Problem 32
Question
The differential equation \(d y / d x=y^{\prime} / x^{\prime}=\left(x^{2}-2 x\right) / y\) can be solved by separating variables. It follows that \(y^{2} / 2=\left(x^{3} / 3\right)-x^{2}+c\) and \(\operatorname{since} \mathbf{X}(0)=\left(x(0), x^{\prime}(0)\right)=(1,0), c=\frac{2}{3} .\) Therefore The differential equation \(d y / d x=y^{\prime} / x^{\prime}=\left(x^{2}-2 x\right) / y\) can be solved by separating variables. It follows that \(y^{2} / 2=\left(x^{3} / 3\right)-x^{2}+c\) and \(\operatorname{since} \mathbf{X}(0)=\left(x(0), x^{\prime}(0)\right)=(1,0), c=\frac{2}{3} .\) Therefore $$\frac{y^{2}}{2}=\frac{x^{3}-3 x^{2}+2}{3}=\frac{(x-1)\left(x^{2}-2 x-2\right)}{3}$$ But \((x-1)\left(x^{2}-2 x-2\right)>0\) for \(1-\sqrt{3} < x < 1\) and so each \(x\) in this interval has 2 corresponding values of \(y\) therefore \(\mathbf{X}(t)\) is a periodic solution.
Step-by-Step Solution
VerifiedKey Concepts
Separation of Variables
This rearrangement allows us to integrate each side independently. Essentially, we are treating the derivatives as if they are fractions that can be separated and recombined after integration. This simplification is the key advantage of this method. After separating the variables, the next step is to integrate both sides, but each with respect to their corresponding variables. This process results in a more manageable form that we can solve to find the function \( y(x) \).
Constant of Integration
For the exercise, after integrating \( y \, dy = (x^2 - 2x) \, dx \), we get \( \frac{y^2}{2} = \frac{x^3}{3} - x^2 + C \). Here, \( C \) is the constant of integration.
The value of \( C \) is determined using initial conditions. In this case, we used the initial condition \( x(0) = 1 \) and \( y(0) = 0 \) which lead us to finding \( C = \frac{2}{3} \). Initial conditions are essential because they allow us to determine this constant, which then gives us a particular solution to the differential equation, rather than a family of solutions.
Periodic Solutions
In this problem, after solving and simplifying the integrated equation, we analyze that the solution for \( x \) in the interval \( 1 - \sqrt{3} < x < 1 \), shows this behavior. During this phase, the function literally repeats itself, making it a periodic solution.
Periodic solutions are often used in modeling real-world phenomena that are cycles, such as waves, vibrations, or other repetitive patterns, making them an important aspect to understand in the study of differential equations.