# Application of a three-dimensional fiber lay-down model to non-woven production processes

- Martin Grothaus
^{1}, - Axel Klar
^{1, 2}, - Johannes Maringer
^{1}Email author, - Patrik Stilgenbauer
^{1}and - Raimund Wegener
^{2}

**4**:4

**DOI: **10.1186/2190-5983-4-4

© Grothaus et al.; licensee Springer. 2014

**Received: **7 May 2012

**Accepted: **19 March 2014

**Published: **3 June 2014

## Abstract

In this work we present the industrial application of fiber lay-down models that enable an efficient simulation of non-woven structures. The models describe the deposition of fibers on a moving conveyor belt with the help of stochastic differential equations on manifolds. The model parameters have to be estimated from more complex models in combination with measurements of the resulting non-woven. In the application we discuss especially a three-dimensional fiber model for a typical industrial problem from non-woven production processes.

### Keywords

fiber lay-down stochastic differential equations on manifolds parameter identification## 1 Introduction

Since the mathematical treatment of the whole process at a stroke is not possible due to its complexity, a hierarchy of models that adequately describe partial aspects of the process chain has been developed in research during the last years. In [1] the conjunction of those models has been elaborated using asymptotic analysis, similarity estimates and parameter identification. More precisely, the description of the fiber dynamics in turbulent air flows has been realized by a stochastic generalized string model that has been deduced from a special Cosserat rod under Kirchhoff constraint, consult [2, 3] for its derivation. This provides the basis for the software tool FIDYST^{a} that enables the full simulation of fiber motion under the influence of surrounding turbulent air flows up to the fiber lay-down on the transport belt. In this manner, the microstructure of virtual fiber webs can be in principle generated. However, this approach is computationally expensive and the complexity is strongly affected by the number of fibers. For this reason, a class of stochastic surrogate models has been proposed in order to compute only the image of the deposited fiber web, instead of describing the full fiber dynamics that lead to this web. These surrogate models have in common the structure of a system of ordinary stochastic differential equations that enables the fast computation of a considerable number of fibers. They contain parameters that are related to the physical production process, as for example turbulence influence and fiber coiling, and that have to be identified from the full simulation of a few fibers with help of the complex string model. Based on the original two-dimensional version in [4], the surrogate models have been frequently improved within the last years. This includes the addition of a moving conveyor belt [5] or, more general, the consideration of more specific types of production processes as for instance rotational spinning processes [1]. Further enhancements are given by a smooth version in [6] where the curvatures of the fibers are taken into account, and by modelling the lay-down in three dimensions [7, 8]. The latter has been intended as first step into a realistic generation of three-dimensional microstructures that can be used for study of flow resistance and elasticity of the non-woven. The mathematical analysis of these models is sophisticated due to degeneracies of the associated Fokker-Planck equations. The trend to equilibrium for the original two-dimensional model has been investigated using Dirichlet forms and operator semi-group techniques in [9], with a hypocoercivity method in [10] and with probabilistic methods in [11–13]. The higher-dimensional models have been accordingly analyzed in [13, 14]. With the help of various techniques from asymptotic analysis connections between these models have been shown and model reduction in the situation of large or small turbulence have been performed in [4–8]. A possible strategy for estimating the parameters of the two-dimensional models has been provided as a heuristic approach in [1] which has been successfully tested by FIDYST simulations of transversal as well as rotational spinning processes in the stated source. In [7] an extension of this identification strategy to the three-dimensional case has been proposed on condition that information about the fiber orientation is available. In this work we realize this approach in a real industrial problem for the first time. At the example of a pilot plant of the company Oerlikon Neumag, we discuss the calibration of the smooth three-dimensional surrogate model and illustrate the computation of corresponding fiber webs. For this we need both the full simulation of a few representative fibers with regard to the problem setting and image processing data from CT-scans of the resulting non-woven.

This paper is structured as follows. At first, we recapitulate the class of surrogate fiber lay-down models developed in the above mentioned papers. This is done in Section 2 where we use a description that can be embedded in the context of geometric Langevin equations on regular submanifolds as investigated in [15]. Via this approach, the highly geometric nature of the class of fiber lay-down models is illustrated.

