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unable to cross ref for quarto bug
Browse files- Code/.gitignore +1 -0
- Data/1_Writing/1_Task/1_Introduction copy.qmd +18 -0
- Data/1_Writing/1_Task/1_Introduction.qmd +4 -18
- Data/1_Writing/1_Task/4_CNMc.qmd +1 -1
- Data/1_Writing/2_Task/0_Methodlogy.qmd +1 -1
- trials.qmd +38 -11
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Data/1_Writing/1_Task/1_Introduction copy.qmd
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# Introduction {#sec-chap_1_Intro}
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In this work, a tool called \glsfirst{cnmc} is further developed.
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The overall goal, in very brief terms, is to generate a model, which is able to
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predict the trajectories of general dynamical systems. The model
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shall be capable of predicting the trajectories when a model parameter
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value is changed.
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Some basics about dynamical systems are covered in
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subsection [-@sec-subsec_1_1_1_Principles] and in-depth explanations about \gls{cnmc} are given in
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chapter [-@sec-chap_2_Methodology]. \newline
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However, for a short and broad introduction to \gls{cnmc} the workflow depicted in figure @fig-fig_1_CNMC_Workflow shall be highlighted.
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The input it receives is data of a dynamical system or space state vectors for a range of model parameter values. The two main important outcomes are some accuracy measurements and the predicted trajectory for each desired model parameter value.
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Any inexperienced user may only have a look at the predicted trajectories to
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quickly decide visually whether the prediction matches the trained data. Since \gls{cnmc} is written in a modular manner, meaning it can be regarded as
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a black-box function, it can easily be integrated into other existing codes or
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workflows. \newline
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{#fig-fig_1_CNMC_Workflow}
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# Introduction {#sec-chap_1_Intro}
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The overall goal, in very brief terms, is to generate a model, which is able to
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predict the trajectories of general dynamical systems. The model
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shall be capable of predicting the trajectories when a model parameter
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value is changed.
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Some basics about dynamical systems are covered in
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subsection [-@sec-subsec_1_1_1_Principles] and in-depth explanations about \gls{cnmc} are given in
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chapter [-@sec-chap_2_Methodlogy]. \newline
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However, for a short and broad introduction to \gls{cnmc} the workflow depicted in figure @fig-fig_1_CNMC_Workflow shall be highlighted.
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The input it receives is data of a dynamical system or space state vectors for a range of model parameter values. The two main important outcomes are some accuracy measurements and the predicted trajectory for each desired model parameter value.
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Any inexperienced user may only have a look at the predicted trajectories to
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quickly decide visually whether the prediction matches the trained data. Since \gls{cnmc} is written in a modular manner, meaning it can be regarded as
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a black-box function, it can easily be integrated into other existing codes or
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workflows. \newline
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{#fig-fig_1_CNMC_Workflow}
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# Chap Test_4 {#sec-chap_1_Abc}
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Here is some more text
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# Introduction {#sec-chap_1_Intro}
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Here is some more text
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It does work when first the ids are defined like first: chap_1_Abc and then chap_1_Intro. In that case the chap_1_Abc is not able to be referenced
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Data/1_Writing/1_Task/4_CNMc.qmd
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for dynamical systems with a control term or a model parameter value $\beta$.
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In this subsection, a review of
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[@Max2021] shall be given with pointing out which parts need to be improved. In addition, some distinctions between the previous version of \gls{cnmc} and the most recent version are named.
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Further applied modifications are provided in chapter [-@sec-
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To avoid confusion between the \gls{cnmc} version described in this thesis and the prior \gls{cnmc} version, the old version will be referred to as *first CNMc*.
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*First CNMc* starts by defining a range of model parameter values
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for dynamical systems with a control term or a model parameter value $\beta$.
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In this subsection, a review of
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[@Max2021] shall be given with pointing out which parts need to be improved. In addition, some distinctions between the previous version of \gls{cnmc} and the most recent version are named.
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Further applied modifications are provided in chapter [-@sec-chap_2_Methodology].\newline
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To avoid confusion between the \gls{cnmc} version described in this thesis and the prior \gls{cnmc} version, the old version will be referred to as *first CNMc*.
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*First CNMc* starts by defining a range of model parameter values
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Data/1_Writing/2_Task/0_Methodlogy.qmd
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# Methodology {#sec-
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In this chapter, the entire pipeline for designing the proposed
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\gls{cnmc} is elaborated. For this purpose, the ideas behind
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the individual processes are explained.
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# Methodology {#sec-chap_2_Methodology}
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In this chapter, the entire pipeline for designing the proposed
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\gls{cnmc} is elaborated. For this purpose, the ideas behind
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the individual processes are explained.
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trials.qmd
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# Trials {
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{{< lof image.png >}}
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{{< downloadthis image.png >}}
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# Trials {#sec-chap_1_Test}
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In this work, a tool called \glsfirst{cnmc} is further developed.
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The overall goal, in very brief terms, is to generate a model, which is able to
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predict the trajectories of general dynamical systems. The model
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shall be capable of predicting the trajectories when a model parameter
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value is changed.
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Some basics about dynamical systems are covered in
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subsection [-@sec-subsec_1_1_1_Principles] and in-depth explanations about \gls{cnmc} are given in
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chapter [-@sec-chap_1_Test]. \newline
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chapter [-@sec-chap_2_Test]
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chapter [-@sec-chap_1_Test_2]
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chapter [-@sec-chap_1_Test_3]
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chapter [-@sec-chap_1_Intro]\newline
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Intra reference: [-@sec-chap_1_Intra]\newline
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Intro reference: [-@sec-chap_1_Intro]\newline
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chapter [-@sec-chap_1_Abc]\newline
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# Chap Test {#sec-chap_2_Test}
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Here is some more text
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# Chap Test_2 {#sec-chap_1_Test_2}
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Here is some more text
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# Chap Test_3 {#sec-chap_1_Test_3}
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Here is some more text
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Further check [@sec-chap_1_Intro] -- is found now (able to resolve crossref)
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chapter [-@sec-chap_1_Abc] -- now this becomes the issue (will not be found anymore)
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{{< lof image.png >}}
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{{< downloadthis image.png >}}
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