Answer on Question #82233 – Math – Differential Equations
Question
Solve the initial value problem: y ′ ′ − 2 y ′ + y = 0 y'' - 2y' + y = 0 y ′′ − 2 y ′ + y = 0 ; y ( 1 ) = y ′ ( 1 ) = 0 y(1) = y'(1) = 0 y ( 1 ) = y ′ ( 1 ) = 0
A. y ( 0 ) = 3 y(0) = 3 y ( 0 ) = 3
B. y ( 0 ) = 1 y(0) = 1 y ( 0 ) = 1
C. y ( 0 ) = 2 y(0) = 2 y ( 0 ) = 2
D. y ( 0 ) = 0 y(0) = 0 y ( 0 ) = 0
Solution
This is a linear homogeneous second-order differential equation with constant coefficients. Solve the characteristic equation:
k 2 − 2 k + 1 = 0 k^2 - 2k + 1 = 0 k 2 − 2 k + 1 = 0 k 1 , 2 = − b ± b 2 − 4 a c 2 a = 2 ± 0 2 → k 1 = k 2 = 1 k_{1,2} = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a} = \frac{2 \pm \sqrt{0}}{2} \rightarrow k_1 = k_2 = 1 k 1 , 2 = 2 a − b ± b 2 − 4 a c = 2 2 ± 0 → k 1 = k 2 = 1
The solutions of the characteristic equation are double roots k 1 = k 2 = k k_1 = k_2 = k k 1 = k 2 = k , then the general solution is then:
y ( x ) = C 1 e k x + C 2 x e k x = { k = 1 } = C 1 e x + C 2 x e x y(x) = C_1 e^{kx} + C_2 x e^{kx} = \{k = 1\} = C_1 e^x + C_2 x e^x y ( x ) = C 1 e k x + C 2 x e k x = { k = 1 } = C 1 e x + C 2 x e x y ( 1 ) = y ′ ( 1 ) = 0 y(1) = y'(1) = 0 y ( 1 ) = y ′ ( 1 ) = 0 initial conditions give the following system:
{ C 1 e x + C 2 x e x = y ( x ) C 1 e x + C 2 e x + C 2 x e x = y ′ ( x ) → { C 1 + C 2 = 0 C 1 + 2 C 2 = 0 → { C 1 = 0 C 2 = 0 \left\{
\begin{array}{l}
C_1 e^x + C_2 x e^x = y(x) \\
C_1 e^x + C_2 e^x + C_2 x e^x = y'(x)
\end{array}
\right.
\rightarrow
\left\{
\begin{array}{l}
C_1 + C_2 = 0 \\
C_1 + 2 C_2 = 0
\end{array}
\right.
\rightarrow
\left\{
\begin{array}{l}
C_1 = 0 \\
C_2 = 0
\end{array}
\right. { C 1 e x + C 2 x e x = y ( x ) C 1 e x + C 2 e x + C 2 x e x = y ′ ( x ) → { C 1 + C 2 = 0 C 1 + 2 C 2 = 0 → { C 1 = 0 C 2 = 0 y ( x ) = 0 y(x) = 0 y ( x ) = 0
A.) y ( 0 ) = 3 y(0) = 3 y ( 0 ) = 3 , y ′ ( 1 ) = 0 y'(1) = 0 y ′ ( 1 ) = 0 initial conditions give the following system:
{ C 1 e x + C 2 x e x = y ( x ) C 1 e x + C 2 e x + C 2 x e x = y ′ ( x ) → { C 1 = 3 3 e 1 + C 2 e 1 + C 2 1 e 1 = 0 → { C 1 = 3 C 2 = − 3 / 2 \left\{
\begin{array}{l}
C_1 e^x + C_2 x e^x = y(x) \\
C_1 e^x + C_2 e^x + C_2 x e^x = y'(x)
\end{array}
\right.
\rightarrow
\left\{
\begin{array}{l}
C_1 = 3 \\
3 e^1 + C_2 e^1 + C_2 1 e^1 = 0
\end{array}
\right.
\rightarrow
\left\{
\begin{array}{l}
C_1 = 3 \\
C_2 = -3/2
\end{array}
\right. { C 1 e x + C 2 x e x = y ( x ) C 1 e x + C 2 e x + C 2 x e x = y ′ ( x ) → { C 1 = 3 3 e 1 + C 2 e 1 + C 2 1 e 1 = 0 → { C 1 = 3 C 2 = − 3/2 y ( x ) = 3 2 ( 2 − x ) e x y(x) = \frac{3}{2} (2 - x) e^x y ( x ) = 2 3 ( 2 − x ) e x
B.) y ( 0 ) = 1 y(0) = 1 y ( 0 ) = 1 , y ′ ( 1 ) = 0 y'(1) = 0 y ′ ( 1 ) = 0 initial conditions give the following system:
{ C 1 e x + C 2 x e x = y ( x ) C 1 e x + C 2 e x + C 2 x e x = y ′ ( x ) → { C 1 = 1 e 1 + C 2 e 1 + C 2 1 e 1 = 0 → { C 1 = 1 C 2 = − 1 / 2 \left\{
\begin{array}{l}
C_1 e^x + C_2 x e^x = y(x) \\
C_1 e^x + C_2 e^x + C_2 x e^x = y'(x)
\end{array}
\right.
