Answer on Question #44251 – Math - Differential Calculus | Equations
Solve the following Cauchy Euler equation by the method of variation of parameters.
x 2 y n − x y ′ + y = 2 x x ^ {2} y ^ {n} - x y ^ {\prime} + y = 2 x x 2 y n − x y ′ + y = 2 x
Determine the singular points of the following differential equation and classify each singular point as regular or irregular.
( x 2 − 9 ) 2 y n + ( x + 3 ) y ′ + 2 y = 0. (x ^ {2} - 9) ^ {2} y ^ {n} + (x + 3) y ^ {\prime} + 2 y = 0. ( x 2 − 9 ) 2 y n + ( x + 3 ) y ′ + 2 y = 0.
**Solution.**
Solve the Cauchy Euler equation by the method of variation of parameters.
By definition a Cauchy-Euler equation of order n n n has the form
a n x n y ( n ) ( x ) + a n − 1 x n − 1 y ( n − 1 ) ( x ) ⋯ + a 0 y ( x ) = 0 a _ {n} x ^ {n} y ^ {(n)} (x) + a _ {n - 1} x ^ {n - 1} y ^ {(n - 1)} (x) \dots + a _ {0} y (x) = 0 a n x n y ( n ) ( x ) + a n − 1 x n − 1 y ( n − 1 ) ( x ) ⋯ + a 0 y ( x ) = 0
So the correct equation
x 2 y ′ ′ − x y ′ + y = 2 x x ^ {2} y ^ {\prime \prime} - x y ^ {\prime} + y = 2 x x 2 y ′′ − x y ′ + y = 2 x
Solve this equation. The general solution will be the sum of the complementary solution and particular solution.
Find the complementary solution by solving x 2 y ′ ′ − x y ′ + y = 0 x^{2}y^{\prime \prime} - xy^{\prime} + y = 0 x 2 y ′′ − x y ′ + y = 0 .
Assume a solution to this Euler-Cauchy equation will be proportional to x λ x^{\lambda} x λ for some constant λ \lambda λ .
Substitute y ( x ) = x λ y(x) = x^{\lambda} y ( x ) = x λ into the differential equation:
x 2 ( x λ ) ′ ′ − x ( x λ ) ′ + x λ = 0 x ^ {2} \left(x ^ {\lambda}\right) ^ {\prime \prime} - x \left(x ^ {\lambda}\right) ^ {\prime} + x ^ {\lambda} = 0 x 2 ( x λ ) ′′ − x ( x λ ) ′ + x λ = 0 λ 2 x λ − 2 λ x λ + x λ = 0 \lambda^ {2} x ^ {\lambda} - 2 \lambda x ^ {\lambda} + x ^ {\lambda} = 0 λ 2 x λ − 2 λ x λ + x λ = 0
Factor out x λ x^{\lambda} x λ :
( λ 2 − 2 λ + 1 ) x λ = 0 (\lambda^ {2} - 2 \lambda + 1) x ^ {\lambda} = 0 ( λ 2 − 2 λ + 1 ) x λ = 0
Assuming x ≠ 0 x \neq 0 x = 0 , the zeros must come from the polynomial:
λ 2 − 2 λ + 1 = 0 \lambda^ {2} - 2 \lambda + 1 = 0 λ 2 − 2 λ + 1 = 0
Solve for λ \lambda λ :
λ 1 , 2 = 1 \lambda_ {1, 2} = 1 λ 1 , 2 = 1
The multiplicity of the root λ = 1 \lambda = 1 λ = 1 is 2 which gives y 1 ( x ) = c 1 x y_{1}(x) = c_{1}x y 1 ( x ) = c 1 x , y 2 ( x ) = c 2 x ln x y_{2}(x) = c_{2}x \ln x y 2 ( x ) = c 2 x ln x as solutions, where c 1 c_{1} c 1 and c 2 c_{2} c 2 are arbitrary constants.
The complementary solution is the sum of the above solutions:
y c ( x ) = y 1 ( x ) + y 2 ( x ) = c 1 x + c 2 x ln x y _ {c} (x) = y _ {1} (x) + y _ {2} (x) = c _ {1} x + c _ {2} x \ln x y c ( x ) = y 1 ( x ) + y 2 ( x ) = c 1 x + c 2 x ln x
Determine the particular solution by variation of parameters.
