![Page 1: ME 680 Introduction to Bifurcation and Chaos (Spring 2004) Notes... · 1 Introduction to Bifurcation and Chaos Anil K. Bajaj School of Mechanical Engineering Office: Room ME 2007A](https://reader035.vdocuments.us/reader035/viewer/2022071008/5fc685b84a25ab1d367b06f0/html5/thumbnails/1.jpg)
1
Introduction to Bifurcation and
Chaos
Anil K. Bajaj
School of Mechanical Engineering
Office: Room ME 2007A
Tel: 494-5688
Email: [email protected]
ME 680- Spring 2014
![Page 2: ME 680 Introduction to Bifurcation and Chaos (Spring 2004) Notes... · 1 Introduction to Bifurcation and Chaos Anil K. Bajaj School of Mechanical Engineering Office: Room ME 2007A](https://reader035.vdocuments.us/reader035/viewer/2022071008/5fc685b84a25ab1d367b06f0/html5/thumbnails/2.jpg)
2
Troger, H. and Steindl, A.: Nonlinear
Stability and Bifurcation Theory: An
Introduction for Scientists and Engineers,
Springer-Verlag, Wein, 1991.
+
Class Notes
Text Book
![Page 3: ME 680 Introduction to Bifurcation and Chaos (Spring 2004) Notes... · 1 Introduction to Bifurcation and Chaos Anil K. Bajaj School of Mechanical Engineering Office: Room ME 2007A](https://reader035.vdocuments.us/reader035/viewer/2022071008/5fc685b84a25ab1d367b06f0/html5/thumbnails/3.jpg)
3
Course grade will be based on:
(i) some home assignments;
(ii) seminar presentations prepared on the
basis of assigned topics from literature;
(iii) project.
Grading
![Page 4: ME 680 Introduction to Bifurcation and Chaos (Spring 2004) Notes... · 1 Introduction to Bifurcation and Chaos Anil K. Bajaj School of Mechanical Engineering Office: Room ME 2007A](https://reader035.vdocuments.us/reader035/viewer/2022071008/5fc685b84a25ab1d367b06f0/html5/thumbnails/4.jpg)
4
Examples of nonlinear behavior in structural,
fluid-mechanical and chemical/biological
systems.
Introduction
![Page 5: ME 680 Introduction to Bifurcation and Chaos (Spring 2004) Notes... · 1 Introduction to Bifurcation and Chaos Anil K. Bajaj School of Mechanical Engineering Office: Room ME 2007A](https://reader035.vdocuments.us/reader035/viewer/2022071008/5fc685b84a25ab1d367b06f0/html5/thumbnails/5.jpg)
5
Consider two concentric
cylinders forming an
annulus – There is fluid in
the gap between the two
cylinders. The inner
cylinder rotates at a
constant rate . At slow
rates, the fluid undergoes
steady shearing motion.
1. Onset of wavy vortices in the finite-length Couette-Taylor
problem
Ref: W. S. Edwards, S. R. Beane, and S. Varma, Phys. Fluids A 3 (6). June 1991
![Page 6: ME 680 Introduction to Bifurcation and Chaos (Spring 2004) Notes... · 1 Introduction to Bifurcation and Chaos Anil K. Bajaj School of Mechanical Engineering Office: Room ME 2007A](https://reader035.vdocuments.us/reader035/viewer/2022071008/5fc685b84a25ab1d367b06f0/html5/thumbnails/6.jpg)
6
Onset of wavy vortices………
At some threshold value of , uniform pattern
becomes unstable and gives way to flow in the
form of cells along the axial direction. The cell
size (axial wave number) is ~ the gap width.
These are called Taylor cells.
![Page 7: ME 680 Introduction to Bifurcation and Chaos (Spring 2004) Notes... · 1 Introduction to Bifurcation and Chaos Anil K. Bajaj School of Mechanical Engineering Office: Room ME 2007A](https://reader035.vdocuments.us/reader035/viewer/2022071008/5fc685b84a25ab1d367b06f0/html5/thumbnails/7.jpg)
7
1. Onset of wavy vortices………
The streamlines of low
Taylor number T-C flow are
circular. This means that if
you were to insert a needle
with dye into the flow, the
dye would trace out a
circular path. If we view this
flow from a radial viewpoint,
we see the picture here.
