Comprehensive Guide to Ordinary Differential Equations: Complementary Functions and Particular Integrals

General Theory of Linear Differential Equations

  • Standard Form of Linear Differential Equations:

    • An nn-th order linear ordinary differential equation with constant coefficients has the general form:     f(D)y=q(x)f(D) y = q(x)     where D=ddxD = \frac{d}{dx} is the differential operator, f(D)f(D) is a polynomial in DD, yy is the dependent variable, and q(x)q(x) is the non-homogeneous term (right-hand side function of xx).

  • Structure of the General Solution:

    • The general solution of an nn-th order linear differential equation consists of two distinct components:     y=CF+PIy = \text{CF} + \text{PI}     where CF\text{CF} represents the Complementary Function and PI\text{PI} represents the Particular Integral.

  • Role of the Complementary Function (CF):

    • The Complementary Function is obtained entirely from the left-hand side (LHS) operator f(D)f(D) by setting the equation to its homogeneous form (q(x)=0q(x) = 0).

    • It solves the homogeneous linear differential equation f(D)y=0f(D) y = 0 and incorporates nn arbitrary constants for an nn-th order differential equation.

  • Role of the Particular Integral (PI):

    • The Particular Integral is derived using the right-hand side (RHS) non-homogeneous term q(x)q(x).

    • The specific method to determine PI\text{PI} depends on the mathematical form of q(x)q(x), such as exponential functions eaxe^{ax}, polynomials xmx^m, trigonometric functions cos⁡(ax)\cos(ax) or sin⁡(ax)\sin(ax), logarithmic functions ln⁡(ax)\ln(ax), or trigonometric functions like tan⁡(ax)\tan(ax).

Complementary Functions for Homogeneous Equations

  • Procedure for Finding the Complementary Function:

    • Step 1: Form the homogeneous equation by setting the right-hand side equal to zero (q(x)=0q(x) = 0).

    • Step 2: Form the Auxiliary Equation (AE) by substituting D=mD = m into f(D)f(D), resulting in the polynomial equation f(m)=0f(m) = 0.

    • Step 3: Solve the polynomial auxiliary equation for its roots m1,m2,…,mnm_1, m_2, \dots, m_n. Standard calculators can be used to solve quadratic or cubic equations directly unless the roots are complex.

  • Classification of Auxiliary Equation Roots and CF Rules:

    • Case 1: Real and Distinct Roots:

    • If the roots m1,m2m_1, m_2 are real numbers and m1≠m2m_1 \neq m_2:       CF=Aem1x+Bem2x\text{CF} = A e^{m_1 x} + B e^{m_2 x}

    • The order of assignment of constants to roots is arbitrary; Aem1x+Bem2xA e^{m_1 x} + B e^{m_2 x} is identical to Aem2x+Bem1xA e^{m_2 x} + B e^{m_1 x}.

    • Case 2: Real and Equal (Repeated) Roots:

    • If two roots are real and equal (m1=m2=mm_1 = m_2 = m):       CF=(Ax+B)emx\text{CF} = (A x + B) e^{m x}

    • If three roots are real and equal (m1=m2=m3=mm_1 = m_2 = m_3 = m):       CF=(Ax2+Bx+C)emx\text{CF} = (A x^2 + B x + C) e^{m x}

    • Case 3: Complex Conjugate Roots:

    • If the roots are complex conjugates of the form m=α±iβm = \alpha \pm i \beta, where α\alpha is the real part and β\beta is the imaginary coefficient:       CF=eαx(Acos⁡(βx)+Bsin⁡(βx))\text{CF} = e^{\alpha x} (A \cos(\beta x) + B \sin(\beta x))

    • If the real part α=0\alpha = 0 (purely imaginary roots m=±iβm = \pm i \beta), then e0x=1e^{0 x} = 1, simplifying the expression to:       CF=Acos⁡(βx)+Bsin⁡(βx)\text{CF} = A \cos(\beta x) + B \sin(\beta x)

    • For quadratic equations where complex roots cannot be determined by factoring by inspection, use the quadratic formula:       m=−b±b2−4ac2am = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a}       for an equation written in standard quadratic form am2+bm+c=0a m^2 + b m + c = 0.