In Section 3 we describe a strategy for estimating the parameters of the surrogate models. The application of the models to the production process in the pilot plant is done in Section 4 where we are able to simulate virtual fiber webs that are numerically investigated with regard to their quality characteristics.

## 2 The fiber lay-down models

As mentioned in the Introduction, in this section we recapitulate the class of surrogate models developed in [1, 7, 8, 13, 15]. In the surrogate fiber lay-down models the paths of the deposited fibers (as images of arc-length parametrized curves) are described by simplified stochastic differential equations. For this purpose, distinctive process parameters that influence the form of the fiber web are incorporated. These are the typical throwing ranges of the fibers and their coiling behavior, whereas the deposition itself is perturbed by some random force which is affected by the entanglement of the fibers above the lay-down region. Other characteristics involve the fiber stiffness and the fiber orientation in space. Additionally, depending on the production process, different specifications can be handled using appropriate reference curves. In this work we restrict ourselves on the situation of a transversal spinning process, that means the fiber lay-down starting from fixed spinning positions onto a straight moving conveyor belt. Therein the belt velocity as well as the spinning speed are predetermined parameters given by the production process. The other parameters have to be appropriately estimated, see Section 3.

**W**denotes a

*d*-dimensional standard Brownian motion. For more details on manifold-valued stochastic differential equations, see e.g. [16]. Here the arc-length parametrized curve $\mathit{\xi}:{\mathbb{R}}_{0}^{+}\to {\mathbb{R}}^{d}$ represents one deposited fiber. ξ is really arc-length parametrized since ω lives on ${\mathbb{S}}^{d-1}$, compare Figure 2. The drift term in the second equation models the coiling behavior of the fiber, where $\mathrm{\Pi}[\mathit{\omega}]:=I-\mathit{\omega}\otimes \mathit{\omega}$ denotes the projection of the tangent onto the sphere ${\mathbb{S}}^{d-1}$ with

*I*the identity matrix and $x\otimes y=x{y}^{T}$. The throwing ranges of the fiber can be controlled with the help of a suitable potential

*V*. The second term in the equation for ω describes a Brownian motion on ${\mathbb{S}}^{d-1}$ with constant noise amplitude $A\in {\mathbb{R}}_{0}^{+}$ and expresses the stochastic forces, i.e. the effect of the turbulent air flows that perturb the deposition of the fibers as desired. We remark that the basic model (1) can also be viewed as a geometric Langevin equation having spherical velocities, see [15].

Therein, the parameter $\mu \in {\mathbb{R}}_{0}^{+}$ takes on the role of the noise amplitude, whereas the stiffness of the fibers can be related to $\lambda \in {\mathbb{R}}_{0}^{+}$. The connection to (1) is given by the white noise limit (compare [7]), i.e. the basic model can be viewed as a model for non-stiff fibers.

and the spherical unit vectors ${\mathbf{n}}_{i}$ are given by ${\mathbf{n}}_{i}:=\frac{1}{|{\partial}_{{\theta}_{i}}\mathit{\tau}|}{\partial}_{{\theta}_{i}}\mathit{\tau}$. So note that the parameters take values in $\mathit{\theta}\in \mathbb{R}/2\pi \mathbb{Z}\times {(0,\pi )}^{d-2}$ (or in $\mathbb{R}/2\pi \mathbb{Z}$ in case $d=2$) and $\mathit{\kappa}\in {\mathbb{R}}^{d-1}$ respectively.

with some finite constant $C>0$. Here the empty product is again equal to 1 in case $d=2$. In the basic case we obtain the stationary distribution by integrating (5) over κ.

Now that we have the abstract framework available, we recur to the application point of view and look at the essential cases $d=2$ and $d=3$ more closely.

### 2.1 The 2D model

A virtual fiber web can now be simulated by simultaneous use of this model for a large number of fibers, neglecting the influence of fiber-fiber-contact. The reference points indicating different spinning nozzles are included by adding an appropriate constant to the ${\mathit{\xi}}_{t}$-process. Using this 2D model, for example, the basis weight distribution of the non-woven can straightforwardly be determined assuming a uniform thickness of the fibers.