Ref: http://www.princeton.edu/~gasdyn/Research/T-C_Research_Folder/Intro_to_T-C_Flows.html
![Page 8: ME 680 Introduction to Bifurcation and Chaos (Spring 2004) Notes... · 1 Introduction to Bifurcation and Chaos Anil K. Bajaj School of Mechanical Engineering Office: Room ME 2007A](https://reader035.vdocuments.us/reader035/viewer/2022071008/5fc685b84a25ab1d367b06f0/html5/thumbnails/8.jpg)
8
Onset of wavy vortices………
Once the flow becomes
unstable the picture
radically changes. The
flow becomes dominated
by toroidal Taylor
vortices. A cross
sectional view of
the flow field looks like:
![Page 9: ME 680 Introduction to Bifurcation and Chaos (Spring 2004) Notes... · 1 Introduction to Bifurcation and Chaos Anil K. Bajaj School of Mechanical Engineering Office: Room ME 2007A](https://reader035.vdocuments.us/reader035/viewer/2022071008/5fc685b84a25ab1d367b06f0/html5/thumbnails/9.jpg)
9
The figure illustrates
m=5 ‘wavy’ flow near
its onset – the
axisymmetric (Taylor)
flow with n=9 vortices
(cells) in the axial
direction becomes
unstable.
End effect is also
seen in the figure.
![Page 10: ME 680 Introduction to Bifurcation and Chaos (Spring 2004) Notes... · 1 Introduction to Bifurcation and Chaos Anil K. Bajaj School of Mechanical Engineering Office: Room ME 2007A](https://reader035.vdocuments.us/reader035/viewer/2022071008/5fc685b84a25ab1d367b06f0/html5/thumbnails/10.jpg)
10
2. Faraday Waves
Applying a vertical sinusoidal oscillation to a dish
of fluid effectively modulates the acceleration of
gravity seen by the fluid. If this modulation
exceeds a critical value, the normally flat state of
the free surface becomes unstable to the formation
of surface waves. These waves have a frequency
which is half that of the driving oscillations (the first
sub-harmonic). This effect was first reported by
Michael Faraday in 1831.
http://www.physics.utoronto.ca/nonlinear/
![Page 11: ME 680 Introduction to Bifurcation and Chaos (Spring 2004) Notes... · 1 Introduction to Bifurcation and Chaos Anil K. Bajaj School of Mechanical Engineering Office: Room ME 2007A](https://reader035.vdocuments.us/reader035/viewer/2022071008/5fc685b84a25ab1d367b06f0/html5/thumbnails/11.jpg)
11
2. Faraday Waves……..
In ordinary Newtonian fluids (those that do not
exhibit shear thickening or shear thinning) the
wave patterns include ones with 1-fold symmetry
(stripes), 2-fold symmetry (squares), 3-fold
symmetry (hexagons) as well as higher orders of
symmetry.
![Page 12: ME 680 Introduction to Bifurcation and Chaos (Spring 2004) Notes... · 1 Introduction to Bifurcation and Chaos Anil K. Bajaj School of Mechanical Engineering Office: Room ME 2007A](https://reader035.vdocuments.us/reader035/viewer/2022071008/5fc685b84a25ab1d367b06f0/html5/thumbnails/12.jpg)
12
2. Faraday Waves……..
Stripes, as viewed on surface Squares
patterns on the surface
![Page 13: ME 680 Introduction to Bifurcation and Chaos (Spring 2004) Notes... · 1 Introduction to Bifurcation and Chaos Anil K. Bajaj School of Mechanical Engineering Office: Room ME 2007A](https://reader035.vdocuments.us/reader035/viewer/2022071008/5fc685b84a25ab1d367b06f0/html5/thumbnails/13.jpg)
13
2. Faraday Waves……..
Hexagons Spirals (metastable)
![Page 14: ME 680 Introduction to Bifurcation and Chaos (Spring 2004) Notes... · 1 Introduction to Bifurcation and Chaos Anil K. Bajaj School of Mechanical Engineering Office: Room ME 2007A](https://reader035.vdocuments.us/reader035/viewer/2022071008/5fc685b84a25ab1d367b06f0/html5/thumbnails/14.jpg)
14
3. Rayleigh-Bénard and Bénard-Marangoni convection
In a horizontal fluid layer maintained at temperature
difference across it by heating from below and
cooling from above, the fluid flows in a pattern of
convection cells if the temperature difference
exceeds a threshold value. The fluid motion
transports additional heat over and above that
carried by thermal conduction through the fluid.
Many variations on this process have been studied
since Bénard's first experiments around the turn
of the 20th century.
