已知 y=ecos⁡−1xy = e^{\cos^{-1} x}。

  1. (i)

    证明 (1−x2)d2ydx2−xdydx=y\left(1 - x^2\right)\dfrac{d^2 y}{dx^2} - x\dfrac{dy}{dx} = y。

  2. (ii)

    求 yy 的麦克劳林级数,给出准确系数,展开至包含 x3x^3 项。

  3. (iii)

    由此求出 −ecos⁡−1x1−x2-\dfrac{e^{\cos^{-1} x}}{\sqrt{1 - x^2}} 展开至包含 x2x^2 项的展开式,并估算曲线 y=ecos⁡−1xy = e^{\cos^{-1} x} 在 x=0.5x = 0.5 处的切线斜率。

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完整解法

6(i)

1. Find the first derivative $\dfrac{dy}{dx}$ and express it in terms of $y$.

y=ecos⁡−1xy = e^{\cos^{-1} x}

Differentiating with respect to xx using the chain rule:
dydx=ecos⁡−1x⋅(−11−x2)\frac{dy}{dx} = e^{\cos^{-1} x} \cdot \left( -\frac{1}{\sqrt{1 - x^2}} \right)

Substitute y=ecos⁡−1xy = e^{\cos^{-1} x} back into the equation:
dydx=−y1−x2\frac{dy}{dx} = -\frac{y}{\sqrt{1 - x^2}}

2. Rearrange the equation and square both sides to eliminate the fraction and square root.

Multiply by 1−x2\sqrt{1 - x^2}:
1−x2dydx=−y\sqrt{1 - x^2} \frac{dy}{dx} = -y

Squaring both sides gives:
(1−x2)(dydx)2=y2(1 - x^2) \left(\frac{dy}{dx}\right)^2 = y^2

3. Differentiate implicitly with respect to $x$ using the product and chain rules, then simplify.

Differentiating both sides with respect to xx:
(1−x2)ddx[(dydx)2]+(dydx)2ddx(1−x2)=ddx(y2)(1 - x^2) \frac{d}{dx}\left[\left(\frac{dy}{dx}\right)^2\right] + \left(\frac{dy}{dx}\right)^2 \frac{d}{dx}(1 - x^2) = \frac{d}{dx}(y^2)

(1−x2)(2dydxd2ydx2)+(dydx)2(−2x)=2ydydx(1 - x^2) \left(2 \frac{dy}{dx} \frac{d^2y}{dx^2}\right) + \left(\frac{dy}{dx}\right)^2 (-2x) = 2y \frac{dy}{dx}

Dividing both sides by the common factor 2dydx2\frac{dy}{dx}:
(1−x2)d2ydx2−xdydx=y(Shown)(1 - x^2) \frac{d^2y}{dx^2} - x \frac{dy}{dx} = y \quad \text{(Shown)}

答案

(1−x2)d2ydx2−xdydx=y\left(1 - x^2\right)\dfrac{d^2 y}{dx^2} - x\dfrac{dy}{dx} = y

6(ii)

1. Evaluate $y$, $\frac{dy}{dx}$, and $\frac{d^2 y}{dx^2}$ at $x = 0$.

Given y=ecos⁡−1xy = e^{\cos^{-1} x}, when x=0x = 0:
y(0)=ecos⁡−10=eπ2y(0) = e^{\cos^{-1} 0} = e^{\frac{\pi}{2}}

Differentiating with respect to xx:
y′=ecos⁡−1x(−11−x2)y' = e^{\cos^{-1} x} \left( -\frac{1}{\sqrt{1 - x^2}} \right)
When x=0x = 0, y′(0)=eπ2(−1)=−eπ2y'(0) = e^{\frac{\pi}{2}} (-1) = -e^{\frac{\pi}{2}}.

From part (i), we have the relation:
(1−x2)y′′−xy′=y(1 - x^2)y'' - xy' = y
Substituting x=0x = 0, y(0)=eπ2y(0) = e^{\frac{\pi}{2}} and y′(0)=−eπ2y'(0) = -e^{\frac{\pi}{2}}:
(1−0)y′′(0)−0=eπ2  ⟹  y′′(0)=eπ2(1 - 0)y''(0) - 0 = e^{\frac{\pi}{2}} \implies y''(0) = e^{\frac{\pi}{2}}

2. Differentiate the given differential equation to find an expression for $\frac{d^3 y}{dx^3}$.

Differentiating (1−x2)y′′−xy′=y(1 - x^2)y'' - xy' = y with respect to xx using the product rule:
(1−x2)y′′′+y′′(−2x)−(xy′′+y′)=y′(1 - x^2)y''' + y''(-2x) - (x y'' + y') = y'

Simplifying the equation:
(1−x2)y′′′−3xy′′−y′=y′(1 - x^2)y''' - 3xy'' - y' = y'
(1−x2)y′′′−3xy′′−2y′=0(1 - x^2)y''' - 3xy'' - 2y' = 0

3. Evaluate $\frac{d^3 y}{dx^3}$ at $x=0$ and construct the Maclaurin's series.

Substitute x=0x = 0, y′(0)=−eπ2y'(0) = -e^{\frac{\pi}{2}}, and y′′(0)=eπ2y''(0) = e^{\frac{\pi}{2}} into the differentiated equation:
(1−0)y′′′(0)−0−2(−eπ2)=0(1 - 0)y'''(0) - 0 - 2\left(-e^{\frac{\pi}{2}}\right) = 0
y′′′(0)=−2eπ2y'''(0) = -2e^{\frac{\pi}{2}}