This is a natural smoother version of (6). See also [6] for a similar model.

gives the deviation of the fiber from a reference point determined by the position of the corresponding spinning nozzle, where $v=\frac{{v}_{\mathrm{belt}}}{{v}_{\mathrm{in}}}\ge 0$ defines the ratio between belt speed and spinning speed of the fiber, see [1]. The image of the fiber on the belt, denoted by ${({\mathit{\eta}}_{t})}_{t\ge 0}$, is then obtained by ${\mathit{\eta}}_{t}={\mathit{\xi}}_{t}-vt{\mathbf{e}}_{1}$. Unfortunately, there is no explicit computable stationary state available in case $v>0$. For a non-moving conveyor belt ($v=0$) the equilibrium is given by (5).

### 2.2 The 3D model

*θ*-distribution. The stationary solution of (9) is given by

*B*to facilitate the reading. The equilibrium state for the basic model (8) is obtained by integrating (10) over the curvatures $({\kappa}_{1},{\kappa}_{2})$. Again the moving conveyor belt can be incorporated via

## 3 Parameter estimation

*v*, we need estimations of the parameters

*μ*,

*λ*and

*B*as well as the shape of the potential

*V*. We use a potential of the following form

*B*is obtained from CT-scans. For the following considerations, we suppose that the reference curve $\mathit{\gamma}=-v{\mathbf{e}}_{1}t$ is known and that the deviation process $\mathit{\xi}=\mathit{\eta}-\mathit{\gamma}$ is centered in the origin. At first, we dedicate ourselves to the afore-mentioned heuristic approach from [1] that enables the estimation of the 2D parameters. The advantage of this method lies in the use of the characteristic parameters that are actually observable in the process. Since the subsequently defined functional is closely related to the parameter space, the identification algorithm is very robust. An alternative method in the context of fiber lay-down models using occupation times can be find in [20]. For more systematic approaches we refer to [21, 22]. Let $\mathcal{D}=({\mathbf{D}}_{1},\dots ,{\mathbf{D}}_{N})\in {({\mathbb{R}}^{2}\times \mathbb{R}\times \mathbb{R})}^{N}$ with ${\mathbf{D}}_{i}=({\mathit{\eta}}_{{t}_{i}},{\alpha}_{{t}_{i}},{\kappa}_{{t}_{i}})$, $1\le i\le N$, be a set of data points obtained from a FIDYST simulation. Here an equidistant time grid with $\mathrm{\u25b3}t={t}_{i+1}-{t}_{i}$ is used. The angles ${\alpha}_{{t}_{i}}$ and curvatures ${\kappa}_{{t}_{i}}$ are reconstructed from the fiber points ${\mathit{\eta}}_{{t}_{i}}$ by finite difference approximations. We note that in [1] the emphasis is on the calibration of the model from [6], whereas we want to work with the smooth model (7) here. Therefore, with ${\mathit{\xi}}_{t}=({\xi}_{t,1},{\xi}_{t,2})$, we consider a slightly different functional of characteristic properties than stated in [1]:

where ${\mathcal{D}}_{\mathrm{fid}}$ indicates the data sample obtained from a FIDYST simulation. This can be solved by a relaxated quasi Newton method with unit Jacobian, i.e. ${\mathbf{P}}^{(n+1)}={\mathbf{P}}^{(n)}+\omega [\mathcal{F}({\mathcal{D}}_{\mathrm{sur}}({\mathbf{P}}^{(n)}))-\mathcal{F}({\mathcal{D}}_{\mathrm{fid}})]$ and starting point ${\mathbf{P}}^{(0)}=\mathcal{F}({\mathcal{D}}_{\mathrm{fid}})$, compare [1]. We note that
is a very good estimator for **P**, if the fiber process is close to its stationary state (5) with $d=2$, i.e. for adequately large data sample and small speed ratio *v*, two conditions which are usually fulfilled in the production processes considered here. It is worth mentioning that this choice of
is completely detached from the white noise limit situation and can therefore be used for larger ranges of applications compared to [1].

