MHB Differential Equations (particular solutions)

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The discussion focuses on finding particular solutions for the differential equation Y'' + 16Y = f(x) with various forms of f(x). For f(x) = 2x^2e^(3x), the particular solution is given as y_p(x) = e^(3x)(ax^2 + bx + c). For f(x) = cos(2x), the solution takes the form y_p(x) = a cos(2x) + b sin(2x). Lastly, for f(x) = 5x cos(3x), the solution is y_p(x) = (ax + b) cos(3x) + (cx + d) sin(3x). The discussion emphasizes the importance of the characteristic roots and the annihilator method in determining these particular solutions.
Fernando Revilla
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I quote a question from Yahoo! Answers

Differential Equations help: Given Y'' + 16Y = f(x)?
1. If f(x) = 2x^2*e^(3x), give the form of Yp.
2. If f(x) = cos(2x) ,give the form of Yp.
3. If f(x) = 5x*cos(3x), give the form of Yp

I have given a link to the topic there so the OP can see my response.
 
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According to a well known theorem if $$y^{(n)}+a_{n-1}y^{(n-1)}+\ldots+a_1y'+a_0y=f(x)\;(E)$$ with $f(x)=e^{\alpha x}\left(P_k(x)\cos \beta x+Q_r(x)\sin \beta x\right)$, a particular solution of $(E)$ has the form: $$y_p(x)=x^se^{\alpha x}\left(\tilde{P_d}(x)\cos \beta x+\tilde{Q_d}(x)\sin \beta x\right)$$ where $(i)$ $\tilde{P_d},\tilde{Q_d}$ are polynomials of degree $d=\max \left\{{k,r}\right\}$. $(ii)$ $s$ is the order of $\alpha +\beta i$ as a root of the characteristic equation $\lambda^n+a_{n-1}\lambda^{n-1}+\ldots+a_1\lambda+a_0=0$. In our case, $\lambda^2+16=0\Leftrightarrow \alpha+\beta i=\pm4i$. So,

1. If $f(x)=2x^2e^{3x}$, then $y_p(x)=e^{3x}(ax^2+bx+c)$.

2. If $f(x)=\cos 2x$, then $y_p(x)=a\cos 2x+b\sin 2x$.

3. If $f(x)=5x\cos 3x$, then $y_p(x)=(ax+b)\cos \color{red}3x+(cx+d)\sin \color{red}3x$.
 
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One may also employ the annihilator method to determine the forms of the particular solutions.

1.) $$f(x)=2x^2e^{3x}$$

If we observe that the differential operator $A$ defined as:

$$A\equiv(D-3)^3$$

annihilates $f(x)$, then we know the particular solution, with the characteristic root $r=3$ of multiplicity 3, must have the form:

$$y_p(x)=c_1e^{3x}+c_2xe^{3x}+c_3x^2e^{3x}=\left(c_1+c_2x+c_3x^2 \right)e^{3x}$$

2.) $$f(x)=\cos(2x)$$

If we observe that the differential operator $A$ defined as:

$$A\equiv D^2+4$$

annihilates $f(x)$, then we know the particular solution, with the characteristic roots $r=\pm2i$, must have the form:

$$y_p(x)=c_1\cos(2x)+c_2\sin(2x)$$

3.) $$f(x)=5x\cos(3x)$$

If we observe that the differential operator $A$ defined as:

$$A\equiv(D^2+9)^2$$

annihilates $f(x)$, then we know the particular solution, with the characteristic roots $r=\pm3i$, both of multiplicity 2, must have the form:

$$y_p(x)=\left(c_1+c_2x \right)\cos(3x)+\left(c_3+c_4x \right)\sin(3x)$$

In all 3 cases, we see that the characteristic roots of the differential operator are different from those of the associated homogeneous equation.
 
Insights auto threads is broken atm, so I'm manually creating these for new Insight articles. In Dirac’s Principles of Quantum Mechanics published in 1930 he introduced a “convenient notation” he referred to as a “delta function” which he treated as a continuum analog to the discrete Kronecker delta. The Kronecker delta is simply the indexed components of the identity operator in matrix algebra Source: https://www.physicsforums.com/insights/what-exactly-is-diracs-delta-function/ by...

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