Initial conditions play a crucial role when using Laplace transforms to solve differential equations. They provide the necessary starting values for a function and its derivatives, allowing us to uniquely determine the solution later on. Often, initial conditions are represented as the value of the function and its first few derivatives at time \(t = 0\).
When we apply the Laplace transform to a differential equation, these initial conditions help us transition from the time domain to the s-domain. Using our knowledge from calculus, the Laplace transform of the first derivative \(x'(t)\) is expressed as:
- \(\mathcal{L}\{x'(t)\} = sX(s) - x(0)\)
The equation intuitively shows how the initial condition \(x(0)\) modifies the Laplace transform. For example, in our exercise, \(x(0) = 2\). Thus, when we compute \(\mathcal{L}\{x'(t)\}\), it becomes \(sX(s) - 2\), clearly indicating how the initial value is used.
Similarly, with the second derivative, \(x''(t)\), the Laplace transform is:
- \(\mathcal{L}\{x''(t)\} = s^2X(s) - sx(0) - x'(0)\)
Here, both initial values \(x(0) = 2\) and \(x'(0) = 3\) are involved, demonstrating how important these conditions are to arriving at the correct solution.