\rightarrow
\left\{
\begin{array}{l}
C_1 = 1 \\
e^1 + C_2 e^1 + C_2 1 e^1 = 0
\end{array}
\right.
\rightarrow
\left\{
\begin{array}{l}
C_1 = 1 \\
C_2 = -1/2
\end{array}
\right. { C 1 e x + C 2 x e x = y ( x ) C 1 e x + C 2 e x + C 2 x e x = y ′ ( x ) → { C 1 = 1 e 1 + C 2 e 1 + C 2 1 e 1 = 0 → { C 1 = 1 C 2 = − 1/2 y ( x ) = 1 2 ( 2 − x ) e x y(x) = \frac{1}{2}(2 - x)e^x y ( x ) = 2 1 ( 2 − x ) e x
C.) y ( 0 ) = 2 y(0) = 2 y ( 0 ) = 2 , y ′ ( 1 ) = 0 y'(1) = 0 y ′ ( 1 ) = 0 initial conditions give the following system:
{ C 1 e x + C 2 x e x = y ( x ) C 1 e x + C 2 e x + C 2 x e x = y ′ ( x ) ⇒ { C 1 = 2 2 e 1 + C 2 e 1 + C 2 1 e 1 = 0 ⇒ { C 1 = 2 C 2 = − 1 \left\{
\begin{array}{c}
C_1 e^x + C_2 x e^x = y(x) \\
C_1 e^x + C_2 e^x + C_2 x e^x = y'(x)
\end{array}
\right.
\Rightarrow
\left\{
\begin{array}{c}
C_1 = 2 \\
2e^1 + C_2 e^1 + C_2 1e^1 = 0
\end{array}
\right.
\Rightarrow
\left\{
\begin{array}{c}
C_1 = 2 \\
C_2 = -1
\end{array}
\right. { C 1 e x + C 2 x e x = y ( x ) C 1 e x + C 2 e x + C 2 x e x = y ′ ( x ) ⇒ { C 1 = 2 2 e 1 + C 2 e 1 + C 2 1 e 1 = 0 ⇒ { C 1 = 2 C 2 = − 1 y ( x ) = ( 2 − x ) e x y(x) = (2 - x)e^x y ( x ) = ( 2 − x ) e x
D.) y ( 0 ) = 0 y(0) = 0 y ( 0 ) = 0 , y ′ ( 1 ) = 0 y'(1) = 0 y ′ ( 1 ) = 0 initial conditions give the following system:
{ C 1 e x + C 2 x e x = y ( x ) C 1 e x + C 2 e x + C 2 x e x = y ′ ( x ) ⇒ { C 1 = 0 C 2 e 1 + C 2 1 e 1 = 0 ⇒ { C 1 = 0 C 2 = 0 \left\{
\begin{array}{c}
C_1 e^x + C_2 x e^x = y(x) \\
C_1 e^x + C_2 e^x + C_2 x e^x = y'(x)
\end{array}
\right.
\Rightarrow
\left\{
\begin{array}{c}
C_1 = 0 \\
C_2 e^1 + C_2 1e^1 = 0
\end{array}
\right.
\Rightarrow
\left\{
\begin{array}{c}
C_1 = 0 \\
C_2 = 0
\end{array}
\right. { C 1 e x + C 2 x e x = y ( x ) C 1 e x + C 2 e x + C 2 x e x = y ′ ( x ) ⇒ { C 1 = 0 C 2 e 1 + C 2 1 e 1 = 0 ⇒ { C 1 = 0 C 2 = 0 y ( x ) = 0 y(x) = 0 y ( x ) = 0
**Answer:**
solution of the IVP: y ( x ) = 0 y(x) = 0 y ( x ) = 0
A. y ( x ) = 3 2 ( 2 − x ) e x y(x) = \frac{3}{2}(2 - x)e^x y ( x ) = 2 3 ( 2 − x ) e x
B. y ( x ) = 1 2 ( 2 − x ) e x y(x) = \frac{1}{2}(2 - x)e^x y ( x ) = 2 1 ( 2 − x ) e x
C. y ( x ) = ( 2 − x ) e x y(x) = (2 - x)e^x y ( x ) = ( 2 − x ) e x
D. y ( x ) = 0 y(x) = 0 y ( x ) = 0
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