The Maclaurin's series is given by:
y=y(0)+y′(0)x+y′′(0)2!x2+y′′′(0)3!x3+…y = y(0) + y'(0)x + \frac{y''(0)}{2!}x^2 + \frac{y'''(0)}{3!}x^3 + \dots

Substituting the exact values:
y=eπ2+(−eπ2)x+eπ22x2+−2eπ26x3+…y = e^{\frac{\pi}{2}} + \left(-e^{\frac{\pi}{2}}\right)x + \frac{e^{\frac{\pi}{2}}}{2}x^2 + \frac{-2e^{\frac{\pi}{2}}}{6}x^3 + \dots
y=eπ2−eπ2x+eπ22x2−eπ23x3+…y = e^{\frac{\pi}{2}} - e^{\frac{\pi}{2}} x + \frac{e^{\frac{\pi}{2}}}{2} x^2 - \frac{e^{\frac{\pi}{2}}}{3} x^3 + \dots

答案

y=eπ2−eπ2x+eπ22x2−eπ23x3+…y = e^{\frac{\pi}{2}} - e^{\frac{\pi}{2}} x + \frac{e^{\frac{\pi}{2}}}{2} x^2 - \frac{e^{\frac{\pi}{2}}}{3} x^3 + \dots

6(iii)

1. Concise derivation of the result from part (ii) (Maclaurin series for $y$ up to $x^3$).

From part (ii), we first need the Maclaurin series of y=ecos⁡−1xy = e^{\cos^{-1} x} up to the term in x3x^3.
At x=0x=0, y(0)=eπ/2y(0) = e^{\pi/2}.
dydx=−ecos⁡−1x1−x2  ⟹  y′(0)=−eπ/2\dfrac{dy}{dx} = -\dfrac{e^{\cos^{-1} x}}{\sqrt{1 - x^2}} \implies y'(0) = -e^{\pi/2}.
Using (1−x2)y′′−xy′=y\left(1 - x^2\right)y'' - xy' = y from (i):
y′′(0)−0=y(0)  ⟹  y′′(0)=eπ/2y''(0) - 0 = y(0) \implies y''(0) = e^{\pi/2}.
Repeated differentiation implicitly yields:
−2xy′′+(1−x2)y′′′−y′−xy′′=y′  ⟹  (1−x2)y′′′−3xy′′−2y′=0-2xy'' + (1-x^2)y''' - y' - xy'' = y' \implies (1-x^2)y''' - 3xy'' - 2y' = 0
y′′′(0)−0−2(−eπ/2)=0  ⟹  y′′′(0)=−2eπ/2y'''(0) - 0 - 2(-e^{\pi/2}) = 0 \implies y'''(0) = -2e^{\pi/2}.
Thus, the series up to x3x^3 is:
y≈eπ/2−eπ/2x+eπ/22x2−2eπ/26x3=eπ/2(1−x+x22−x33)y \approx e^{\pi/2} - e^{\pi/2}x + \dfrac{e^{\pi/2}}{2}x^2 - \dfrac{2e^{\pi/2}}{6}x^3 = e^{\pi/2}\left(1 - x + \dfrac{x^2}{2} - \dfrac{x^3}{3}\right).

2. Recognise the given expression as the first derivative of $y$ and differentiate the series to find its expansion.

Notice that −ecos⁡−1x1−x2=dydx-\dfrac{e^{\cos^{-1} x}}{\sqrt{1 - x^2}} = \dfrac{dy}{dx}.
Using the "Hence" instruction, we differentiate the Maclaurin series of yy term-by-term to find the expansion of its derivative:
dydx≈ddx(eπ/2−eπ/2x+eπ/22x2−eπ/23x3)\dfrac{dy}{dx} \approx \dfrac{d}{dx} \left( e^{\pi/2} - e^{\pi/2}x + \dfrac{e^{\pi/2}}{2}x^2 - \dfrac{e^{\pi/2}}{3}x^3 \right)
dydx≈−eπ/2+eπ/2x−eπ/2x2\dfrac{dy}{dx} \approx -e^{\pi/2} + e^{\pi/2}x - e^{\pi/2}x^2

3. Use the expansion to estimate the gradient of the tangent at $x = 0.5$.

The gradient of the tangent to the curve is given by dydx\dfrac{dy}{dx}.
Substituting x=0.5x = 0.5 into the truncated expansion:
Gradient≈−eπ/2+eπ/2(0.5)−eπ/2(0.5)2\text{Gradient} \approx -e^{\pi/2} + e^{\pi/2}(0.5) - e^{\pi/2}(0.5)^2
=eπ/2(−1+12−14)= e^{\pi/2} \left(-1 + \dfrac{1}{2} - \dfrac{1}{4}\right)
=−34eπ/2= -\dfrac{3}{4}e^{\pi/2}
≈−3.61 (to 3 s.f.)\approx -3.61 \text{ (to 3 s.f.)}

答案

Expansion: −eπ/2+eπ/2x−eπ/2x2-e^{\pi/2} + e^{\pi/2}x - e^{\pi/2}x^2
Gradient estimate: −34eπ/2-\dfrac{3}{4}e^{\pi/2} (or ≈−3.61\approx -3.61)

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