If y(x) is a solution of the differential equation \(\frac{{dy}}{{dx}} + 4xy = {x^3},y(0) = 0\) then \(\mathop {\lim }\limits_{x \to 0} y(x)\) is
0
Solving differential equations is a fundamental topic in calculus. This problem involves finding the limit of the solution \(y(x)\) of a first-order linear differential equation as \(x \to 0\), given an initial condition.
The given differential equation is \(\frac{{dy}}{{dx}} + 4xy = {x^3}\). This is a first-order linear differential equation of the form \(\frac{{dy}}{{dx}} + P(x)y = Q(x)\), where \(P(x) = 4x\) and \(Q(x) = x^3\). To solve this type of differential equation, we first find the integrating factor.
The integrating factor for a first-order linear differential equation is given by \(IF = e^{\int P(x) dx}\).
Here, \(P(x) = 4x\).
\(IF = e^{\int 4x dx} = e^{4 \int x dx} = e^{4 \left(\frac{x^2}{2}\right)} = e^{2x^2}\).
So, the integrating factor is \(e^{2x^2}\). This factor helps us solve the differential equation.
Multiply the entire differential equation by the integrating factor:
\(e^{2x^2} \left( \frac{{dy}}{{dx}} + 4xy \right) = e^{2x^2} x^3\)
The left side is the derivative of \(y \cdot IF\):
\(\frac{d}{dx} (y \cdot e^{2x^2}) = x^3 e^{2x^2}\)
Now, integrate both sides with respect to \(x\):
\(y \cdot e^{2x^2} = \int x^3 e^{2x^2} \, dx + C\)
To evaluate the integral \(\int x^3 e^{2x^2} \, dx\), we use substitution and integration by parts.
Let \(u = 2x^2\). Then \(du = 4x \, dx\), so \(x \, dx = \frac{1}{4} du\). Also, \(x^2 = \frac{u}{2}\).
The integral becomes \(\int x^2 \cdot x e^{2x^2} \, dx = \int \frac{u}{2} e^u \frac{1}{4} du = \frac{1}{8} \int u e^u \, du\).
Using integration by parts (\(\int v \, dw = vw - \int w \, dv\)) with \(v = u\) and \(dw = e^u \, du\), we get \(dv = du\) and \(w = e^u\).
\(\int u e^u \, du = u e^u - \int e^u \, du = u e^u - e^u = e^u(u-1)\).
Substitute back \(u = 2x^2\): \(e^{2x^2}(2x^2 - 1)\).
So, \(\int x^3 e^{2x^2} \, dx = \frac{1}{8} e^{2x^2}(2x^2 - 1)\).
The general solution for the differential equation is:
\(y \cdot e^{2x^2} = \frac{1}{8} e^{2x^2}(2x^2 - 1) + C\)
\(y(x) = \frac{1}{8}(2x^2 - 1) + C e^{-2x^2}\)
This is the general solution involving the constant \(C\). We need to use the initial condition to find the specific solution.
We are given the initial condition \(y(0) = 0\).
Substitute \(x = 0\) and \(y(0) = 0\) into the general solution:
\(y(0) = \frac{1}{8}(2(0)^2 - 1) + C e^{-2(0)^2}\)
\(0 = \frac{1}{8}(0 - 1) + C e^0\)
\(0 = -\frac{1}{8} + C \cdot 1\)
\(C = \frac{1}{8}\)
Substitute the value of \(C\) back into the general solution to get the specific solution of the differential equation:
\(y(x) = \frac{1}{8}(2x^2 - 1) + \frac{1}{8} e^{-2x^2}\)
We need to find \(\mathop {\lim }\limits_{x \to 0} y(x)\) for the specific solution we found.
\(\mathop {\lim }\limits_{x \to 0} y(x) = \mathop {\lim }\limits_{x \to 0} \left( \frac{1}{8}(2x^2 - 1) + \frac{1}{8} e^{-2x^2} \right)\)
We can evaluate the limit of each term separately:
Therefore, the limit is:
\(\mathop {\lim }\limits_{x \to 0} y(x) = -\frac{1}{8} + \frac{1}{8} = 0\)
The limit of the solution \(y(x)\) as \(x\) approaches 0 is 0.
The equation of motion of a one-dimensional forced harmonic oscillator in the presence of a dissipative force is described by \(\frac{{{{\rm{d}}^{\rm{2}}}{\rm{x}}}}{{{\rm{d}}{{\rm{t}}^{\rm{2}}}}}\,{\rm{ + }}\,{\rm{10}}\frac{{{\rm{dx}}}}{{{\rm{dt}}}}\,{\rm{ + }}\,{\rm{16x}}\,{\rm{ = }}\,{\rm{6t}}{{\rm{e}}^{{\rm{ - 8t}}}}{\rm{ + }}\,{\rm{4}}{{\rm{t}}^{\rm{2}}}{{\rm{e}}^{{\rm{ - 2t}}}}\) The general form of the particular solution, in terms of constants A, B etc., is
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