x=0 일 때 y−1y−2=21>0 임을 알 수 있다. 또한 21e1−cosx 는, 따라서 y−1y−2 도, 결코 0 이 될 수 없다. y(x) 는 x 에 따라 연속적으로 변하므로 y(x) 는 계속 2 보다 커야 한다. 따라서 y−1y−2 는 계속 양수이므로 절댓값 기호를 없앨 수 있다. 그러므로
간단히 하기 위해 L=1−log2 라 하면 L>0 이다. (2<e 이므로 log2<loge=1 이고, 따라서 1−log2>0 임에서 알 수 있다.)
x=0 은 우리가 구한 함수의 정의역에 속하지만, 점 x=±arccos(L)=±arccos(1−log2) 는 정의역에 속하지 않는다.
따라서 우리의 답이 의미를 갖는 가장 큰 구간은 −arccos(1−log2))>x>arccos(1−log2)
이고, 이는 대략 −1.259<x<1.259 이다.
원본 교재 풀이(영어)
What we're given is an equation relating y to the integral of a function of y. What we know how to solve is an equation relating the derivative of y to a function of y. We can create this by differentiating the given integral equation.
By the Fundamental Theorem of Calculus, part 1:
So y(x) satisfies the differential equation y′=(y2−3y+2)sinx=(y−2)(y−1)sinx
and the initial equation y(0)=3 (just substitute x=0 into (∗)).
For y=1,2:
dxdy(y−2)(y−1)dy∫(y−2)(y−1)dyUsing the method of partial fractions, we see (y−2)(y−1)1=y−21−y−11.∫[y−21−y−11]dylog∣y−2∣−log∣y−1∣logy−1y−2y−1y−2The condition y(0)=3 forces 3−13−2=ec−1 or ec=21e, hencey−1y−2=(y−2)(y−1)sinx=sinxdx=∫sinxdx=∫sinxdx=−cosx+c=−cosx+c=ec−cosx=21e1−cosx
Observe that, when x=0, y−1y−2=21>0. Furthermore
21e1−cosx, and hence y−1y−2,
can never take the value zero. As y(x) varies continuously with x,
y(x) must remain larger than 2. Consquently, y−1y−2 remains
positive and we may drop the absolute value signs. Hence
y−1y−2=21e1−cosx Solving for y,y−1y−22(y−2)2y−4y(2−e1−cosx)y=21e1−cosx=e1−cosx(y−1)=ye1−cosx−e1−cosx=4−e1−cosx=2−e1−cosx4−e1−cosx
To avoid division by zero in the last step, we need
e1−cosx1−cosxcosx=2=log2=1−log2
Let L=1−log2, for brevity, and note that L>0. (This can be seen by observing 2<e, so, log2<loge=1, hence 1−log2>0.)
We know x=0 is in the domain of our function, but the points x=±arccos(L)=±arccos(1−log2) are not.
Therefore, the largest interval for which our answer makes sense is −arccos(1−log2))>x>arccos(1−log2)
or approximately −1.259<x<1.259.
Thus y=f(x) obeys the differential equation y′=(y−1)(y−2).
(c) If y=1,2,
dxdy(y−1)(y−2)dy∫(y−1)(y−2)dyUsing the method of partial fractions,∫(y−21−y−11)dylog∣y−2∣−log∣y−1∣logy−1y−2 Observe that dxdy=(y−1)(y−2)>0 for all y≥2. That is, f(x) is increasing at all x for which f(x)>2. As f(0)=3, f(x) increases for all x≥0, and f(x)≥3 for all x≥0. So we may drop the absolute value signs.logf(x)−1f(x)−2f(x)−1f(x)−2 At x=0, f(x)−1f(x)−2=21 so eC=21.f(x)−1f(x)−22f(x)−4[2−ex]f(x)f(x)=(y−1)(y−2)=dx=∫dx=∫dx=x+C=x+C=x+C=eCex=21ex=[f(x)−1]ex=4−ex=2−ex4−ex
We start by antidifferentiating both sides with respect to x.
∫(dx2d2y)dxThe right integral is in exactly the form we would use for a change of variables (substitution) to y.dxdyWhen y=1, dxdy=3.3CSo,dxdy This is a separable differential equation. dxdy4y2−1y2dy∫4y2−1y2dy=∫(y32⋅dxdy)dx=∫(y32)dy=−y21+C=−11+C=4=−y21+4=y24y2−1=dx=∫dx(∗)
We can evaluate the left integral with partial fractions, but because the numerator has the same degree as the denominator, we have to simplify first. We do this by inspection, but you can also use long division.
We can check our answer by differentiating with respect to x.
x4xdxd{4x}44dxdyDifferentiating with respect to x again, using the chain rule,dx2d2y=41(y−1+41log2y+12y−1)=y−1+41log∣2y−1∣−41log∣2y+1∣=dxd{y−1+41log∣2y−1∣−41log∣2y+1∣}=dxdy+41⋅2y−12dxdy−41⋅2y+12dxdy=dxdy(1+2y−11/2−2y+11/2)=dxdy(4y2−14y2)=y24y2−1=4−y21=y32⋅dxdy(∗∗)
This is exactly the differential equation we were meant to solve.