List the basis solutions in y c ( x ) y_{c}(x) y c ( x ) :
y b 1 ( x ) = x and y b 2 ( x ) = x ln x y _ {b _ {1}} (x) = x \text{ and } y _ {b _ {2}} (x) = x \ln x y b 1 ( x ) = x and y b 2 ( x ) = x ln x
Compute the Wronskian of y b 1 ( x ) y_{b_1}(x) y b 1 ( x ) and y b 2 ( x ) y_{b_2}(x) y b 2 ( x ) :
W ( x ) = ∣ x x ln x d d x ( x ) d d x ( x ln x ) ∣ = ∣ x x ln x 1 ln x + 1 ∣ = x W (x) = \left| \begin{array}{cc} x & x \ln x \\ \frac {d}{d x} (x) & \frac {d}{d x} (x \ln x) \end{array} \right| = \left| \begin{array}{cc} x & x \ln x \\ 1 & \ln x + 1 \end{array} \right| = x W ( x ) = ∣ ∣ x d x d ( x ) x ln x d x d ( x ln x ) ∣ ∣ = ∣ ∣ x 1 x ln x ln x + 1 ∣ ∣ = x
Divide the differential equation by the leading term's coefficient x 2 x^2 x 2 :
y ′ ′ − y ′ x + y x 2 = 2 x y ^ {\prime \prime} - \frac {y ^ {\prime}}{x} + \frac {y}{x ^ {2}} = \frac {2}{x} y ′′ − x y ′ + x 2 y = x 2
Let f ( x ) = 2 x f(x) = \frac{2}{x} f ( x ) = x 2 . Let ν 1 ( x ) = − ∫ f ( x ) y b 2 ( x ) W ( x ) d x \nu_{1}(x) = -\int \frac{f(x)y_{b_{2}}(x)}{W(x)} dx ν 1 ( x ) = − ∫ W ( x ) f ( x ) y b 2 ( x ) d x and ν 2 ( x ) = − ∫ f ( x ) y b 1 ( x ) W ( x ) d x \nu_{2}(x) = -\int \frac{f(x)y_{b_{1}}(x)}{W(x)} dx ν 2 ( x ) = − ∫ W ( x ) f ( x ) y b 1 ( x ) d x .
The particular solution will be given by:
y p ( x ) = v 1 ( x ) y b 1 ( x ) + v 2 ( x ) y b 2 ( x ) y _ {p} (x) = v _ {1} (x) y _ {b _ {1}} (x) + v _ {2} (x) y _ {b _ {2}} (x) y p ( x ) = v 1 ( x ) y b 1 ( x ) + v 2 ( x ) y b 2 ( x )
Compute ν 1 ( x ) \nu_{1}(x) ν 1 ( x ) :
ν 1 ( x ) = − ∫ 2 ln x x d x = − ln 2 x \nu_ {1} (x) = - \int \frac {2 \ln x}{x} d x = - \ln^ {2} x ν 1 ( x ) = − ∫ x 2 ln x d x = − ln 2 x
Compute ν 2 ( x ) \nu_{2}(x) ν 2 ( x ) :
ν 2 ( x ) = ∫ 2 x d x = 2 ln x \nu_ {2} (x) = \int \frac {2}{x} d x = 2 \ln x ν 2 ( x ) = ∫ x 2 d x = 2 ln x
The particular solution is thus:
y p ( x ) = v 1 ( x ) y b 1 ( x ) + v 2 ( x ) y b 2 ( x ) = − x ln 2 x + 2 x ln 2 x y _ {p} (x) = v _ {1} (x) y _ {b _ {1}} (x) + v _ {2} (x) y _ {b _ {2}} (x) = - x \ln^ {2} x + 2 x \ln^ {2} x y p ( x ) = v 1 ( x ) y b 1 ( x ) + v 2 ( x ) y b 2 ( x ) = − x ln 2 x + 2 x ln 2 x
Simplify:
y p ( x ) = x ln 2 x y _ {p} (x) = x \ln^ {2} x y p ( x ) = x ln 2 x
So the general solution:
y ( x ) = y c ( x ) + y p ( x ) = c 1 x + c 2 x ln x + x ln 2 x y (x) = y _ {c} (x) + y _ {p} (x) = c _ {1} x + c _ {2} x \ln x + x \ln^ {2} x y ( x ) = y c ( x ) + y p ( x ) = c 1 x + c 2 x ln x + x ln 2 x
Answer: y ( x ) = c 1 x + c 2 x ln x + x ln 2 x y(x) = c_{1}x + c_{2}x\ln x + x\ln^{2}x y ( x ) = c 1 x + c 2 x ln x + x ln 2 x .
Determine the singular points of the following differential equation and classify each singular point as regular or irregular.