*μ*m, which is about an order of magnitude smaller than a typical fiber diameter, see Table 1. The CT-scan provides a real-valued three-dimensional matrix with so-called gray values. These raw image data are edited by image processing, which translates them into local fiber directions at each pixel with the help of an eigenvalue analysis of the Hessian matrix of the second partial derivatives of the gray values, for more details consult [23]. In other words, the image processing data (IPD) yield spherical polar angles that determine the orientation of the tangents at the fiber points. With these we generate the corresponding density distribution ${\stackrel{\u02d8}{p}}^{(CT)}(\alpha ,\theta )$ with $(\alpha ,\theta )\in \stackrel{\u02d8}{U}=\mathbb{R}/2\pi \mathbb{Z}\times (0,\frac{\pi}{2}]$. The restriction to the hemisphere is obligatory, since the data of the CT-scan do not reveal the temporal course of the (undistinguishable) fiber paths. Thus the tangents contain no more than an unsigned directional information. Therefore, the density ${\stackrel{\u02d8}{p}}^{(CT)}(\alpha ,\theta )$ has to be distinguished from the (unknown) angular density distribution obtained by our model (9) with moving conveyor belt, in the following denoted by ${p}^{(M)}(\alpha ,\theta )$ with $(\alpha ,\theta )\in U=\mathbb{R}/2\pi \mathbb{Z}\times (0,\pi )$. The latter can be convert to the hemisphere via

**Predetermined parameters by the pilot plant and size of data samples**

Predetermined | FIDYST | IPD | ||||
---|---|---|---|---|---|---|

${\mathit{v}}_{\mathbf{belt}}\phantom{\rule{0.25em}{0ex}}\mathbf{[}\mathbf{m}\mathbf{/}\mathbf{s}\mathbf{]}$ | ${\mathit{v}}_{\mathbf{spin}}\phantom{\rule{0.25em}{0ex}}\mathbf{[}\mathbf{m}\mathbf{/}\mathbf{s}\mathbf{]}$ | ${\mathit{f}}_{\mathbf{diam}}\phantom{\rule{0.25em}{0ex}}\mathbf{[}\mathbf{m}\mathbf{]}$ | △t [m] | # points | # points | |

Sample | 0.633 | 79.400 | 12⋅10 | 0.001 | 13×19,850 | 4,352,392 |

Sample | 4.167 | 79.400 | 12⋅10 | 0.001 | 13×17,850 | 500,583 |

Assuming that the fiber lay-down process is close to equilibrium, or in other words, if *v* is sufficiently small, we can identify the parameter *B* without great effort. In that case, we demand the equality of the standard deviation ${\sigma}_{B}$ of the *θ*-marginal of the distribution function obtained from the CT-scan, denoted by ${\stackrel{\u02d8}{p}}_{\theta}^{(CT)}$, and the explicitly computed standard deviation ${\overline{\sigma}}_{B}$ of the *θ*-marginal of the stationary distribution (10) of our model (with $v=0$). The latter reads ${\overline{\sigma}}_{B}={({\int}_{0}^{\pi}{C}_{B}{(sin\theta )}^{\frac{1}{B}}{(\theta -\frac{\pi}{2})}^{2}\phantom{\rule{0.2em}{0ex}}\mathrm{d}\theta )}^{\frac{1}{2}}$ with normalization constant ${C}_{B}^{-1}={\int}_{0}^{\pi}{(sin\theta )}^{\frac{1}{B}}\phantom{\rule{0.2em}{0ex}}\mathrm{d}\theta $. Besides, the influence of the belt speed on the size of *B* is expected to be small in contrast to the other parameters, since it involves the deviation from the planar structure. In the case of very large *v*, the estimation of *B* can be straightforwardly embedded in the above heuristic identification approach with a little more effort. For our purposes, however, the described identification strategy will turn out to be adequate anyway.

