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alekssr [168]
3 years ago
10

Consider the BVP

Mathematics
1 answer:
babymother [125]3 years ago
6 0

y''+\lambda y=0

has the corresponding characteristic equation (CE)

r^2+\lambda=0

a. If \lambda=0, then the CE has one root, r=0, and so the general solution to the ODE is

y(t)=C_1+C_2t

Given that y'(0)=y'\left(\frac\pi6\right)=0, and

y'(t)=C_2

it follows that C_2=0, and so

\boxed{y(t)=C_1}

b. If \lambda>0, then the CE has two complex roots, r=\pm i\sqrt\lambda, and the general solution is

y(t)=C_1\cos(\lambda t)+C_2\sin(\lambda t)

\implies y'(t)=-\lambda C_1\sin(\lambda t)+\lambda C_2\cos(\lambda t)

With the given boundary values, we have

y'(0)=0\implies\lambda C_2=0\implies C_2=0

y'\left(\dfrac\pi6\right)=0\implies-\lambda C_1\sin\left(\dfrac{\lambda\pi}6\right)=0

\implies\sin\left(\dfrac{\lambda\pi}6\right)=0

\implies\dfrac{\lambda\pi}6=n\pi

\implies\lambda=6n

where n\in\Bbb Z.

  • If \lambda is a (positive) multiple of 6, we have

y'\left(\dfrac\pi6\right)=0\implies-6nC_1\sin\left(\dfrac{6n\pi}6\right)=0\implies C_1=0

and the solution would be

\boxed{y(t)=0}

  • Otherwise, if \lambda is not a multiple of 6, we have

y'\left(\dfrac\pi6\right)=0\implies-\lambda C_1\sin\left(\dfrac{\lambda\pi}6\right)=0\implies C_1=0

so that we still get

\boxed{y(t)=0}

c. If \lambda, then the CE has two real roots, r=\pm\sqrt\lambda, so that the general solution is

y(t)=C_1e^{\sqrt\lambda\,t}+C_2e^{-\sqrt\lambda\,t}

\implies y'(t)=C_1\sqrt\lambda\,e^{\sqrt\lambda\,t}-C_2\sqrt\lambda\,e^{-\sqrt\lambda\,t}

From the boundary conditions we get

y'(0)=0\implies C_1\sqrt\lambda-C_2\sqrt\lambda=0\implies C_1=C_2

y'\left(\dfrac\pi6\right)=0\implies C_1\sqrt\lambda\,e^{(\pi\sqrt\lambda)/6}-C_2\sqrt\lambda\,e^{-(\pi\sqrt\lambda)/6}=0\implies C_1e^{(\pi\sqrt\lambda)/3}=C_2

from which it follows that C_1=C_2=0, so again the solution is

\boxed{y(t)=0}

d. We only get eigenvalues in the case when \lambda>0, as in part (b):

\boxed{\lambda=6n,\,n\in\{1,2,3,\ldots\}}

for which we get the corresponding eigenfunctions

\boxed{y(t)=\cos(6nt),\,n\in\{1,2,3,\ldots\}}

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