참고: 시료의 0.5퍼센트가 하루 동안 붕괴한다고 할 때, 이것은 처음 시료의 0.5퍼센트를 뜻하는 것이 아니다. 어떤 날이 시작될 때 시료가 1 마이크로그램이라면, 그 후 24시간 동안 붕괴하는 양은 (어떤 시각 t=0 에 "처음" 시료가 얼마였든 상관없이) 그 1 마이크로그램의 약 0.5퍼센트이다.
특히 시료가 점점 작아지므로, 매일 붕괴하는 0.5퍼센트는 실제로 붕괴하는 원자의 수가 점점 줄어든다는 것을 뜻한다. 그래서 매일 0.5%가 붕괴하고 100×0.5=50 이라고 해서, 약 100일 후에 시료의 절반(50%)이 붕괴한다고 말할 수는 없다.
원본 교재 풀이(영어)
We know that the amount of Polonium-210 in a sample after t days is given by
Q(t)where C is the original amount of the sample, and k is some positive constant.The question asks us what percentage of the sample decays in a day. Since t is measured in days, the amount that decays in a day is Q(t)−Q(t+1). The percentage of Q(t) that this represents is 100Q(t)Q(t)−Q(t+1). (For example, if there were two grams at time t, and one gram at time t+1, then 10012−1=50: 50% of the sample decayed in a day.)In order to simplify, we should figure out a better expression for Q(t). As usual, we make use of the half-life.Q(138)Ce−k⋅138(e−k)138e−kNow, we have a better formula for Q(t):Q(t)Q(t)Finally, we can evaluate what percentage of the sample decays in a day.100Q(t)Q(t)−Q(t+1)=Ce−kt=2C=2C=21=2−1=2−1381=C(e−k)t=C⋅2−138t=100C⋅2−138tC⋅2−138t−C⋅2−138t+1(C1C1)=1002−138t2−138t−2−138t+1=100(2−138t−2−138t+1)2138t=100(1−2−1381)≈0.5
About 0.5% of the sample decays in a day.
Remark: when we say that half a percent of the sample decays in a day, we don't mean half a percent of the original sample. If a day starts out with, say, 1 microgram, then what decays in the next 24 hours is about half a percent of that 1 microgram, regardless of what the “original" sample (at some time t=0) held.
In particular, since the sample is getting smaller and smaller, that half of a percent that decays every day represents fewer and fewer actual atoms decaying. That's why we can't say that half of the sample (50%) will decay after about 100 days, even though 0.5% decays every day and 100×0.5=50.
광석 시료에 우라늄-232가 7.2±0.3μg 들어 있다고 한다. 우라늄-232의 반감기는 68.8년에서 70년 사이이다. 10년 후 이 시료에 붕괴하지 않고 남아 있는 우라늄-232의 양은 얼마인지 구하세요.
영어 원문 보기
A sample of ore is found to contain 7.2±0.3μg of Uranium-232, the half-life of which is between 68.8 and 70 years. How much Uranium-232 will remain undecayed in the sample in 10 years?
The amount of Uranium-232 in the sample of ore at time t will be
Q(t)where 6.9≤Q(0)≤7.5. We don’t exactly know Q(0), and we don’t exactly know the half-life, so we also won’t exactly know Q(10): we can only say that is it between two numbers. Our strategy is to find the highest and lowest possible values of Q(10), given the information in the problem.In order for the most possible Uranium-232 to be in the sample after 10 years, we should start with the most and have the longest half-life (since this represents the slowest decay). So, we take Q(0)=7.5 and Q(70)=21(7.5).Q(t)21(7.5)=Q(70)212−701So, in this secenario,Q(t)After ten years,Q(10)So after ten years, the sample contains at most 6.8 μg.Now, let’s think about the least possible amount of Uranium-232 that could be left after 10 years. We should start with as little as possible, so take Q(0)=6.9, and the sample should decay quickly, so take the half-life to be 68.8 years.Q(t)216.9=Q(68.8)212−68.81In this scenario,Q(t)After ten years,Q(10)So after ten years, the sample contains at least 6.2 μg.=Q(0)e−kt=7.5e−kt=7.5e−k(70)=(e−k)70=e−k=7.5⋅2−70t=7.5⋅2−7010≈6.79=6.9e−kt=6.9e−k(68.8)=(e−k)68.8=e−k=6.9⋅2−68.8t=6.9⋅2−68.810≈6.24
After ten years, the sample contains between 6.2 and 6.8 μg of Uranium-232.
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.