  • Worked Examples for Complementary Functions:

    • Example 1: Second-Order Equation with Distinct Real Roots:

    • Differential Equation: (D2−5D+6)y=0(D^2 - 5D + 6)y = 0

    • Auxiliary Equation: m2−5m+6=0m^2 - 5m + 6 = 0

    • Factoring: (m−3)(m−2)=0  ⟹  m1=2,m2=3(m - 3)(m - 2) = 0 \implies m_1 = 2, m_2 = 3

    • Complementary Function: CF=Ae2x+Be3x\text{CF} = A e^{2x} + B e^{3x} (or CF=Ae3x+Be2x\text{CF} = A e^{3x} + B e^{2x})

    • Example 2: Second-Order Equation with Repeated Real Roots:

    • Differential Equation: (D2+2D+1)y=0(D^2 + 2D + 1)y = 0

    • Auxiliary Equation: m2+2m+1=0m^2 + 2m + 1 = 0

    • Factoring: (m+1)2=0  ⟹  m1=−1,m2=−1(m + 1)^2 = 0 \implies m_1 = -1, m_2 = -1

    • Complementary Function: CF=(Ax+B)e−x\text{CF} = (A x + B) e^{-x}

    • Example 3: Third-Order Equation with Three Repeated Real Roots:

    • Differential Equation: (D3+3D2+3D+1)y=0(D^3 + 3D^2 + 3D + 1)y = 0

    • Auxiliary Equation: m3+3m2+3m+1=0m^3 + 3m^2 + 3m + 1 = 0

    • Factoring: (m+1)3=0  ⟹  (m+1)(m+1)(m+1)=0  ⟹  m=−1,−1,−1(m + 1)^3 = 0 \implies (m + 1)(m + 1)(m + 1) = 0 \implies m = -1, -1, -1

    • Caveat: Do not drop repeated factors or state m=−1m = -1 as a single root; all three repeated roots must be accounted for in the degree of the polynomial pre-factor.

    • Complementary Function: CF=(Ax2+Bx+C)e−x\text{CF} = (A x^2 + B x + C) e^{-x}

    • Example 4: Second-Order Equation with Complex Roots:

    • Differential Equation: (D2+2D+5)y=0(D^2 + 2D + 5)y = 0

    • Auxiliary Equation: m2+2m+5=0m^2 + 2m + 5 = 0

    • Applying Quadratic Formula (a=1,b=2,c=5a = 1, b = 2, c = 5):       m=−2±22−4(1)(5)2(1)=−2±4−202=−2±−162=−2±4i2=−1±2im = \frac{-2 \pm \sqrt{2^2 - 4(1)(5)}}{2(1)} = \frac{-2 \pm \sqrt{4 - 20}}{2} = \frac{-2 \pm \sqrt{-16}}{2} = \frac{-2 \pm 4i}{2} = -1 \pm 2i

    • Identification: Real part α=−1\alpha = -1, imaginary coefficient β=2\beta = 2

    • Complementary Function: CF=e−x(Acos⁡(2x)+Bsin⁡(2x))\text{CF} = e^{-x} (A \cos(2x) + B \sin(2x))

    • Example 5: Third-Order Equation with Mixed Real and Complex Roots:

    • Differential Equation: (D3−1)y=0(D^3 - 1)y = 0

    • Auxiliary Equation: m3−1=0m^3 - 1 = 0

    • Warning: Do not simplify improperly as m3=1  ⟹  m=1,1,1m^3 = 1 \implies m = 1, 1, 1.

