last round of updates from Maxi, minor fixes
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Meshless Methods
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=======================
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For all computers and based methods we need to find a suitable discrete representation.
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For all computer-based methods we need to find a suitable _discrete_ representation.
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While this is straight-forward for cases such as data consisting only of integers, it is more challenging
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for continuously changing quantities such as the temperature in a room.
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While the previous examples have focused on aspects beyond discretization
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@@ -52,9 +52,10 @@ amount of additional complexity in an implementation, and the arbitrary
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connectivities call for _message-passing_ approaches between the nodes of a graph.
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This message passing is usually realized using fully-connected layers, instead of convolutions.
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Thus, in the following, we will focus on a particle-based method, which offers
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the same flexibility in terms of spatial adaptivity as GNNs, but still
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employs a convolution operator for learning the physical relationships.
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Thus, in the following, we will focus on a particle-based method {cite}`ummenhofer2019contconv`, which offers
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the same flexibility in terms of spatial adaptivity as GNNs. These were previously employed for
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a very similar goal {cite}`sanchez2020learning`, however, the method below
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enables a real convolution operator for learning the physical relationships.
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## Meshless and particle-based methods
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