通过代换 u=x−yu = x - y,求解微分方程 dydx+4(x−y)2cos⁡2x=sin⁡2x.\dfrac{dy}{dx} + 4(x - y)^2\cos^2 x = \sin^2 x. 一种用于治疗糖尿病的新药以每天 RR 毫克的恒定速率输给患者。药物从患者体内流失的速率与时间 tt(天)时体内存在的药物量 xx(毫克)的平方成正比。 如果在药物量为 2R2R(毫克)的瞬间,患者体内的药物量保持恒定,证明 dxdt=4R2−x24R.\dfrac{dx}{dt} = \dfrac{4R^2 - x^2}{4R}. 已知当 t=0t = 0 时 x=0x = 0,求以 RR 和 tt 表示的 xx。 解释这一结果在长期来看的意义。

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完整解法

4(a)

1. Differentiate the substitution with respect to $x$ to express $\dfrac{dy}{dx}$ in terms of $\dfrac{du}{dx}$.

Given u=x−yu = x - y, differentiating with respect to xx gives:
dudx=1−dydx\frac{du}{dx} = 1 - \frac{dy}{dx}
dydx=1−dudx\frac{dy}{dx} = 1 - \frac{du}{dx}

2. Substitute $u$ and $\dfrac{dy}{dx}$ into the original differential equation and simplify to form a separable equation.

1−dudx+4u2cos⁡2x=sin⁡2x1 - \frac{du}{dx} + 4u^2\cos^2 x = \sin^2 x
dudx=1−sin⁡2x+4u2cos⁡2x\frac{du}{dx} = 1 - \sin^2 x + 4u^2\cos^2 x
Using the identity cos⁡2x=1−sin⁡2x\cos^2 x = 1 - \sin^2 x:
dudx=cos⁡2x+4u2cos⁡2x\frac{du}{dx} = \cos^2 x + 4u^2\cos^2 x
dudx=cos⁡2x(1+4u2)\frac{du}{dx} = \cos^2 x (1 + 4u^2)

3. Separate the variables and set up the integrals.

∫11+4u2 du=∫cos⁡2x dx\int \frac{1}{1 + 4u^2} \, du = \int \cos^2 x \, dx

4. Evaluate both integrals using standard techniques.

For the left side, we integrate to get an inverse tangent:
∫11+(2u)2 du=12tan⁡−1(2u)\int \frac{1}{1 + (2u)^2} \, du = \frac{1}{2}\tan^{-1}(2u)

For the right side, we use the double angle identity cos⁡2x=1+cos⁡2x2\cos^2 x = \frac{1 + \cos 2x}{2}:
∫1+cos⁡2x2 dx=12x+14sin⁡2x+C′\int \frac{1 + \cos 2x}{2} \, dx = \frac{1}{2}x + \frac{1}{4}\sin 2x + C'

Equating both sides:
12tan⁡−1(2u)=12x+14sin⁡2x+C′\frac{1}{2}\tan^{-1}(2u) = \frac{1}{2}x + \frac{1}{4}\sin 2x + C'
Multiplying through by 22 and letting C=2C′C = 2C':
tan⁡−1(2u)=x+12sin⁡2x+C\tan^{-1}(2u) = x + \frac{1}{2}\sin 2x + C

5. Substitute $u$ back in and make $y$ the subject to state the general solution.

2u=tan⁡(x+12sin⁡2x+C)2u = \tan\left(x + \frac{1}{2}\sin 2x + C\right)
2(x−y)=tan⁡(x+12sin⁡2x+C)2(x - y) = \tan\left(x + \frac{1}{2}\sin 2x + C\right)
x−y=12tan⁡(x+12sin⁡2x+C)x - y = \frac{1}{2}\tan\left(x + \frac{1}{2}\sin 2x + C\right)
y=x−12tan⁡(x+12sin⁡2x+C)y = x - \frac{1}{2}\tan\left(x + \frac{1}{2}\sin 2x + C\right)

答案

y=x−12tan⁡(x+12sin⁡2x+C)y = x - \dfrac{1}{2}\tan\left(x + \dfrac{1}{2}\sin 2x + C\right)

4(b)(i)

1. Formulate the differential equation using the given rates

Let xx be the amount of drug in the body at time tt.
The rate of drug administered is RR, and the rate of loss is proportional to x2x^2.
dxdt=R−kx2\dfrac{dx}{dt} = R - kx^2

2. Determine the proportionality constant $k$ and show the given equation

When x=2Rx = 2R, the amount of drug remains constant, so dxdt=0\dfrac{dx}{dt} = 0.
0=R−k(2R)20 = R - k(2R)^2
4kR2=R  ⟹  k=14R4kR^2 = R \implies k = \dfrac{1}{4R}
Substituting kk back into the differential equation:
dxdt=R−x24R=4R2−x24R\dfrac{dx}{dt} = R - \dfrac{x^2}{4R} = \dfrac{4R^2 - x^2}{4R}