    • Factoring Identity: a3−b3=(a−b)(a2+ab+b2)a^3 - b^3 = (a - b)(a^2 + ab + b^2)

    • Factored Form: (m−1)(m2+m+1)=0(m - 1)(m^2 + m + 1) = 0

    • Root 1: m−1=0  ⟹  m1=1m - 1 = 0 \implies m_1 = 1

    • Roots 2 & 3: For m2+m+1=0m^2 + m + 1 = 0, apply quadratic formula (a=1,b=1,c=1a = 1, b = 1, c = 1):       m=−1±12−4(1)(1)2(1)=−1±−32=−12±i32m = \frac{-1 \pm \sqrt{1^2 - 4(1)(1)}}{2(1)} = \frac{-1 \pm \sqrt{-3}}{2} = -\frac{1}{2} \pm i \frac{\sqrt{3}}{2}

    • Complementary Function: Combining real root m=1m = 1 and complex conjugate pair α=−12,β=32\alpha = -\frac{1}{2}, \beta = \frac{\sqrt{3}}{2}:       CF=e−12x(Acos⁡(32x)+Bsin⁡(32x))+Cex\text{CF} = e^{-\frac{1}{2} x} \left( A \cos\left(\frac{\sqrt{3}}{2} x\right) + B \sin\left(\frac{\sqrt{3}}{2} x\right) \right) + C e^x

    • Example 6: Fourth-Order Equation with Mixed Real and Imaginary Roots:

    • Differential Equation: (D4−1)y=0(D^4 - 1)y = 0

    • Auxiliary Equation: m4−1=0m^4 - 1 = 0

    • Warning: Do not simplify as m4=1  ⟹  m=1,1,1,1m^4 = 1 \implies m = 1, 1, 1, 1.

    • Factoring Strategy: Use a2−b2=(a−b)(a+b)a^2 - b^2 = (a - b)(a + b), writing (m2)2−12=0(m^2)^2 - 1^2 = 0:       (m2−1)(m2+1)=0(m^2 - 1)(m^2 + 1) = 0

    • Real Roots: m2−1=0  ⟹  m=±1m^2 - 1 = 0 \implies m = \pm 1

    • Imaginary Roots: m2+1=0  ⟹  m2=−1  ⟹  m=±i=0±1im^2 + 1 = 0 \implies m^2 = -1 \implies m = \pm i = 0 \pm 1i

    • Roots Summary: Four distinct roots m=1,−1,i,−im = 1, -1, i, -i

    • Complementary Function:       CF=Aex+Be−x+Ccos⁡(x)+Dsin⁡(x)\text{CF} = A e^x + B e^{-x} + C \cos(x) + D \sin(x)       (written equivalently as CF=Acos⁡(x)+Bsin⁡(x)+Cex+De−x\text{CF} = A \cos(x) + B \sin(x) + C e^x + D e^{-x})

Particular Integrals for Exponential Functions

  • Methodology for Type 1 (q(x)=eaxq(x) = e^{ax}):

    • Standard Particular Integral Form:     PI=1f(D)eax\text{PI} = \frac{1}{f(D)} e^{ax}

    • Basic Substitution Rule: Replace the differential operator DD with the constant aa (D=aD = a).

    • Case 1: Non-Zero Denominator (f(a)≠0f(a) \neq 0):

    • If substituting D=aD = a results in a non-zero denominator:       PI=1f(a)eax\text{PI} = \frac{1}{f(a)} e^{ax}

    • Case 2: Zero Denominator / Rule Failure (f(a)=0f(a) = 0):

    • Substituting D=aD = a yielding f(a)=0f(a) = 0 causes division by zero, indicating rule failure.

