u = 0 \).
- After a short time \( t \), the force \( F \) results in an acceleration \( a \), which increases the velocity of the cart. Given constant acceleration, the final speed \( v \) can be expressed as: \[ v = u + at = 0 + at = at \] This increase in speed is directly dependent on the force applied and the mass of the cart.
Experiment 2: Cart Already in Motion
- Now the cart is already moving with some initial speed \( u \) in the direction of the force.
- When we apply the same force \( F \) for the same time interval \( t \), we still get the same acceleration \( a \): \[ a = \frac{F}{m} \]
- The final speed in this scenario, considering the initial speed, is given by: \[ v = u + at \] Here, the increase in speed \( \Delta v \) is: \[ \Delta v = at \]
In both scenarios, the increase in speed \( \Delta v \) under the influence of the same constant force and the same time interval is the same, which corresponds to \( at \).
Conclusion:
Thus, the increase in the cart's speed when starting from rest is the same as the increase in speed when starting from an initial velocity.
The answer is:
- is the same as when it started from rest.