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Discrete equation
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aidan
Navier-Stokes Equations
Navier-Stokes Equations

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#1
Discrete equation
Stability of constant solutions

Investigate the stability of the constant solutions (u_{n+1} = u_n) of the discrete equation
u_{n+1} = 4u_n (1 - u_n)In the case 0 \le u_0 \le 1, use the substitution u_0 = \sin^2 \theta to find the general solution and verify your stability results. Can you find an explicit form of the general solution in the case u_0 > 1?
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PostPosted: Sun Nov 01, 2009 5:26 am  Back to top 
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J.Y.Choi
Poincare Conjecture
Poincare Conjecture

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#2
I want to type for you but I don't know how...(I'm a computer illiteracy, sorry.) It's about the logistic map. See the book [Mathematical Methods for Physicists] by Arfken.

Thinking graph of the function y = 4x(1 - x)and y=x will help.

PostPosted: Sun Nov 01, 2009 7:11 am  Back to top 
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Kent Merryfield
Birch & Swinnerton Dyer
Birch & Swinnerton Dyer

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#3
The interation u_{n+1}=f(u_n) can only possibly converge to a fixed point of the function, namely an x such that x=f(x).

Such a fixed point x is stable (all sequences starting sufficiently close to x converge to x) if an only if |f'(x)|<1. If |f'(x)|>1, then the fixed point x is unstable, and sequences that start very close to (but not exactly at) x do not remain very close to x.

(Point for which |f'(x)|=1 require more delicate analysis; I will not attempt such analysis below.)

The family of logistic mappings f(x)=rx(1-x) maps [0,1] into [0,1] as long as 0\le r\le 4.

Solving x=rx(1-x) gives us two roots: x=0 and x=1-\frac1r.

f'(x)=r for x=0 and f'(x)=2-r for x=1-\frac1r.

For 0\le x<1, the point x=0 is a stable fixed point and the point x=1-\frac1r does not lie in [0,1] and cannot be accessed by a sequence starting inside [0,1]. Hence, x=0 is the unique stable solution, and all sequences starting in [0,1] tend to zero.

For 1<x<3, the fixed point x=0 is unstable but the fixed point x=1-\frac1r is stable. All sequences starting in [0,1] tend to 1-\frac1r.

But for 3<x\le 4 (which includes the r=4 case that aidan is asking about), both the x=0 and x=1-\frac1r fixed points are unstable. Unless the sequence starts precisely at one of those fixed points, it will not converge.

The output of the following program (written in pseudo-code) is a famous picture.

Set up a [0,4]\times[0,1] window for plotting. (Or perhaps [3,4]\tiimes[0,1].)

Set up a loop, incrementing r by many very small steps from 0 to 4 (or perhaps from 3 to 4).

Let x: =\frac12.

Loop 250 times:

Let x: =rx(1-x).

For the first 50 iterations, plot nothing; for the next 200 iterations, plot a dot at (r,x).

End of loop.

End of loop on r.

PostPosted: Sun Nov 01, 2009 10:53 am  Back to top 
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aidan
Navier-Stokes Equations
Navier-Stokes Equations

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#4
Ah this is interesting - I've been reading a wikipedia article about the logistic map too. Thanks!
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PostPosted: Mon Nov 02, 2009 5:19 am  Back to top 
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