Help using Green’s functions in solving Differential Equations please

In summary, the conversation included difficulties with tasks related to the Green function and solving differential equations using it. The summary also mentioned the use of partial integration and convolution as potential solutions to the tasks.
  • #1
Lambda96
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Homework Statement
see post
Relevant Equations
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Hi,

unfortunately I have several problems with the following task:

Bildschirmfoto 2023-07-06 um 10.52.15.png


Bildschirmfoto 2023-07-06 um 10.52.41.png


I have problems with the tasks a, d and e

Unfortunately, the Green function and solving differential equations with the Green function is completely new to me

In task b, I got the following for ##f_h(t)=e^{-at}##.Task a

$$\hat{L}G(t)=\Bigl( \frac{d}{dt} +a \Bigr) \Theta(t) f_h(t)$$
$$\hat{L}G(t)=\frac{d}{dt}\Theta(t) f_h(t) +a \Theta(t) f_h(t)$$
$$\hat{L}G(t)=\delta(t) f_h(t) + \Theta(t) f'_h(t) +a \Theta(t) f_h(t)$$
$$\hat{L}G(t)=\delta(t) f_h(t) -a \Theta(t) f_h(t) +a \Theta(t) f_h(t)$$
$$\hat{L}G(t)=\delta(t) f_h(t)$$

Can I now argue as follows that ##\hat{L}G(t)=\delta(t)## so when I multiply the operator by the Green function, I always get only one value. Then the following ##\delta(t)=\delta(0)## applies, so it follows that ##\delta(t) f_h(t)=\delta(0) f_h(0)## and since ##f_h(0)=1## only ##\delta(t)## remains on the left side of the equationTask d

I assumed that I should calculate the following integral.

$$\tilde{G}(\omega)= \int_{-\infty}^{\infty} dt \ e^{i \omega t} \hat{L} G(t) $$
$$ \tilde{G}(\omega)=\int_{-\infty}^{\infty} dt \ e^{i \omega t} \frac{d}{dt} G(t) +e^{i \omega t} a G(t) $$
$$ \tilde{G}(\omega)=\int_{-\infty}^{\infty} dt \ e^{i \omega t} \frac{d}{dt} G(t) +\int_{-\infty}^{\infty} dt \ e^{i \omega t} a G(t) $$

I then applied partial integration for the first integral

$$ \tilde{G}(\omega)=\biggl[ e^{i \omega t} G(t) \biggr]_{-\infty}^{\infty}-\int_{-\infty}^{\infty} dt \ i \omega e^{i \omega t} G(t) +\int_{-\infty}^{\infty} dt \ e^{i \omega t} a G(t) $$

Now, unfortunately, I don't get any further and I can't do anything with the hint from the task at the moment.
Task e

I thought that a solution may look like the following.

$$ f(t)= \int_{0}^{t} G(t)g(t) dt $$

I then calculated the following integral

$$ f(t)= \int_{0}^{t} G(t)g(t) dt $$
$$ f(t)= \int_{0}^{t} e^{-at} e^{2at} dt $$
$$ f(t)= \frac{e^{at} -1}{a}$$

If I substitute this ##f(t)## into ##\hat{L}f(t)##, I get ##2e^{at}-2## but I should get ##e^{2at}##.
 
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  • #2
Lambda96 said:
Task a

$$\hat{L}G(t)=\Bigl( \frac{d}{dt} +a \Bigr) \Theta(t) f_h(t)$$
$$\hat{L}G(t)=\frac{d}{dt}\Theta(t) f_h(t) +a \Theta(t) f_h(t)$$
$$\hat{L}G(t)=\delta(t) f_h(t) + \Theta(t) f'_h(t) +a \Theta(t) f_h(t)$$
$$\hat{L}G(t)=\delta(t) f_h(t) -a \Theta(t) f_h(t) +a \Theta(t) f_h(t)$$
$$\hat{L}G(t)=\delta(t) f_h(t)$$
Just use the property ##f(t)\delta(t) = f(0)\delta(t)##.

Lambda96 said:
Task d

I assumed that I should calculate the following integral.
The problem said to take the Fourier transform of the differential equation.

Lambda96 said:
Task e

I thought that a solution may look like the following.

$$ f(t)= \int_{0}^{t} G(t)g(t) dt $$
Look up convolution.
 
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  • #3
Thanks vela for your help 👍👍👍, with your tips I could solve the tasks now :smile:
 
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