3. Separate variables and integrate

Separating variables:
∫14R2−x2 dx=∫14R dt\int \dfrac{1}{4R^2 - x^2} \, dx = \int \dfrac{1}{4R} \, dt
Using the standard integral ∫1a2−x2 dx=12aln⁡∣a+xa−x∣\int \dfrac{1}{a^2 - x^2} \, dx = \dfrac{1}{2a} \ln \left| \dfrac{a+x}{a-x} \right| with a=2Ra = 2R:
12(2R)ln⁡∣2R+x2R−x∣=t4R+C\dfrac{1}{2(2R)} \ln \left| \dfrac{2R + x}{2R - x} \right| = \dfrac{t}{4R} + C
14Rln⁡∣2R+x2R−x∣=t4R+C\dfrac{1}{4R} \ln \left| \dfrac{2R + x}{2R - x} \right| = \dfrac{t}{4R} + C

4. Use the initial condition to find the constant of integration

Given x=0x = 0 when t=0t = 0:
14Rln⁡∣2R+02R−0∣=0+C\dfrac{1}{4R} \ln \left| \dfrac{2R + 0}{2R - 0} \right| = 0 + C
C=14Rln⁡1=0C = \dfrac{1}{4R} \ln 1 = 0
So, 14Rln⁡∣2R+x2R−x∣=t4R\dfrac{1}{4R} \ln \left| \dfrac{2R + x}{2R - x} \right| = \dfrac{t}{4R}
Multiplying both sides by 4R4R:
ln⁡∣2R+x2R−x∣=t\ln \left| \dfrac{2R + x}{2R - x} \right| = t

5. Express $x$ in terms of $R$ and $t$

Since xx starts at 00 and increases (with dx/dt=0dx/dt = 0 at the asymptote x=2Rx = 2R), we have 0≤x<2R0 \le x < 2R, meaning 2R+x2R−x>0\dfrac{2R+x}{2R-x} > 0. We can remove the absolute value signs.
2R+x2R−x=et\dfrac{2R + x}{2R - x} = e^t
2R+x=(2R−x)et2R + x = (2R - x) e^t
2R+x=2Ret−xet2R + x = 2R e^t - x e^t
x+xet=2Ret−2Rx + x e^t = 2R e^t - 2R
x(et+1)=2R(et−1)x(e^t + 1) = 2R(e^t - 1)
x=2R(et−1)et+1x = \dfrac{2R(e^t - 1)}{e^t + 1}

答案

x=2R(et−1)et+1x = \dfrac{2R(e^t - 1)}{e^t + 1}

4(b)(ii)

1. Concisely solve the differential equation from part (b)(i) to find the explicit formula for $x$ in terms of $t$ (as required to analyse its limit).

Separating variables and using partial fractions:
∫4R4R2−x2 dx=∫dt\int \frac{4R}{4R^2 - x^2} \, dx = \int dt
∫(12R−x+12R+x)dx=∫1 dt\int \left( \frac{1}{2R-x} + \frac{1}{2R+x} \right) dx = \int 1 \, dt
−ln⁡∣2R−x∣+ln⁡∣2R+x∣=t+C-\ln|2R-x| + \ln|2R+x| = t + C
ln⁡∣2R+x2R−x∣=t+C\ln\left|\frac{2R+x}{2R-x}\right| = t + C
Given x=0x = 0 when t=0t = 0, we find C=ln⁡1=0C = \ln 1 = 0. Since xx increases from 00, 2R−x>02R-x > 0:
2R+x2R−x=et\frac{2R+x}{2R-x} = e^t
2R+x=2Ret−xet2R+x = 2Re^t - xe^t
x(et+1)=2R(et−1)  ⟹  x=2Ret−1et+1x(e^t+1) = 2R(e^t-1) \implies x = 2R\frac{e^t-1}{e^t+1}

2. Determine the mathematical behaviour of $x$ as $t \to \infty$.

Divide the numerator and the denominator by ete^t:
x=2R1−e−t1+e−tx = 2R\frac{1 - e^{-t}}{1 + e^{-t}}
As t→∞t \to \infty, e−t→0e^{-t} \to 0. Therefore:
x→2R(1−01+0)=2Rx \to 2R\left(\frac{1-0}{1+0}\right) = 2R

3. Interpret the mathematical limit in the context of the problem.

The mathematical limit x→2Rx \to 2R means that over a long period of time, the amount of the drug in the patient's body approaches and stabilizes at a constant level of 2R mg2R\text{ mg}.

答案

In the long run, the amount of the drug in the patient's body will approach and stabilize at 2R mg2R\text{ mg}.

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