update
DESCRIPTION
Update. By Rob Chase and Pat Dragon Supervised by Robin Young. Given initial conditions and a system of PDEs, what happens?. The decoupled case can be modeled (u,v)t+(u+v,u-v)x=0 (u,v)t+(u,v)x=0 Decoupling is equivalent to finding the eigensystem. Recall. Shock Profiles u-x - PowerPoint PPT PresentationTRANSCRIPT
Given initial conditions and a system of PDEs, what happens?
The decoupled case can be modeled
(u,v)t+(u+v,u-v)x=0
(u,v)t+(u,v)x=0
Decoupling is equivalent to finding the eigensystem
RecallShock Profiles
u-x
Initial Conditions:
u = exp[-x^2]
As time goes on, burgur’s (backward) flux function the pulse will move to the right (left).
RecallState Space
u-v
Initial Conditions:u = exp[-x^2]v = exp[-x^2]
The Curve is a parametric function of x with one bell curve superimposed on the other as shock profiles.
State Space 2D t=.1
As the two pulses diverge (one going left, the other right), the curve billows out.
State Space 2D t=2
The shock “eats” information (whatever u,v symbolize) and very little is left over at the end.
The horizontal and vertical lines are where the shock profile has become overdefined.
The Riemann Problem
Given an initial state and a final state, can simple waves connect them?
RarefractionsCompressionsShocks
The curves found by integrating the eigenvectors represent a locus of states connected to the initial conditions.
P-System: The shock tube is immersed in water of constant temperature
ut + a*v^(-g)*x = 0 a, g constants
vt - ux = 0
0 p’(v)
-1 0
+/- c = Sqrt[-p’(v)]
(c,1) (-c,1)
Euler’s Full Gas Equations(holy grail)
pt + (pv)x = 0
(pv)t + (pv^2+P)x = 0
Et + (v(E+P))x = 0
The Elastic StringUt+Vx=0
Vt+T(U)x=0
Plane Solutions to Maxwell’s Equations
Lie Brackets of Eigenvectors
Definition:
[X,Y] = D[Y]X-D[X]Y
Frobeneous:
If [X,Y] = 0 Then the vectors define a surface