적분법에 의한 속도와 위치

Velocity is found by integrating the acceleration function with respect to time. Since acceleration is the time derivative of velocity, taking the integral reverses this relationship. The integration produces a constant of integration, which is determined using initial conditions—the velocity at a known time. Substituting this constant yields the velocity as a function of time.

Initial conditions specify the state of motion at a known time, typically t = 0. They allow you to calculate the integration constant that appears when integrating acceleration or velocity. Without initial conditions, the integration constant remains unknown, and you cannot obtain a specific equation for velocity or position. These constants are essential for converting general integral solutions into the first and second kinematic equations.

Position is found by integrating the velocity function with respect to time. Since velocity is the time derivative of position, integration reverses this relationship and yields position as a function of time. An integration constant appears in this process and is determined from initial position conditions. This procedure produces the second kinematic equation for position.

The integral method derives kinematic equations from first principles using calculus. By integrating acceleration, you obtain the first kinematic equation for velocity. By integrating that velocity expression, you obtain the second kinematic equation for position. For constant acceleration, these integral results match the standard kinematic equations used in kinematics problem solving.

The integration constant is an unknown value that appears when integrating acceleration or velocity. It represents the offset or reference value needed to match the physical situation. For velocity integration, it equals the initial velocity. For position integration, it equals the initial position. Applying initial conditions allows you to calculate this constant and obtain specific equations for the motion.

Yes, the integral method works for any acceleration function, whether constant or time-dependent. You integrate the given acceleration function to find velocity, then integrate the resulting velocity function to find position. Each integration introduces a constant determined by initial conditions. This approach is more general than the standard kinematic equations, which assume constant acceleration.

The motorboat example shows how to apply integration to a real scenario where acceleration varies with time: a = −1/4·t m/s². Integrating this acceleration function and applying the initial velocity of 5.0 m/s yields the velocity function. Integrating the velocity function and applying the initial position yields the position function. This demonstrates how the integral method handles time-dependent acceleration.