I have to replicate a High Pass filter for some old speakers, however this filter is encased in resin and I can't destroy it to look at the component markings. I do know however the schematic configuration (not the values though). It is a T-Network like the one pictured below. I thought about measuring the response of the filter with a signal generator and an osci, then fitting this curve to the theoretical response curve of such a filter topology, thus finaly figuring out the component values.
However I cannot solve this simple Kirchoff problem, I would highly appreciate it if you can spot the mistake, I've been at this for 3 nights now 
I swear I'm suppoused to have a degree on this.
Hello there,
A degree on what?
There is no way you can calculate this without a load of some type, at the very least, a resistive load like 2 Ohms, 4 Ohms, 8 Ohms, 16 Ohms, 32 Ohms, and in some cases 64 Ohms. At least use 8 Ohms to get a feel for how this works. Heck, even use 10 Ohms just to see how it works.
The reason for this is the transfer function changes enormously with a load vs without a load of any kind. The output is not an ideal voltage source, it changes with load, and it changes a lot.
To illustrate this in detail, here is the transfer function with no load (and you can see how C2 factors out of the calculation as others have suggested):
Vout/Vin=(s^2*C1*L1)/(s^2*C1*L1 1)
and here is the transfer function with a resistive load Ro:
Vout/Vin=(Ro*s^3*C1*C2*L1)/(Ro*s^3*C1*C2*L1 s^2*C2*L1 s^2*C1*L1 Ro*s*C2 1)
See any difference?

Now with s=jw the first becomes:
(w^2*C1*L1)/(w^2*C1*L1-1)
and the second becomes:
(j*Ro*w^3*C1*C2*L1)/(j*Ro*w^3*C1*C2*L1 w^2*C2*L1 w^2*C1*L1-j*Ro*w*C2-1)
See any difference?

The first has phase shift of zero and the second has a non zero phase shift.
With Ro=1,C1=1,C2=1,L1=1, the first becomes:
w^2/(w^2-1)
and the second becomes:
(j*w^3)/(j*w^3 2*w^2-j*w-1)
where the first above has phase shift:
ph=0
and the second:
ph=atan2((2*w^5-w^3)/(w^6 2*w^4-3*w^2 1),(w^6-w^4)/(w^6 2*w^4-3*w^2 1))
and the first has amplitude:
w^2/abs(w^2-1)
and the second:
w^3/sqrt((w-w^3)^2 (1-2*w^2)^2)
You can see there is a huge difference between the load and no load versions. It would be impossible to curve fit the filter without the load.
What you could do is try to find a filter online that is used for the same purpose. Either that or maybe look up what your load impedance is.
You also have to keep in mind that the filter may be designed with the enclosure in mind. That would then have to include some speaker box calculations or some trial and error to get it right with the actual real life load and real life speaker box.
I do like the suggestions of looking at it as a 2 port network and going from there. You can even short the output for another reading, and short the input for another reading also. You may be able to determine the values that way, which absolutely works in theory. The only problem is that real life inductors have some strange characteristics when driven at unusual power levels. You may have to try a number of different frequencies and amplitudes to get a good look at the profile of this thing.
For more information on this, you can look up 2 port networks.
You'll have to make some decent measurements too.
Just to note, the output current with the output shorted to ground is:
Iout(s)=(s^2*Vin*C1*L1)/(s^2*C2*L1 s^2*C1*L1 1)
and with this we can see that C2 is still in effect.