To find the general solution to the differential equation xdydx = 4y + x3 + x, we can begin by rearranging the terms and separating the variables.
First, we rewrite the equation:
xdydx - 4y = x3 + x.
This can be reorganized as:
xdydx = 4y + x3 + x.
Next, we divide both sides by x (assuming x ≠ 0) to make it easier to work with:
dydx = (4y/x) + x2 + 1.
This form shows that it’s a first-order linear differential equation. We can express it as:
dydx - (4/x)y = x2 + 1.
Now, we can identify the integrating factor μ(x), which is given by:
μ(x) = exp(∫ -4/x \, dx) = exp(-4 ln|x|) = |x|^{-4}.
Next, we multiply through by the integrating factor:
|x|^{-4}dydx - 4|x|^{-5}y = |x|^{-4}(x2 + 1).
After simplifying, we find:
(|x|^{-4}y)' = |x|^{-4}(x2 + 1).
Now, we can integrate both sides:
∫ (|x|^{-4}y)' dx = ∫ |x|^{-4}(x2 + 1) dx.
Calculating the right side, we can break it into two separate integrals:
∫ |x|^{-4}(x2) dx + ∫ |x|^{-4} dx.
Using the power rule, we have:
y|-3/x^3 + C - (1/3) |x|^{-3} + C_1
Where C is the constant of integration. Thus:
y = -rac{3C}{x^3} - rac{1}{3x^2} + C_1x4.
Therefore, the final general solution to the differential equation is:
y = -rac{3}{x^3} + C_1x4 + C
where C is an arbitrary constant. This solution is applicable for x > 0 and x < 0.