## 4 Application

In the following we want to demonstrate the adaptation of the surrogate models on the basis of a industrial test case describing a real non-woven production process. From a pilot plant of the company Oerlikon Neumag process data have been available that have been used to initialize FIDYST simulations of the full process. Plant specific parameters, such as machine geometry and prevailing air flows have been included in these computations. In addition, an associated non-woven product has been produced by the pilot plant with the same configuration data. Pieces of this non-woven have been cut and have been analyzed in CT-scans. The statistics of the fiber orientation in the non-woven given as image processing data (IPD) complement the FIDYST informations as described in the previous chapter.

*I*and sample

*II*. Associated characteristic values and data sizes are summarized in Table 1. The resolution of FIDYST is something to be viewed critically. A more accurate resolution increases the effort and leads to unreasonable computational costs, compare Chapter 1. At least the surrogate models use the same grid sizes and they can be viewed as optimal discrete substitutes for FIDYST, see also below. The different numbers of IPD points indicate a different usable sample size of the pieces of nonwoven. A larger number of points leads to smoother

*α*-marginals ${\stackrel{\u02d8}{p}}_{\alpha}^{(CT)}(\alpha ,\theta )$, compare Figures 8, 9, otherwise, it is not relevant. The essential difference between the two samples is the belt speed. Nevertheless, the speed ratio

*v*is sufficiently small in both cases, which can be ascertained by the comparison between the standard deviation ${\overline{\sigma}}_{B}$ and the one of our model with given

*v*using Monte-Carlo simulations. Thus the calibration of the surrogate model (9) is carried out as described above. The estimated parameters are summarized in Table 2. In Figures 10-13 we illustrate a comparison of fibers computed by FIDYST and the calibrated 2D model (7) with moving transport belt. Qualitatively the same fiber lay-down structures are observed. The parameter

*B*is identified from the CT-scans data as outlined above. This leads to

*θ*-marginal distributions as in Figures 14, 15.

**Identified parameters to be used in the surrogate model**

${\mathit{\sigma}}_{\mathbf{1}}\phantom{\rule{0.25em}{0ex}}\mathbf{[}\mathbf{m}\mathbf{]}$ | ${\mathit{\sigma}}_{\mathbf{2}}\phantom{\rule{0.25em}{0ex}}\mathbf{[}\mathbf{m}\mathbf{]}$ | $\mathit{\mu}\phantom{\rule{0.25em}{0ex}}\mathbf{[}{\mathbf{m}}^{\mathbf{-}\mathbf{3}\mathbf{/}\mathbf{2}}\mathbf{]}$ | $\mathit{\lambda}\phantom{\rule{0.25em}{0ex}}\mathbf{[}{\mathbf{m}}^{\mathbf{-}\mathbf{1}}\mathbf{]}$ | B | v | |
---|---|---|---|---|---|---|

Sample | 0.0050 | 0.0049 | 49,096 | 1,039 | 0.398 | 0.0080 |

Sample | 0.0055 | 0.0045 | 49,885 | 997 | 0.375 | 0.0525 |

Furthermore, in Figures 8, 9 we compare the *α*-marginal ${\stackrel{\u02d8}{p}}_{\alpha}^{(CT)}(\alpha ,\theta )$ of the CT-scan data with the corresponding distributions obtained from FIDYST simulations ${\stackrel{\u02d8}{p}}_{\alpha}^{({M}_{F})}(\alpha ,\theta )$ and from the surrogate models ${\stackrel{\u02d8}{p}}_{\alpha}^{({M}_{2d})}(\alpha ,\theta )$ and ${\stackrel{\u02d8}{p}}_{\alpha}^{({M}_{3d})}(\alpha ,\theta )$, which can be computed with the help of (11), (where $\theta =\pi /2$ is fixed for ${p}^{({M}_{F})}$ and ${p}^{({M}_{2d})}$). It seems conspicious, that the large amplitude in the CT-scans is not reached by the models. On the contrary, both FIDYST and the surrogate models (7) and (9) show an almost uniform distribution, which is not surprising because of the very small speed ratio. Indeed, the surrogate models show the same quantitative behavior as the FIDYST simulation.