    • Action: Pre-multiply the expression by xx and differentiate the denominator polynomial f(D)f(D) with respect to DD:       PI=x1f′(D)eax\text{PI} = x \frac{1}{f'(D)} e^{ax}

    • Evaluate f′(a)f'(a). If f′(a)≠0f'(a) \neq 0, the Particular Integral is:       PI=x1f′(a)eax\text{PI} = x \frac{1}{f'(a)} e^{ax}

    • Iterative Failure Rule: If f′(a)=0f'(a) = 0 remains zero, repeat the procedure by multiplying by xx again (yielding x2x^2) and differentiating the denominator again (f′′(D)f''(D)):       PI=x21f′′(D)eax\text{PI} = x^2 \frac{1}{f''(D)} e^{ax}

    • Continue iterating until a non-zero value is obtained in the denominator upon evaluating at D = a$.\n\n* **Worked Examples for Type 1 Exponential Functions**:\n * **Problem 1: Non-Zero Denominator Case**:\n * Differential Equation: (D^2 + 3D + 2)y = e^x\n * Complementary Function: Homogeneous equation (D^2 + 3D + 2)y = 0 \implies m^2 + 3m + 2 = 0 \implies (m + 1)(m + 2) = 0 \implies m = -1, -2.\n      \text{CF} = A e^{-x} + B e^{-2x}\n * Particular Integral:\n      \text{PI} = \frac{1}{D^2 + 3D + 2} e^x\n      Here a = 1.Substitute. SubstituteD = 1 into denominator:\n      \text{Denominator} = 1^2 + 3(1) + 2 = 6 eq 0\n      \text{PI} = \frac{1}{6} e^x\n * General Solution:\n      y = \text{CF} + \text{PI} = A e^{-x} + B e^{-2x} + \frac{1}{6} e^x\n * **Problem 2: Single Rule Failure Case**:\n * Differential Equation: (D^2 - 3D + 2)y = e^x\n * Complementary Function: Homogeneous equation (D^2 - 3D + 2)y = 0 \implies m^2 - 3m + 2 = 0 \implies (m - 1)(m - 2) = 0 \implies m = 1, 2.\n      \text{CF} = A e^x + B e^{2x}\n * Particular Integral:\n      \text{PI} = \frac{1}{D^2 - 3D + 2} e^x\n      Here a = 1.Substitute. SubstituteD = 1 into denominator:\n      \text{Denominator} = 1^2 - 3(1) + 2 = 0\n      Rule fails due to zero denominator.\n * Apply Failure Rule: Multiply by xanddifferentiatedenominatorw.r.tand differentiate denominator w.r.tD((\frac{d}{dD}(D^2 - 3D + 2) = 2D - 3):\n      \text{PI} = x \frac{1}{2D - 3} e^x\n      Substitute D = 1intointo2D - 3:\n      \text{Denominator} = 2(1) - 3 = -1 eq 0\n      \text{PI} = x \frac{1}{-1} e^x = -x e^x\n * General Solution:\n      y = \text{CF} + \text{PI} = A e^x + B e^{2x} - x e^x\n * **Problem 3: Double Rule Failure Case**:\n * Differential Equation: (D^2 + 2D + 1)y = e^{-x}\n * Complementary Function: Auxiliary equation m^2 + 2m + 1 = 0 \implies (m + 1)^2 = 0 \implies m = -1, -1.\n      \text{CF} = (A x + B) e^{-x}\n * Particular Integral:\n      \text{PI} = \frac{1}{D^2 + 2D + 1} e^{-x}\n      Here a = -1.Substitute. SubstituteD = -1 into denominator:\n      \text{Denominator} = (-1)^2 + 2(-1) + 1 = 1 - 2 + 1 = 0\n      Rule fails.\n * First Failure Step: Multiply by xanddifferentiatedenominatorw.r.tand differentiate denominator w.r.tD((\frac{d}{dD}(D^2 + 2D + 1) = 2D + 2):\n      \text{PI} = x \frac{1}{2D + 2} e^{-x}\n      Substitute D = -1intointo2D + 2:\n      \text{Denominator} = 2(-1) + 2 = 0\n      Rule fails again.\n * Second Failure Step: Multiply by xagain(again (x \times x = x^2)anddifferentiatedenominatorw.r.t) and differentiate denominator w.r.tD((\frac{d}{dD}(2D + 2) = 2):\n      \text{PI} = x^2 \frac{1}{2} e^{-x} = \frac{x^2}{2} e^{-x}\n * General Solution:\n      y = \text{CF} + \text{PI} = (A x + B) e^{-x} + \frac{x^2}{2} e^{-x}\n\n# Particular Integrals for Trigonometric Functions\n\n* **Methodology for Type 2 (q(x) = \sin(ax)oror\cos(ax)**):\n * Standard Particular Integral Form:\n    \text{PI} = \frac{1}{f(D^2)} \sin(ax) \quad \text{or} \quad \text{PI} = \frac{1}{f(D^2)} \cos(ax)\n * Substitution Rule: Replace D^2withwith-a^2.\n * Critical Warning on Order of Operations: The expression -a^2meansmeans-(a^2),NOT, NOT(-a)^2.Forexample,if. For example, ifa = 2,,D^2isreplacedbyis replaced by-2^2 = -4,not, not(-2)^2 = +4$.

