this is for holding javascript data
Kiran Samudrala edited local states.tex
almost 10 years ago
Commit id: 995023f1f2c741ff51998ccc5cdbde63271d3949
deletions | additions
diff --git a/local states.tex b/local states.tex
index b847e93..1de067e 100644
--- a/local states.tex
+++ b/local states.tex
...
\begin{equation}
{^{1}\beta(x),^{2}\beta(x),...^{I}\beta(x)} = \sum_{H} \, m_{s}^{h} \chi_{s}(x) \chi^{h_{1}}(^{1}\beta(x)) \chi^{h_{2}}(^{2}\beta(x)) ... \chi^{h_{I}}(^{I}\beta(x))
\end{equation}
where $\chi^{h_{i}}(^{i}\beta(x))$ is that basis representation of the $i^{th}$ tuple of the local material state $^{i}\beta(x)$ . The local state index $h$ is uniquely mapped to (h_{1},h_{2},...h_{I}). It is expected that each local state space expressed by the microstructure function will require a different basis function. For example, if the local material state is expressed as a 3-tuple, $\{\rho, V, (\varphi_{1},\Phi,\varphi_{1})\}$, that corresponds to the discrete phase indicator of the material ($\rho$), the volume fraction of an element within a
phase, phase $\varphi$, and the grain orientation $V_{f}$, then a different basis function will be needed for each element.
Literature reports an extensive variety of basis functions.[ref] Fortunately, characteristics of the local state space inform the choice of basis functions for the
ith $i^{th}$ mode of the local state,
EQUATION. $\chi^{h}(^{i}\beta(x))$. The following list describes all of the possible characteristics of the local state spaces:
Discrete LSS – The local state is identified by a discrete index that demarcates a particular class of material features. For example in steel, a discrete basis will uniquely index different phases of steel (e.g. martensite, austenite, pearlite). Indicator basis functions can suite this application.
Bounded, Periodic LSS – The local states on opposite boundaries exhibit similar material behavior(this sentence stinks). A local state space that identifies the angle of a material feature over [0,2π] is periodic. The cosine transform provides a basis for this type of local state space. Some new work will show an application of generalized spherical harmonics to grain orientation.
Bounded, Non-periodic LSS – I need help with this description. Legendre polynomials are an example of a basis function for this application. Volume fraction is the example here.