This discrepancy between the CT-scan measurements and the models with respect to the *α*-distribution might be explained by the fact that the CT-scan has analyzed pieces of non-woven that had already passed through several process steps of reworking and reinforcement which had influenced the angular distribution. On the contrary, both, FIDYST and the surrogate fiber lay-down models have described the texture before post-processing. To investigate this issue more closely, it would be of great interest to have CT-scans of the deposited fibers without effects due to post-processing.

*V*. Unfortunately, it is technically impossible to get at this parameter. We can only estimate in terms of the fiber diameter ${f}_{\mathrm{diam}}$. Exemplary simulations for the two samples with a presumed non-woven thickness ${d}_{f}=200{f}_{\mathrm{diam}}$ are shown in Figures 16-21. To compare the quality of the resulting fiber webs, we investigate the homogeneity more closely. As is common in the practical application, we look at the basis weight distribution. For this purpose, a 2D grid is placed over a fixed area of the simulated fiber web (projected to 2D) and the basis weight of each cell is numerically determined. This weight

*M*of a given cell is proportional to the time the fiber process is present in that cell. In Figures 22-27 the relative deviations $\frac{|E[M]-M|}{E[M]}$ between the (expected) averaged and the actual basis weight in the cells are illustrated for different grid sizes. The standard deviations of these values give the corresponding coefficients of variation (

*CV*-values) which are summarized in Table 3. As specimen we choose a square of size 100 cm

^{2}for each sample. Due to the respective smaller

*CV*-values we can state that the simulated fiber web associated to sample

*I*is more homogeneous than the one given by sample

*II*and hence better quality characteristics of nonwovens are expected for the machine configuration of sample

*I*, i.e. for a slower conveyor belt. Due to the different belt speed, however, the basis weight with respect to sample

*II*is six times smaller compared to sample

*I*.

**Basis weight distribution in terms of CV-values (in %) of the simulated fiber webs**

Grid | |||
---|---|---|---|

32 × 32 | 64 × 64 | 128 × 128 | |

Sample | 16.4 | 18.9 | 22.6 |

Sample | 31.8 | 38.9 | 49.1 |

## 5 Conclusion and outlook

We presented the application of a 3D surrogate fiber lay-down model to an industrial problem. The parameters are identified on the basis of experimental data. The calibrated model enables the efficient simulation of a whole virtual fiber web. Further modifications of the model will include, for example, the impenetrability of the fibers. This is examined in further studies. To predict material properties like permeability of the textile, the geometric model presented here has to be used as a basic model for a complex flow simulation to determine macroscopic properties of the textile.

## Endnote

FIDYST: **Fi** ber **Dy** namics **S** imulation **T** ool developed at Fraunhofer ITWM, Kaiserslautern.

## Declarations

### Acknowledgements

This work has been supported by Bundesministerium für Bildung und Forschung (BMBF), Verbundprojekt ProFil, 03MS606. Moreover, we thank the colleagues from the departments Transport Processes and Image Processing at Fraunhofer ITWM.

