Green Function for Second Order Differential Equation with Initial Value Problem

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To find the Green's function for the second-order differential equation d^2X/dt^2 + 2 dX/dt + (1+k^2)X = f(t) with initial conditions X(0) = dX/dt(0) = 0, the function must satisfy specific properties, including continuity and a jump condition in the first derivative. The homogeneous solution is given by e^t(C_1cos(kt) + C_2sin(kt)), leading to a Green's function of the form G(t, τ) that is zero for 0 ≤ t ≤ τ. The continuity condition at t = τ requires that the limits from both sides equal zero, resulting in a relationship between constants C and D. The jump condition on the derivative provides a non-zero solution for C and D, indicating that G(t, τ) is not zero for τ ≤ t ≤ 1. The final query pertains to setting up the equation sum lambda G = f(x) for further solution steps.
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Homework Statement


need to find the green function for

d^2X / dt^2 + 2 dX/dt +(1+k^2)X= f(t)

with IV X(0)=dX/dt (=0) = 0

Homework Equations



eq. attached

The Attempt at a Solution


attached

whenever I try to solve the homogonous part, I get 0 due to the IV.
guessing my strategy is wrong.

what should it be??
 

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A "Green's function", G(t, \tau), for a problem like this (the coefficient of the second derivative is 1) must satisfy several properties:
1) It must satisfy the homogenous d.e. in t for every \tau.
2) It must satisfy the boundary conditions.
3) It must be continuous.
4) The "jump" in the first derivative at t= \tau must be one.

Here, the general solution to the homogeneous equation is
e^t(C_1cos(kt)+ C_2sin(kt))
which means that the Green's function must be of the form
G(t, \tau)= \begin{pmatrix}e^t(Acos(kt)+ Bsin(kt) & 0\le t\le \tau \\ e^t(Ccos(kt)+ Dsin(kt) & \tau\le t\le 1\end{pmatrix}

To satisfy the first boundary condition, since 0\le\tau, we must have
G(0,\tau)= A= 0
To satisfy the second boundary conditon, we must have
G_t(0,\tau)= A+ B= 0
which, since A= 0, give B= 0. That is, G(t, \tau) is identically 0 for all 0\le t\le \tau.

But that does NOT say that G(t,\tau) must be 0 for \tau\le t\le 1.

The continuity condition gives that
\lim_{t\to\tau^+}G(t,\tau)= e^{\tau}(C cos(k\tau)+ Dsin(k\tau))= \lim_{t\to\tau^-} G(t,\tau)= 0
so we must have
e^{\tau}(C cos(k\tau)+ D sin(k\tau))= 0
which leads to
D= -\frac{cos(k\tau)}{sin(k\tau)}C

The "jump" condition on the derivative says that
\lim_{t\to\tau^-}G_t(t,\tau)- \lim_{t\to\tau^+}G_t(t,\tau)= 1
which gives
e^\tau(Ck cos(kt)+ Dk sin(kt))+ e^\tau(-Ck sin(kt)+ Dk cos(kt))= 1

those two equations give non-zero values for C and D.
 
Thank you so much!

one more question though, do I set sum lambda G = f(x) and solve? (sorry, couldn't figure the Latex here)
 
Question: A clock's minute hand has length 4 and its hour hand has length 3. What is the distance between the tips at the moment when it is increasing most rapidly?(Putnam Exam Question) Answer: Making assumption that both the hands moves at constant angular velocities, the answer is ## \sqrt{7} .## But don't you think this assumption is somewhat doubtful and wrong?

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