ps01_solns

# ps01_solns - 18.03 PSI Solutions—Spring 09 PartB{1 6pts=2...

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Unformatted text preview: 18.03 PSI Solutions—Spring 09 PartB: {1. 6pts=2+2+2-];[2. 9pts=2+1+1+2+3]; [3. 5pts=2+2+1] 1a. dT dT . ﬁ—k(30—'T) => m——kdt => ln(T—30)=—kt+c => T—30=Ae“'“ (A :6“) T(0)=70 => ; T(24)=50 => k=—2-111n2~.o3 1b. T’ = k(30 + q/k — T). Same type of equation as (a) with 30 + q/k in place of 30: T=30+%—Ae‘kt As t —> oo, 6"“ -——> 0, so steady state T: 30 + q/k 1c. 30+%=60,30+q—;=70 => q1=30k,q2=40k => 3—1: 2 r5105 2a. See Figure 1. 2b. Answer: .73; 31(0) 2 .74 = curve goes up; 31(0) S .72 => curve goes down. Thus .72<A<.74 y’=0 => or b=:l:\/E,a20 2d. f(w) = —\/5 works (other answers are ok). Direction ﬁeld is horizontal but f’ (x) = —%a:‘3/2 < 0 so direction ﬁeld points into y > —\/E and solutions can’t cross from above. See Figure 2. 2c. 29. Same idea as (d). We will check that z is a subsolution (2’ < z2 —a:) and hence solutions that begin above the graph of 2 stay above it. dz—lda: => 2—1—1:r+c : z— -1 ' 22—2 ‘2 _c+a:/2 ’ 1 2 2(0)—2 = C—"'2' => 21—1—3: Notice that z —-> 00 as x -—> 1, so we can focus on a: < 1. Comparing slopes: 2 2 2 2 I 2_ __ _ 1__ 2 2 z<z z ¢=> (l—m)2<<1—x> a: 4:: \$<(1——x)2 4:» :c( as) < which is true for 0 < a: < 1, hence z’ < 22 —- a3, i.e., z is a subsolution. The graph of this inequality (Figure 3) shows direction ﬁelds that point into the region above 2(w). Solution curves are trapped in y > 2(15). They can enter, but can’t leave. In symbols, y(0)>2 => y(m)>z(m)forallm ==> y—>ooasm—>x1forsomea:1\$1. 3a. Given y = ace2 —- 3x, a = (y + Saw/\$2. ' 2 ‘3 y’=2a,z—3=2(”+23”)x—3=2§+3 = 3/: 9+ ”3 {I} {I} ~ (I! 3b. Y=ky=k(am2—3m)=%k2w2—3k¢ =>v Y=§XL3X ...
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