    • Handling Odd Powers of DD: For odd powers of DD like D3D^3, rewrite the term as D⋅D2D \cdot D^2 to allow substitution of D2=−a2D^2 = -a^2.

    • Case 1: Non-Zero Denominator (f(−a2)≠0f(-a^2) \neq 0):

    • If evaluating f(−a2)f(-a^2) yields a non-zero denominator:       \text{PI} = \frac{1}{f(-a^2)} \sin(ax) \quad \text{or} \t\text{PI} = \frac{1}{f(-a^2)} \cos(ax)

    • Case 2: Zero Denominator (f(−a2)=0f(-a^2) = 0):

    • If substitution yields zero, pre-multiply by xx and differentiate the denominator with respect to DD:       PI=x1f′(D)sin⁡(ax)\text{PI} = x \frac{1}{f'(D)} \sin(ax)

    • If the derivative leaves an isolated DD in the denominator, multiply numerator and denominator by DD to re-introduce D2D^2 in the denominator, substitute D2=−a2D^2 = -a^2, and differentiate the numerator function.

    • Conjugate Method for Linear Operator Terms in Denominator:

    • When substituting D2=−a2D^2 = -a^2 leaves a linear expression in DD (e.g., αD+β\alpha D + \beta), multiply numerator and denominator by its algebraic conjugate αD−β\alpha D - \beta:       1αD+β=αD−β(αD+β)(αD−β)=αD−βα2D2−β2\frac{1}{\alpha D + \beta} = \frac{\alpha D - \beta}{(\alpha D + \beta)(\alpha D - \beta)} = \frac{\alpha D - \beta}{\alpha^2 D^2 - \beta^2}

    • Practical Recommendations for Sign Error Prevention:

      • If the denominator contains negative terms like −2D−3-2D - 3, factor out −1-1 to write −(2D+3)-(2D + 3), then multiply numerator and denominator by conjugate (2D−3)(2D - 3).

      • If the denominator is −4D+5-4D + 5, factor out −1-1 to write −(4D−5)-(4D - 5), then multiply numerator and denominator by conjugate (4D+5)(4D + 5).

  • Worked Examples for Type 2 Trigonometric Functions:

    • Problem 1: Standard Non-Zero Denominator Case:

    • Differential Equation: (D2+4)y=cos⁡(x)(D^2 + 4)y = \cos(x)

    • Complementary Function: Auxiliary equation m2+4=0  ⟹  m=±2i=0±2im^2 + 4 = 0 \implies m = \pm 2i = 0 \pm 2i.       CF=Acos⁡(2x)+Bsin⁡(2x)\text{CF} = A \cos(2x) + B \sin(2x)

    • Particular Integral:       PI=1D2+4cos⁡(x)\text{PI} = \frac{1}{D^2 + 4} \cos(x)       Here a=1a = 1. Replace D2D^2 with −12=−1-1^2 = -1:       Denominator=−1+4=3≠0\text{Denominator} = -1 + 4 = 3 \neq 0       PI=13cos⁡(x)\text{PI} = \frac{1}{3} \cos(x)