Ref: http://www.physics.utoronto.ca/nonlinear/
![Page 15: ME 680 Introduction to Bifurcation and Chaos (Spring 2004) Notes... · 1 Introduction to Bifurcation and Chaos Anil K. Bajaj School of Mechanical Engineering Office: Room ME 2007A](https://reader035.vdocuments.us/reader035/viewer/2022071008/5fc685b84a25ab1d367b06f0/html5/thumbnails/15.jpg)
15
3. Rayleigh-Bénard……..
The fluid is confined between rigid plates held at
constant temperature. Lord Rayleigh showed
(1916) that an initially motionless fluid layer
becomes unstable to small flow perturbations when
the temperature difference is sufficiently large. The
flow pattern consists of rolls or hexagonal cells,
depending on the temperature dependence of the
fluid. The flow pattern may be stable, undergo
secondary instabilities or become chaotic.
![Page 16: ME 680 Introduction to Bifurcation and Chaos (Spring 2004) Notes... · 1 Introduction to Bifurcation and Chaos Anil K. Bajaj School of Mechanical Engineering Office: Room ME 2007A](https://reader035.vdocuments.us/reader035/viewer/2022071008/5fc685b84a25ab1d367b06f0/html5/thumbnails/16.jpg)
16
Mike Thompson and
Group, UCL, Center for
Nonlinear Dynamics
4. Hysteresis and Loop Formation
![Page 17: ME 680 Introduction to Bifurcation and Chaos (Spring 2004) Notes... · 1 Introduction to Bifurcation and Chaos Anil K. Bajaj School of Mechanical Engineering Office: Room ME 2007A](https://reader035.vdocuments.us/reader035/viewer/2022071008/5fc685b84a25ab1d367b06f0/html5/thumbnails/17.jpg)
17
5. Flow induced instabilities
Post-divergence
shape of the
rubber shell for
mode n=3.
a.Computed
shape for flow
velocity 30 m/s;
b.experimental
shape, from Ref. 7
Ref: A Amabili, Pellicani,
Paidoussis/J. Appl. Mech, 2001
![Page 18: ME 680 Introduction to Bifurcation and Chaos (Spring 2004) Notes... · 1 Introduction to Bifurcation and Chaos Anil K. Bajaj School of Mechanical Engineering Office: Room ME 2007A](https://reader035.vdocuments.us/reader035/viewer/2022071008/5fc685b84a25ab1d367b06f0/html5/thumbnails/18.jpg)
18
6. Buckling of rings under axial moments
Ref: F. Pai et al.
2001/U Missouri,
Columbia
![Page 19: ME 680 Introduction to Bifurcation and Chaos (Spring 2004) Notes... · 1 Introduction to Bifurcation and Chaos Anil K. Bajaj School of Mechanical Engineering Office: Room ME 2007A](https://reader035.vdocuments.us/reader035/viewer/2022071008/5fc685b84a25ab1d367b06f0/html5/thumbnails/19.jpg)
19
6. Buckling of rings under axial moments…….
![Page 20: ME 680 Introduction to Bifurcation and Chaos (Spring 2004) Notes... · 1 Introduction to Bifurcation and Chaos Anil K. Bajaj School of Mechanical Engineering Office: Room ME 2007A](https://reader035.vdocuments.us/reader035/viewer/2022071008/5fc685b84a25ab1d367b06f0/html5/thumbnails/20.jpg)
20
7. Break-up of a liquid jet
A series of
photographs showing
different stages of
fission that occur
when a pendant water
drop falls from a
circular plate.
Ref: Shi, Brenner and Nagel, Science, 256, 8 July 1994, 219-221.
![Page 21: ME 680 Introduction to Bifurcation and Chaos (Spring 2004) Notes... · 1 Introduction to Bifurcation and Chaos Anil K. Bajaj School of Mechanical Engineering Office: Room ME 2007A](https://reader035.vdocuments.us/reader035/viewer/2022071008/5fc685b84a25ab1d367b06f0/html5/thumbnails/21.jpg)
21
8. Patterns of complexity-1
Viscous journal
bearing flow: the flow
between two
periodically rotated
eccentric cylinders,
rotated in opposite
directions.
Ottino, Scientific Amer.,
260, Jan 1989, 56-67.
![Page 22: ME 680 Introduction to Bifurcation and Chaos (Spring 2004) Notes... · 1 Introduction to Bifurcation and Chaos Anil K. Bajaj School of Mechanical Engineering Office: Room ME 2007A](https://reader035.vdocuments.us/reader035/viewer/2022071008/5fc685b84a25ab1d367b06f0/html5/thumbnails/22.jpg)
22
9. Patterns of complexity-2
Rectangular cavity
flow with periodically
moving boundaries:
in a period, the upper
plate is moved to the
right, and then the
bottom plate is moved
to the left. Ref: Ottino, Scientific Amer.,
260, Jan 1989, 56-67.