Equation in standard form
N ( x ) y ′ ′ + P ( x ) y ′ + Q ( x ) y = 0 N(x) y'' + P(x) y' + Q(x) y = 0 N ( x ) y ′′ + P ( x ) y ′ + Q ( x ) y = 0
So our equation
( x 2 − 9 ) 2 y ′ ′ + ( x + 3 ) y ′ + 2 y = 0 (x^2 - 9)^2 y'' + (x + 3) y' + 2 y = 0 ( x 2 − 9 ) 2 y ′′ + ( x + 3 ) y ′ + 2 y = 0
The singular points of the equation are then the points where N ( x ) = 0 N(x) = 0 N ( x ) = 0 :
( x 2 − 9 ) 2 = 0 (x^2 - 9)^2 = 0 ( x 2 − 9 ) 2 = 0 x 1 , 2 = 3 , x 3 , 4 = − 3 x_{1,2} = 3, x_{3,4} = -3 x 1 , 2 = 3 , x 3 , 4 = − 3
Suppose x 0 x_0 x 0 is a singular point. Multiplying through by ( x − x 0 ) 2 / N ( x ) (x - x_0)^2 / N(x) ( x − x 0 ) 2 / N ( x ) , we may rewrite equation as
( x − x 0 ) 2 y ′ ′ + ( x − x 0 ) u ( x ) y ′ + v ( x ) y = 0 , (x - x_0)^2 y'' + (x - x_0) u(x) y' + v(x) y = 0, ( x − x 0 ) 2 y ′′ + ( x − x 0 ) u ( x ) y ′ + v ( x ) y = 0 ,
where
u ( x ) = ( x − x 0 ) P ( x ) N ( x ) , v ( x ) = ( x − x 0 ) 2 Q ( x ) N ( x ) , u(x) = \frac{(x - x_0) P(x)}{N(x)}, \quad v(x) = \frac{(x - x_0)^2 Q(x)}{N(x)}, u ( x ) = N ( x ) ( x − x 0 ) P ( x ) , v ( x ) = N ( x ) ( x − x 0 ) 2 Q ( x ) ,
We say that x 0 x_0 x 0 is a regular singular point if the rational functions u ( x ) u(x) u ( x ) and v ( x ) v(x) v ( x ) have no singularity at x 0 x_0 x 0 – that is, if the factors of x − x 0 x - x_0 x − x 0 in N ( x ) N(x) N ( x ) that cause N ( x ) N(x) N ( x ) to vanish at x 0 x_0 x 0 are canceled by such factors in ( x − x 0 ) P ( x ) (x - x_0)P(x) ( x − x 0 ) P ( x ) and ( x − x 0 ) 2 Q ( x ) (x - x_0)^2 Q(x) ( x − x 0 ) 2 Q ( x ) . Otherwise x 0 x_0 x 0 is an irregular singular point.
Consider x 0 = 3 x_0 = 3 x 0 = 3 . Find u ( x ) u(x) u ( x ) and v ( x ) v(x) v ( x ) :
u ( x ) = ( x − 3 ) ( x + 3 ) ( x 2 − 9 ) 2 = 1 x 2 − 9 u(x) = \frac{(x - 3)(x + 3)}{(x^2 - 9)^2} = \frac{1}{x^2 - 9} u ( x ) = ( x 2 − 9 ) 2 ( x − 3 ) ( x + 3 ) = x 2 − 9 1 v ( x ) = ( x − 3 ) 2 ⋅ 2 ( x 2 − 9 ) 2 = 2 ( x + 3 ) 2 v(x) = \frac{(x - 3)^2 \cdot 2}{(x^2 - 9)^2} = \frac{2}{(x + 3)^2} v ( x ) = ( x 2 − 9 ) 2 ( x − 3 ) 2 ⋅ 2 = ( x + 3 ) 2 2 u ( x ) u(x) u ( x ) has singularity at x 0 x_0 x 0 , so x 0 = 3 x_0 = 3 x 0 = 3 is an irregular singular point.
Consider x 0 = − 3 x_0 = -3 x 0 = − 3 . Find u ( x ) u(x) u ( x ) and v ( x ) v(x) v ( x ) :
u ( x ) = ( x + 3 ) ( x + 3 ) ( x 2 − 9 ) 2 = 1 ( x − 3 ) 2 u(x) = \frac{(x + 3)(x + 3)}{(x^2 - 9)^2} = \frac{1}{(x - 3)^2} u ( x ) = ( x 2 − 9 ) 2 ( x + 3 ) ( x + 3 ) = ( x − 3 ) 2 1 v ( x ) = ( x + 3 ) 2 ⋅ 2 ( x 2 − 9 ) 2 = 2 ( x − 3 ) 2 v(x) = \frac{(x + 3)^2 \cdot 2}{(x^2 - 9)^2} = \frac{2}{(x - 3)^2} v ( x ) = ( x 2 − 9 ) 2 ( x + 3 ) 2 ⋅ 2 = ( x − 3 ) 2 2 u ( x ) u(x) u ( x ) and v ( x ) v(x) v ( x ) have no singularity at x 0 x_0 x 0 , so x 0 = − 3 x_0 = -3 x 0 = − 3 is a regular singular point.
**Answer**: x 0 = 3 x_0 = 3 x 0 = 3 is an irregular singular point, x 0 = − 3 x_0 = -3 x 0 = − 3 is a regular singular point.
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