    • General Solution:       y=CF+PI=Acos⁡(2x)+Bsin⁡(2x)+13cos⁡(x)y = \text{CF} + \text{PI} = A \cos(2x) + B \sin(2x) + \frac{1}{3} \cos(x)

    • Problem 2: Zero Denominator Case with Operational Operator Multiplication:

    • Differential Equation: (D2+4)y=cos⁡(2x)(D^2 + 4)y = \cos(2x)

    • Complementary Function: Auxiliary equation m2+4=0  ⟹  m=±2im^2 + 4 = 0 \implies m = \pm 2i.       CF=Acos⁡(2x)+Bsin⁡(2x)\text{CF} = A \cos(2x) + B \sin(2x)

    • Particular Integral:       PI=1D2+4cos⁡(2x)\text{PI} = \frac{1}{D^2 + 4} \cos(2x)       Here a=2a = 2. Replace D2D^2 with −22=−4-2^2 = -4:       Denominator=−4+4=0\text{Denominator} = -4 + 4 = 0       Rule fails.

    • Multiply by xx and differentiate denominator w.r.t DD (ddD(D2+4)=2D\frac{d}{dD}(D^2 + 4) = 2D):       PI=x12Dcos⁡(2x)\text{PI} = x \frac{1}{2D} \cos(2x)

    • Multiply numerator and denominator by DD to form D2D^2 in denominator:       PI=xD2D2cos⁡(2x)\text{PI} = x \frac{D}{2D^2} \cos(2x)       Substitute D2=−4D^2 = -4 into denominator:       Denominator=2(−4)=−8\text{Denominator} = 2(-4) = -8       PI=x1−8D(cos⁡(2x))\text{PI} = x \frac{1}{-8} D(\cos(2x))       Evaluate D(cos⁡(2x))=ddx(cos⁡(2x))=−2sin⁡(2x)D(\cos(2x)) = \frac{d}{dx}(\cos(2x)) = -2 \sin(2x), giving:       PI=−x8(−2sin⁡(2x))=xsin⁡(2x)4\text{PI} = -\frac{x}{8} (-2 \sin(2x)) = \frac{x \sin(2x)}{4}

    • General Solution:       y=CF+PI=Acos⁡(2x)+Bsin⁡(2x)+xsin⁡(2x)4y = \text{CF} + \text{PI} = A \cos(2x) + B \sin(2x) + \frac{x \sin(2x)}{4}

    • Problem 3: Conjugate Method for First-Degree Operator Denominator:

    • Differential Equation: (D2+5D+6)y=sin⁡(3x)(D^2 + 5D + 6)y = \sin(3x)

    • Complementary Function: Auxiliary equation m2+5m+6=0  ⟹  (m+2)(m+3)=0  ⟹  m=−2,−3m^2 + 5m + 6 = 0 \implies (m + 2)(m + 3) = 0 \implies m = -2, -3.       CF=Ae−2x+Be−3x\text{CF} = A e^{-2x} + B e^{-3x}

    • Particular Integral:       PI=1D2+5D+6sin⁡(3x)\text{PI} = \frac{1}{D^2 + 5D + 6} \sin(3x)       Here a=3a = 3. Substitute D2=−32=−9D^2 = -3^2 = -9 into denominator:       Denominator=−9+5D+6=5D−3\text{Denominator} = -9 + 5D + 6 = 5D - 3

    • Multiply numerator and denominator by conjugate (5D+3)(5D + 3):       PI=5D+3(5D−3)(5D+3)sin⁡(3x)=5D+325D2−9sin⁡(3x)\text{PI} = \frac{5D + 3}{(5D - 3)(5D + 3)} \sin(3x) = \frac{5D + 3}{25 D^2 - 9} \sin(3x)       Substitute D2=−9D^2 = -9 into denominator:       Denominator=25(−9)−9=−225−9=−234≠0\text{Denominator} = 25(-9) - 9 = -225 - 9 = -234 \neq 0

