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MotivationResearch ProblemNumerical Results
Future Plans and Expected ResultsSummary
Modelling of Web Dynamics in Paper Making
Process
Tytti Saksa
Department of Mathematical Information Technology
University of Jyväskylä
Postgraduate Seminar in Information Technology,November 28, 2011
Tytti Saksa Paper Web Dynamics
MotivationResearch ProblemNumerical Results
Future Plans and Expected ResultsSummary
Background and Current Status
Name: Tytti Saksa
Master's degree in Mathematics, December 2009
Postgraduate studies begun in January 2010
Status of the Ph.D. Thesis
Two years behind � two years ahead
Expected dissertation, December 2013
Format: collection of articles
Two articles published, two submitted
57 ECTS / 60 ECTS completed
Tytti Saksa Paper Web Dynamics
MotivationResearch ProblemNumerical Results
Future Plans and Expected ResultsSummary
Research Collaborators
Research group members
Lead by Prof. Pekka Neittaanmäki (supervisor)Prof. Nikolay Banichuk, RAS (2 one-month visits per year,supervisor)M.Sc. Juha JeronenM.Sc. Tero TuovinenM.Sc. Maria TirronenTech.Lic. Matti KurkiMe
Prof. Raino Mäkinen is also supervising my Ph.D. studies
Tytti Saksa Paper Web Dynamics
MotivationResearch ProblemNumerical Results
Future Plans and Expected ResultsSummary
Outline
1 Motivation
2 Research Problem
3 Numerical Results
4 Future Plans and Expected Results
Tytti Saksa Paper Web Dynamics
MotivationResearch ProblemNumerical Results
Future Plans and Expected ResultsSummary
MotivationAbout this presentation
Paper Making
Desire for high productivity and controlled machine running.
Press
nip
Dryer
section
Detail of a paper machine
Tytti Saksa Paper Web Dynamics
MotivationResearch ProblemNumerical Results
Future Plans and Expected ResultsSummary
MotivationAbout this presentation
Avoiding Web Breaks
Web breaks are expensive.
Non-productive machinerunning causes signi�canteconomic losses.
Tytti Saksa Paper Web Dynamics
MotivationResearch ProblemNumerical Results
Future Plans and Expected ResultsSummary
MotivationAbout this presentation
Original Research
This presentation is based on the following research:
Banichuk, Jeronen, Saksa and Tuovinen. Journal of StructuralMechanics (Rakenteiden mekaniikka). 44:172�185, 2011.
Tytti Saksa Paper Web Dynamics
MotivationResearch ProblemNumerical Results
Future Plans and Expected ResultsSummary
ModelObjectivesPhenomenon
Model
The travelling paper web ismodelled as a moving beam orpanel taking into account the(Earth's) gravity.
Panel: the webdisplacement does notvary in the cross directionto the movement.
V0 = web velocity, T =tension, g = the standardgravity, m = mass perunit area.
Tytti Saksa Paper Web Dynamics
MotivationResearch ProblemNumerical Results
Future Plans and Expected ResultsSummary
ModelObjectivesPhenomenon
Research Objectives in Figures
How fast can we run the traveling plate?
What is the shape of the buckled plate?
Tytti Saksa Paper Web Dynamics
MotivationResearch ProblemNumerical Results
Future Plans and Expected ResultsSummary
ModelObjectivesPhenomenon
Research Objectives in Words
Stability analysis of thin, elastic panels.
Critical conditions and critical velocity estimations.
E�ects of the gravity on the web behaviour and stability.
The e�ect of gravity has usually been neglected.
Tytti Saksa Paper Web Dynamics
MotivationResearch ProblemNumerical Results
Future Plans and Expected ResultsSummary
ModelObjectivesPhenomenon
The Governing Equations
The dynamic equation for the transversedisplacement w of the panel:
mwtt +2mV0wxt +mV 20 wxx = T wxx +Tx wx −Dwxxxx
Tension varies due to the gravity:
T (x) = T0 +mgx
Pinned (hinged) boundary conditions:w(0) = wxx(0) = 0, w(`) = wxx(`) = 0.
Tytti Saksa Paper Web Dynamics
MotivationResearch ProblemNumerical Results
Future Plans and Expected ResultsSummary
ModelObjectivesPhenomenon
Buckling Problem
Dimensionless static form of the buckling problem:
α wxxxx +(c20 −1−βx)wxx −β wx = 0 ,
w(0) = wxx(0) = 0 , w(1) = wxx(1) = 0 .
Energy:
α
∫ 1
0w2xx dx +(1− c20)
∫ 1
0w2x dx +β
∫ 1
0xw2
x dx = 0 .
Goal: to �nd the minimal (dimensionless) velocity c0 at whichthe energy equation (above) has a solution.
Tytti Saksa Paper Web Dynamics
MotivationResearch ProblemNumerical Results
Future Plans and Expected ResultsSummary
ModelObjectivesPhenomenon
Optimization Problem
First, the buckling problem is solved minimizing the energy:
Solve
(c∗0)2 = min
w∈K
(1+α
∫ 10 (wxx)
2 dx∫ 10 (wx)2 dx
+β
∫ 10 x (wx)
2 dx∫ 10 (wx)2 dx
),
whereK = {w ∈ C ([0,1]) : w(0) = 0 , w(1) = 0} .
