So welcome to our today's tutorial. Today we will consider exercise number nine, which
is a two-dimensional system with a unit thickness T and it is subjected to a heat flux Q as depicted
and the system is discretized by two linear triangular finite elements with a given connectivity
matrix. So you see here the red arrows, they indicate the heat flux and here the vectorial
description of the heat flux is given. As you see this heat flux extends over two elements
and the link between local and global coordinates is given by the connectivity matrix here on the
right hand side. Q0 is the only quantity that is given and we should compute the heat flow
vector per unit thickness due to the heat flux Q. This is the only task we have here, but yeah,
it's a little bit longer this exercise because we have to consider several issues that we
discussed during the last lectures. Okay, so the heat flow vector there we have to consider in the
recapitulations, the associated formulation we addressed this this morning. So let me just copy that.
So this is the heat flow vector and yeah, when we have a look at this there is only
one part that will play a role here namely the first part with a heat flux. We do not have any
distributed heat sources or see heat sources are so the second part does not appear here.
We have to do several steps to solve this question here or to answer this question.
And I would like to summarize them briefly as already discussed in the morning. We have to
start with the shape functions.
So somehow maybe we have to reopen it. So we start with the shape functions
and closely related to the shape functions we have the element representation. I put
that here in red because this is yet to be discussed. So
then we have to compute the Jacobian.
It's determinant and the inverse of the Jacobian.
Then we have to provide the link between and I put that here in red because this is also a
very important quantity. GEA which links the global sorry the reference and the physical
area elements. At least we will see that later we have to consider some of them.
Then
so we have to consider also Q bar in terms of the local coordinates. It is just given here in the
global coordinate system so we have to translate that into the local coordinates.
So we need QE of X and from that we have to derive QE of Xi and then we have to compute the
integral and eventually to get the vector which is fx for element one and for element two because
we have of course two elements and then we have to assemble the heat flow vector.
So these are the basic steps and we have to do them one after the other.
Let me first start with the element representation in the reference configuration.
So the triangular element we have the coordinates Xi 1 and Xi 2 and then we have a triangular
element and I would like to know from you what are the element nodes where are they located and
what are the associated shape functions. So first what are the local nodes where are they
placed. Let us start here in the corner which node is that?
Say it once again. Someone said that at least I meant to hear that. The third one yes. This one
is first. Okay and this is the second. Okay so and the shape functions which are they?
First shape function.
Which Xi? Xi 1. Second one. Two and third.
Let me go back to the question. Which parts of the question indicate that you indeed have to
use these shape functions? Exactly so this is important linear triangular elements.
This governs the number of element nodes and of course also the shape functions.
Okay let me furthermore copy the connectivity matrix.
This is the link between local and global coordinates and for the consideration of
this heat flux we need the surfaces of the element which are in the two-dimensional case
not the not areas but here edges and in addition we need also the surface normal vectors. Let me
just draw them. I do not specifically label them yet. I just sketch them here and of course they
would require specific labeling which I omit here because they are three different ones.
Presenters
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Dauer
01:21:09 Min
Aufnahmedatum
2024-05-28
Hochgeladen am
2024-05-31 02:29:06
Sprache
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