## Authors’ Affiliations

## References

- Klar A, Marheineke N, Wegener R:
**Hierarchy of mathematical models for production processes of technical textiles.***Z Angew Math Mech*2009,**89**(12):941–961. 10.1002/zamm.200900282MATHMathSciNetView ArticleGoogle Scholar - Marheineke N, Wegener R:
**Fiber dynamics in turbulent flows: general modeling framework.***SIAM J Appl Math*2006,**66**(5):1703–1726. 10.1137/050637182MATHMathSciNetView ArticleGoogle Scholar - Marheineke N, Wegener R:
**Modeling and application of a stochastic drag for fibers in turbulent flows.***Int J Multiph Flow*2011,**37:**136–148. 10.1016/j.ijmultiphaseflow.2010.10.001View ArticleGoogle Scholar - Götz T, Klar A, Marheineke N, Wegener R:
**A stochastic model and associated Fokker-Planck equation for the fiber lay-down process in nonwoven production processes.***SIAM J Appl Math*2007,**67**(6):1704–1717. 10.1137/06067715XMATHMathSciNetView ArticleGoogle Scholar - Bonilla LL, Götz T, Klar A, Marheineke N, Wegener R:
**Hydrodynamic limit of a Fokker-Planck equation describing fiber lay-down processes.***SIAM J Appl Math*2007/08,**68**(3):648–665.MathSciNetView ArticleGoogle Scholar - Herty M, Klar A, Motsch S, Olawsky F:
**A smooth model for fiber lay-down processes and its diffusion approximations.***Kinet Relat Models*2009,**2**(3):489–502.MATHMathSciNetView ArticleGoogle Scholar - Klar A, Maringer J, Wegener R:
**A smooth 3D model for fiber lay-down in nonwoven production processes.***Kinet Relat Models*2012,**5:**97–112.MATHMathSciNetView ArticleGoogle Scholar - Klar A, Maringer J, Wegener R:
**A 3D model for fiber lay-down in nonwoven production processes.***Math Models Methods Appl Sci*2012.,**22**(9): Article ID 1250020 Article ID 1250020 - Grothaus M, Klar A:
**Ergodicity and rate of convergence for a nonsectorial fiber lay-down process.***SIAM J Math Anal*2008,**40**(3):968–983. 10.1137/070697173MATHMathSciNetView ArticleGoogle Scholar - Dolbeault J, Klar A, Mouhot C, Schmeiser C:
**Exponential rate of convergence to equilibrium for a model describing fiber lay-down processes.***Appl Math Res Express*2012. 10.1093/amrx/abs015Google Scholar - Kolb M, Savov M, Wübker A:
**(Non-)ergodicity of a degenerate diffusion modeling the fiber lay down process.***SIAM J Math Anal*2013,**45:**1–13. 10.1137/120870724MATHMathSciNetView ArticleGoogle Scholar - Kolb M, Savov M, Wübker A: Geometric ergodicity of a hypoelliptic diffusion modelling the melt-spinning process of nonwoven materials; 2012 http://arxiv.org/abs/arXiv:1112.6159
- Grothaus M, Klar A, Maringer J, Stilgenbauer P: Geometry, mixing properties and hypocoercivity of a degenerate diffusion arising in technical textile industry; 2012 http://arxiv.org/abs/arXiv:1203.4502
- Grothaus M, Stilgenbauer P: Hypocoercivity for Kolmogorov backward evolution equations and applications; 2012 http://arxiv.org/abs/arXiv:1207.5447
- Grothaus M, Stilgenbauer P:
**Geometric Langevin equations on submanifolds and applications to the stochastic melt-spinning process of nonwovens and biology.***Stoch Dyn*2013.,**13**(4): Article ID 1350001 Article ID 1350001 - Hsu EP
**Graduate Studies in Mathematics.**In*Stochastic Analysis on Manifolds*. Am. Math. Soc., Providence; 2002.View ArticleGoogle Scholar - Hietel D, Wegener R:
**Simulation of spinning and lay-down processes.***Tech Text*2005,**3:**145–148.Google Scholar - Hearle J, Sultan M, Govender S:
**The form taken by threads laid on a moving belt.***J Text Inst*1976,**67:**373–386. 10.1080/00405007608630170View ArticleGoogle Scholar - Mahadevan L, Keller J:
**Coiling of flexible ropes.***Proc R Soc Lond A*1996,**452**(1950):1679–1694. 10.1098/rspa.1996.0089MATHMathSciNetView ArticleGoogle Scholar - arXiv: http://arxiv.org/abs/arXiv:1112.3550 Bock W, Götz T, Liyanage P: Parameter estimation of fiber lay-down in nonwoven production - an occupation time approach; 2011 [arXiv:1112.3550]
- Kutoyants YA
**Springer Series in Statistics.**In*Statistical Inference for Ergodic Diffusion Processes*. Springer, London; 2004.View ArticleGoogle Scholar - Gobet E, Hoffmann M, Reiß M:
**Nonparametric estimation of scalar diffusions based on low frequency data.***Ann Stat*2004,**32**(5):2223–2253. 10.1214/009053604000000797MATHView ArticleGoogle Scholar - Redenbach C, Rack A, Schladitz K, Wirjadi O, Godehardt M:
**Beyond imaging: on the quantitative analysis of tomographic volume data.***Int J Mater Res*2012,**2:**217–227.View ArticleGoogle Scholar

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