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Seminar on Computational Engineering 19.4.2001 by Jukka-Pekka Onnela
Variational Methods Seminar on Computational Engineering by Jukka-Pekka Onnela
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Variational Methods Brief history of calculus of variations
Variational calculus: Euler’s equation Derivation of the equation Example Lagrangian mechanics Generalised co-ordinates and Lagrange’s equation Examples Soap bubbles and the Plateau Problem
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Brief History of Calculus of Variations
Calculus of variations: A branch of mathematics concerned with the problem of finding a function for which the value of a certain integral is either the largest or the smallest possible Calculus: from Latin calx for stone; used as pebbles or beads on the countingboard and abacus; to calculate Isoperimetric problem known to Greek mathematicians in the 2nd century BC Euler developed a general method to find a function for which a given integral assumes a max or min value Introduced isoperimetric problems as a separate mathematical discipline: calculus of variations
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Variational Calculus: Euler’s Equation
We seek a function that minimises the distance between the two points Minimising Generally:
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Variational Calculus: Euler’s Equation
Introduce test function Required property Extremum at At extremum Differentiating
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Variational Calculus: Euler’s Equation
Integrating the second term by parts Noticing Gives By the fundamental lemma of calculus of variations we obtain Euler’s Equation
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Variational Calculus: Euler’s Equation
Example: Surface of revolution for a soap film Film minimises its area <=> minimises surface energy Infinitesimal area Total area
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Variational Calculus: Euler’s Equation
This function satisfies Derivatives Substituting Integrating Integrating again
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Variational Calculus: Euler’s Equation
Substituting Gives And finally
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Lagrangian Mechanics Incorporation of constraints as generalised co-ordinates Minimising the number of independent degrees of freedom
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Lagrangian Mechanics For conservative forces Lagrange’s equation can be derived as Lagrangian defined as kinetic energy - potential energy
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Lagrangian Mechanics Example 1: Pendulum
The generalised co-ordinate is Kinetic energy Potential energy Lagrangian Pendulum equation
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Lagrangian Mechanics Example 2: Bead on a Hoop
The generalised co-ordinate is Cartesian co-ordinates of the bead Velocities obtained by differentiation
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Lagrangian Mechanics Kinetic energy Lagrangian Evaluating
Simplifies to
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Soap Bubbles and The Plateau Problem
Physicist Joseph Plateau started experimenting with soap bubbles to examine their configurations - Plateau problem Accurately modelled by minimal surfaces Why bubbles are spherical? Poisson: Surface of separation between two media in equilibrium is the surface of constant mean curvature Pressure = [surface tension][mean curvature] => For bubbles and films the pressure on two sides of the surface is a constant function Soap film enclosing a space with pressure inside greater than outside => constant positive mean curvature Soap film spanning a wire frame => zero mean curvature
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Soap Bubbles and The Plateau Problem
Response to perturbations depends on the nature of extremum point: Local minimum => Film is stable and resists small perturbations Saddle point => Film is unstable and small perturbations decrease its surface area New configuration lower in energy and topologically different Example: Two coaxial circles
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Soap Bubbles and The Plateau Problem
Examples of minimal surfaces - Soap Bubbles!
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