    • Apply operator numerator to sin⁡(3x)\sin(3x):       (5D+3)sin⁡(3x)=5D(sin⁡(3x))+3sin⁡(3x)=5(3cos⁡(3x))+3sin⁡(3x)=15cos⁡(3x)+3sin⁡(3x)(5D + 3)\sin(3x) = 5 D(\sin(3x)) + 3 \sin(3x) = 5(3 \cos(3x)) + 3 \sin(3x) = 15 \cos(3x) + 3 \sin(3x)       PI=1−234(15cos⁡(3x)+3sin⁡(3x))\text{PI} = \frac{1}{-234} (15 \cos(3x) + 3 \sin(3x))

    • General Solution:       y=CF+PI=Ae−2x+Be−3x−1234(15cos⁡(3x)+3sin⁡(3x))y = \text{CF} + \text{PI} = A e^{-2x} + B e^{-3x} - \frac{1}{234} (15 \cos(3x) + 3 \sin(3x))

Particular Integrals for Polynomial Functions

  • Methodology for Type 3 (q(x)=xmq(x) = x^m):

    • Standard Particular Integral Form:     PI=1f(D)xm\text{PI} = \frac{1}{f(D)} x^m

    • Procedure:

    • Step 1: Factor out the lowest degree term or constant term from f(D)f(D) to transform the operator expression into the form [1±g(D)][1 \pm g(D)] in the denominator.

    • Step 2: Move the operator expression to the numerator as a negative binomial power, yielding [1±g(D)]−1[1 \pm g(D)]^{-1} or [1±g(D)]−2[1 \pm g(D)]^{-2}.

    • Step 3: Determine derivative truncation limit: Compute derivatives of xmx^m. Since Dm+1(xm)=0D^{m+1}(x^m) = 0, all series terms containing powers of DD greater than mm evaluate to zero and are truncated.

    • Step 4: Expand using standard Binomial expansion series and apply term-by-term to x^m$.\n\n* **Standard Binomial Expansion Formulas (Valid for \lvert x \rvert < 1)**:\n * First Binomial Identity:\n    (1 - x)^{-1} = 1 + x + x^2 + x^3 + \dots\n * Second Binomial Identity:\n    (1 + x)^{-1} = 1 - x + x^2 - x^3 + \dots\n    (Odd powers are negative, even powers are positive)\n * Third Binomial Identity:\n    (1 - x)^{-2} = 1 + 2x + 3x^2 + 4x^3 + \dots\n * Fourth Binomial Identity:\n    (1 + x)^{-2} = 1 - 2x + 3x^2 - 4x^3 + \dots\n    (Odd powers are negative, integer coefficients follow sequence 1, 2, 3, 4, \dots)\n\n* **Worked Examples for Type 3 Polynomial Functions**:\n * **Problem 1: Quadratic Polynomial RHS Case**:\n * Differential Equation: (D^2 - 4D + 4)y = x^2\n * Complementary Function: Auxiliary equation m^2 - 4m + 4 = 0 \implies (m - 2)^2 = 0 \implies m = 2, 2$.       CF=(Ax+B)e2x\text{CF} = (A x + B) e^{2x}

    • Particular Integral:       PI=1D2−4D+4x2=1(D−2)2x2=1(2−D)2x2\text{PI} = \frac{1}{D^2 - 4D + 4} x^2 = \frac{1}{(D - 2)^2} x^2 = \frac{1}{(2 - D)^2} x^2       Factor out 22=42^2 = 4 from denominator:       (2−D)2=22(1−D2)2=4(1−D2)2(2 - D)^2 = 2^2 \left(1 - \frac{D}{2}\right)^2 = 4 \left(1 - \frac{D}{2}\right)^2       Bring operator to numerator:       PI=14(1−D2)−2x2\text{PI} = \frac{1}{4} \left(1 - \frac{D}{2}\right)^{-2} x^2

