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Unformatted text preview: o ensure that this is so, we must supplement the ODEs by the algebraic
x2 + y2 = l2 :
The two second-order di erential equations and the constraint comprise a system of
ve di erential algebraic equations (DAEs) for the unknowns x(t), y(t), and T (t).
Initial conditions specify x(0), dx(0)=dt, y(0), and dy(0)=dt, but not T (0).
5 Of course, for this problem, it's easy to eliminate the constraint by introducing the
change of variables x = l sin , y = l cos . This would reduce the DAEs to the
d2 = ; g sin :
Such simpli cations would not be possible with more di cult systems. θ
mg Figure 1.1.3: Oscillations of a simple Pendelum.
IVPs will comprise our initial study (Part 2 of these notes). We'll take up BVPs
next (Part 3) and conclude with a study of DAEs (Part 4). In almost all cases, it will
su ce to develop and analyze numerical methods for IVPs and BVPs that are written
as rst-order vector systems of ODEs in the explicit form y (t) = f (t y)
0 t>0 (1.1.1a...
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This document was uploaded on 03/16/2014 for the course CSCI 6820 at Rensselaer Polytechnic Institute.
- Spring '14