Integration transforms an acceleration function, which describes the rate of change of velocity, into a velocity function. This fundamental calculus process involves computing the antiderivative. Here's how it works in simple terms:
Our acceleration function from the problem is given by:\[a(t) = 3t^2 - 2t\]
Integrating this function with respect to time gives us the velocity function:\[v(t) = \int (3t^2 - 2t) \, dt = t^3 - t^2 + C\]
Here, \(C\) is the constant of integration we find using initial conditions. At time \(t = 0\), velocity \(v(0)\) is 200 m/s, allowing us to solve for \(C\).
- The antiderivative of \(t^2\) is \(t^3/3\), and \(t\) turns into \(t^2/2\), illustrated simply here.
- Apply initial conditions to solve for constants, ensuring the resulting function accurately represents the system's initial state.
Thus, the velocity function translates a potentially complex physics problem into manageable math, providing insights into how a particle's motion evolves over time given its acceleration.