    • Truncation Analysis for x2x^2:       D(x2)=2x,D2(x2)=2,D3(x2)=0D(x^2) = 2x, \quad D^2(x^2) = 2, \quad D^3(x^2) = 0

    • Expanding Series (1−X)−2=1+2X+3X2+…(1 - X)^{-2} = 1 + 2X + 3X^2 + \dots with X=D2X = \frac{D}{2}:       (1−D2)−2=1+2(D2)+3(D2)2=1+D+34D2\left(1 - \frac{D}{2}\right)^{-2} = 1 + 2\left(\frac{D}{2}\right) + 3\left(\frac{D}{2}\right)^2 = 1 + D + \frac{3}{4} D^2

    • Operating on x2x^2:       PI=14[1(x2)+D(x2)+34D2(x2)]=14[x2+2x+34(2)]=14[x2+2x+32]\text{PI} = \frac{1}{4} \left[ 1(x^2) + D(x^2) + \frac{3}{4} D^2(x^2) \right] = \frac{1}{4} \left[ x^2 + 2x + \frac{3}{4}(2) \right] = \frac{1}{4} \left[ x^2 + 2x + \frac{3}{2} \right]       Simplifying inside brackets using common denominator:       PI=14(2x2+4x+32)=18(2x2+4x+3)\text{PI} = \frac{1}{4} \left( \frac{2x^2 + 4x + 3}{2} \right) = \frac{1}{8} (2x^2 + 4x + 3)

    • General Solution:       y=CF+PI=(Ax+B)e2x+18(2x2+4x+3)y = \text{CF} + \text{PI} = (A x + B) e^{2x} + \frac{1}{8} (2x^2 + 4x + 3)

    • Problem 2: Linear Polynomial RHS Case:

    • Differential Equation: (D2+5D+6)y=x+1(D^2 + 5D + 6)y = x + 1

    • Complementary Function: Auxiliary equation m^2 + 5m + 6 = 0 \implies (m + 2)(m + 3) = 0 \implies m = -2, -3$.\n      \text{CF} = A e^{-2x} + B e^{-3x}\n * Particular Integral:\n      \text{PI} = \frac{1}{D^2 + 5D + 6} (x + 1) = \frac{1}{6 + 5D + D^2} (x + 1)\n      Factor out constant 6 from denominator:\n      \text{PI} = \frac{1}{6 \left[ 1 + \frac{5D + D^2}{6} \right]} (x + 1) = \frac{1}{6} \left[ 1 + \frac{5D + D^2}{6} \right]^{-1} (x + 1)\n * Truncation Analysis for (x + 1):\n      D(x + 1) = 1, \quad D^2(x + 1) = 0\n * Binomial Expansion (1 + X)^{-1} = 1 - X + X^2 - \dotswithwithX = \frac{5D + D^2}{6}:\n      Because D^2(x + 1) = 0,second−orderterms, second-order termsX^2containingcontainingD^2vanish.Retainonlyvanish. Retain only1 - X:\n      \text{PI} = \frac{1}{6} \left[ 1 - \frac{5D + D^2}{6} \right] (x + 1) = \frac{1}{6} \left[ (x + 1) - \frac{5 D(x + 1) + D^2(x + 1)}{6} \right]\n      \text{PI} = \frac{1}{6} \left[ x + 1 - \frac{5(1) + 0}{6} \right] = \frac{1}{6} \left[ x + 1 - \frac{5}{6} \right]\n      Simplify constant 1 - \frac{5}{6} = \frac{1}{6}:\n      \text{PI} = \frac{1}{6} \left( x + \frac{1}{6} \right)\n * General Solution:\n      y = \text{CF} + \text{PI} = A e^{-2x} + B e^{-3x} + \frac{1}{6} \left( x + \frac{1}{6} \right)$$