Tytti Saksa Paper Web Dynamics
MotivationResearch ProblemNumerical Results
Future Plans and Expected ResultsSummary
ModelObjectivesPhenomenon
Estimations for the Critical Velocity
From the minimization problem on the previous slide, we may derivethe following analytical estimates for the critical buckling velocity
1+α π2 ≤ (c∗0)
2 ≤ 1+α π2 +
β
2.
The parameters (above) are de�ned as
c0 := V0/√T0/m ,
α :=D
`2T0, β :=
mg`
T0.
Tytti Saksa Paper Web Dynamics
MotivationResearch ProblemNumerical Results
Future Plans and Expected ResultsSummary
ModelObjectivesPhenomenon
Eigenvalue Problem
Secondly, the buckling problem is solved directly as an eigenvalueproblem:
α wxxxx −β (xwxx +wx) = λ wxx ,
w(0) = wxx(0) = 0 , w(1) = wxx(1) = 0 ,
whereλ := 1− c20
is the eigenvalue.
Goal: �nd the largest eigenvalue λ (corresponding to the minimalcritical velocity c0) of the eigenvalue problem.
Tytti Saksa Paper Web Dynamics
MotivationResearch ProblemNumerical Results
Future Plans and Expected ResultsSummary
Observations madeIllustrations
Overall Discussion
Two di�erent solution methods were presented and realizednumerically.
There was a very good agreement in the results given by theenergy minimization and the eigenvalue problem.
The optimization approach was found to be trusted.
The gravity had a large e�ect on the buckling mode, while thee�ect on the critical velocity was minor.
Tytti Saksa Paper Web Dynamics
MotivationResearch ProblemNumerical Results
Future Plans and Expected ResultsSummary
Observations madeIllustrations
Buckling Mode Dependence on the Band Angle to the
Gravity
! = 0! = " / 8
! = " / 4
! = 3 " / 8
! = " / 2
Tytti Saksa Paper Web Dynamics
MotivationResearch ProblemNumerical Results
Future Plans and Expected ResultsSummary
Observations madeIllustrations
E�ect of the Problem Parameters on the Critical Velocity
α corresponds to bending rigidity, β corresponds mass(assuming that the problem geometry does not change)
!
"
Critical velocity as fraction of sqrt(T0/m)
0 0.002 0.004 0.006 0.008 0.010
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1x 10
−5
1
1.0001
1.0002
1.0003
1.0004
1.0005
1.0006
1.0007
1.0008
1.0009
Tytti Saksa Paper Web Dynamics
MotivationResearch ProblemNumerical Results
Future Plans and Expected ResultsSummary
Future Plans
To continue studies on 1D viscoelastic model
one submitted paper, continuation to the work I presented inthis seminar in March 2011.
Optimization of the paper productivity
taking into account limitations in the web speed and growingof cracks at the web edges.
Tytti Saksa Paper Web Dynamics
MotivationResearch ProblemNumerical Results
Future Plans and Expected ResultsSummary
Expected Results
Basic research.
Increase the understanding of the physical phenomenon.
Real time simulations.
Direct application in paper making process.
About 5 journal papers.
Tytti Saksa Paper Web Dynamics
MotivationResearch ProblemNumerical Results
Future Plans and Expected ResultsSummary
Summary
Stability of thin, elastic panels (beams) travelling between twosupports was studied taking into account the e�ect of thegravity.
Analytical estimations for the critical velocities were found.
Energy minimization was found to be a reliable method forsolving this type of problems, but it was seen to be slowcompared to the (direct) eigenvalue problem solver.
The e�ect of the gravity on the buckling shapes was seen tobe large.
Tytti Saksa Paper Web Dynamics
MotivationResearch ProblemNumerical Results
Future Plans and Expected ResultsSummary
Thank You for Your Attention!
Tytti Saksa Paper Web Dynamics
Appendix For Further Reading
For Further Reading
N. Banichuk, J. Jeronen, M. Kurki, P. Neittaanmäki, T. Saksa and T.
Tuovinen.
On the limit velocity and buckling phenomena of axially moving
orthotropic membranes and plates.International Journal of Solids and Structures. 48:2015-2025, 2011.doi:10.1016/j.ijsolstr.2011.03.010.
T. Saksa.
Dynamic behaviour of an axially moving viscoelastic panel in contact with
supporting rollers.In Proceedings of ECCOMAS Thematic Conference on ComputationalAnalysis and Optimization. Eds. S. Repin, T. Tiihonen and T. Tuovinen.University of Jyväskylä, 2011.
N. Banichuk, J. Jeronen, T. Saksa and T. Tuovinen.
Static instability analysis of an elastic band travelling in the gravitational
�eld.
Journal of Structural Mechanics (Rakenteiden mekaniikka). 44:172�185,2011. Tytti Saksa Paper Web Dynamics