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Unformatted text preview: Mathematics 33B This is intended to be an outline for the entire course and a guide for studying for the final exam. I. First Order Equations (Sections 2.1,2.2, 2.42.9) We covered quite a bit here, but it really all comes under the following topics: i) Solving y ′ + a ( t ) y = g ( t ) for the unknown function y ( t ) (Section 2.4). ii) Exact equations in general, and y ′ = f ( t ) h ( y ) in particular (Section 2.2 and 2.6). iii) Asymptotic stability and instability of solutions to autonomous equations (Sec tion 2.9). iv) Learning to use these differential equations in simple applications (Section 2.5, 3.1 and 3.3). v) The dreaded existence and uniqueness theory (Section 2.1 and 2.7). With regard to (2.4) you should definitely know how to explain that y ′ + a ( t ) y = g ( t ) is equivalent to ( e A ( t ) y ) ′ = e A ( t ) g ( t ) , where A ( t ) = integraltext a ( t ) dt is any antiderivative of a ( t ), as I asked some of you to do on the first hour exam. For y ′ = f ( t ) h ( y ) be on the lookout for values of y where h ( y ) = 0. Remember, if h ( y ) = 0, then the constant function y ( x ) = y will be a solution that you will NOT find by the standard method of reducing the equation to integraltext ( h ( y )) − 1 dy = integraltext f ( t ) dt . There are some basic facts from Section 2.6 which you need to know: a) The statement that y ( x ) is a solution to y ′ = f ( x, y ) is equivalent to the statement that the differential form ω = μ ( x, y ) dy − μ ( x, y ) f ( x, y ) dx is zero on y = y ( x ). When ω = ( ∂F/∂x ) dx + ( ∂F/∂x ) dy , then the level curves F ( x, y ( x )) = C are solutions to y ′ = f ( x, y ). b) The differential form ω = Pdx + Qdy equals ( ∂F/∂x ) dx + ( ∂F/∂x ) dy for some function F on a rectangle if and only if ∂P/∂y = ∂Q/∂x . When this happens, ω is called “exact”. c) When ω is exact, you can find F in the form F = integraldisplay Pdx + h ( y ) or F = integraldisplay Qdy + g ( x ) , where you have to choose h so that ∂F/∂y = Q , or you have to choose g so that ∂F/∂x = P . On the first hour exam I asked some of you to explain why that works. I might ask again. 2 d) If ω is not exact, you can always multiply it by an integrating factor μ ( x, y ) to make it exact. Unfortunately, finding μ is usually very difficult. It is not difficult to look for integrating factors which just depend on one variable, and I might ask you to do that. For all first order equations remember that two solutions of the same equation “cannot cross” each other, meaning if two solutions agree at a point, y ( t 1 ) = z ( t 1 ), then they must agree on their whole interval of existence, that means y ( t ) ≡ z ( t )....
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This note was uploaded on 03/04/2008 for the course MATH 33B taught by Professor Staff during the Spring '07 term at UCLA.
 Spring '07
 staff
 Math, Equations

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