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multiple time scale dynamics with two fast variables and one slow ...

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from the evolution equations hold <strong>and</strong> then extend this procedure by com-<br />

pactness of B.<br />

• Step 5: This step provides the basic estimates to control the evolution of<br />

all 2-forms inside B. The estimates appear to be rather involved but the<br />

essential tool is just Gronwall’s Lemma.<br />

• Step 6: This step collects all the previous results <strong>and</strong> derives from estimates<br />

at q the final estimates at ¯q. This final part of the proof is subdivided into<br />

three parts. The first tracks M from q to Sǫ, the second follows M near Sǫ<br />

<strong>and</strong> the third deals <strong>with</strong> the exit from Sǫ towards ¯q. The overall patching<br />

strategy is the same as in Step 4.<br />

Step 1: We start <strong>with</strong> a remark on 2-forms in R 4 . Letσi for i=1, 2, 3, 4 be<br />

coordinates in R 4 . Observe that if P is a 2-plane then the natural first attempt<br />

to define how to evaluate a 2-form on P is to take <strong>two</strong> independent vectors<br />

that span P <strong>and</strong> then evaluate the 2-form on those vectors; this process is only<br />

defined up to a <strong>multiple</strong> as we can <strong>scale</strong> basis vectors inside P. To avoid this<br />

ambiguity consider a unit rectangle R of P <strong>and</strong> evaluate the form on the vectors<br />

spanning it. We can interpret this process geometrically in the usual way; for<br />

example, consider (dσ1∧ dσ2)(P) which can be evaluated projecting R onto the<br />

(σ1,σ2)-plane along the coordinate axesσ3 <strong>and</strong>σ4 <strong>and</strong> then taking the area of<br />

this projection. Hence we have defined the evaluation of 2-forms on planes up<br />

to orientation; the orientation will not matter for us in the following as we will<br />

only consider absolute values when evaluating 2-forms on planes. Furthermore<br />

observe that e.g. the (σ1,σ2)-plane is characterized by vanishing of all basic 2-<br />

forms execept dσ1∧ dσ2 <strong>and</strong> dσ2∧ dσ1.<br />

39

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