Given that y=(cos⁡−1x)2y=(\cos^{-1} x)^2.

  1. (i)

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

  2. (ii)

    Hence find the Maclaurin's series for (cos⁡−1x)2(\cos^{-1} x)^2, up to and including the term in x3x^3. Give the coefficients in exact form.

  3. (iii)

    Show that, if xx is sufficiently small for powers of xx above x2x^2 to be neglected, then e(cos⁡−1x)2≈eπ2/4(1+ax+bx2)e^{(\cos^{-1} x)^2} \approx e^{\pi^2/4}(1+ax+bx^2), where aa and bb are constants to be determined exactly.

    [You may use standard results given in the List of Formulae (MF15).]

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Worked solution

1(i)

1. Differentiate $y$ with respect to $x$ using the chain rule.

dydx=2(cos⁡−1x)⋅(−11−x2)\dfrac{dy}{dx} = 2(\cos^{-1} x) \cdot \left( -\dfrac{1}{\sqrt{1-x^2}} \right)

2. Rearrange the equation to avoid applying the quotient rule in the subsequent differentiation.

1−x2dydx=−2cos⁡−1x\sqrt{1-x^2}\dfrac{dy}{dx} = -2\cos^{-1} x

3. Differentiate both sides implicitly with respect to $x$ using the product rule.

1−x2d2ydx2+dydx(121−x2⋅(−2x))=−2(−11−x2)\sqrt{1-x^2}\dfrac{d^2y}{dx^2} + \dfrac{dy}{dx}\left(\dfrac{1}{2\sqrt{1-x^2}} \cdot (-2x)\right) = -2\left(-\dfrac{1}{\sqrt{1-x^2}}\right)
1−x2d2ydx2−x1−x2dydx=21−x2\sqrt{1-x^2}\dfrac{d^2y}{dx^2} - \dfrac{x}{\sqrt{1-x^2}}\dfrac{dy}{dx} = \dfrac{2}{\sqrt{1-x^2}}

4. Simplify the equation to obtain the required form.

Multiply both sides by 1−x2\sqrt{1-x^2}:
(1−x2)d2ydx2−xdydx=2(1-x^2)\dfrac{d^2y}{dx^2} - x\dfrac{dy}{dx} = 2 (Shown)

Answer

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

1(ii)

1. Find the values of $y$ and $\frac{dy}{dx}$ at $x=0$.

When x=0x = 0,
y=(cos⁡−10)2=(π2)2=π24y = (\cos^{-1} 0)^2 = \left(\frac{\pi}{2}\right)^2 = \frac{\pi^2}{4}

dydx=2(cos⁡−1x)⋅(−11−x2)\frac{dy}{dx} = 2(\cos^{-1} x) \cdot \left(-\frac{1}{\sqrt{1-x^2}}\right)
At x=0x = 0, dydx=2(π2)(−1)=−π\frac{dy}{dx} = 2\left(\frac{\pi}{2}\right)(-1) = -\pi

2. Find the value of $\frac{d^2y}{dx^2}$ at $x=0$ using the result from part (i).

From part (i), we have:
(1−x2)d2ydx2−xdydx=2(1-x^2)\frac{d^2y}{dx^2} - x\frac{dy}{dx} = 2
Substituting x=0x = 0,
(1−0)d2ydx2−0=2(1 - 0)\frac{d^2y}{dx^2} - 0 = 2
d2ydx2=2\frac{d^2y}{dx^2} = 2

3. Differentiate the equation from part (i) to find the value of $\frac{d^3y}{dx^3}$ at $x=0$.

Differentiating (1−x2)d2ydx2−xdydx=2(1-x^2)\frac{d^2y}{dx^2} - x\frac{dy}{dx} = 2 implicitly with respect to xx:
(1−x2)d3ydx3+(−2x)d2ydx2−(xd2ydx2+1⋅dydx)=0(1-x^2)\frac{d^3y}{dx^3} + (-2x)\frac{d^2y}{dx^2} - \left(x\frac{d^2y}{dx^2} + 1\cdot\frac{dy}{dx}\right) = 0
(1−x2)d3ydx3−3xd2ydx2−dydx=0(1-x^2)\frac{d^3y}{dx^3} - 3x\frac{d^2y}{dx^2} - \frac{dy}{dx} = 0

Substituting x=0x = 0,
(1−0)d3ydx3−0−(−π)=0(1-0)\frac{d^3y}{dx^3} - 0 - (-\pi) = 0
d3ydx3=−π\frac{d^3y}{dx^3} = -\pi

4. Form the Maclaurin's series up to the term in $x^3$.

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 known values:
(cos⁡−1x)2=π24+(−π)x+22!x2+−π3!x3+…(\cos^{-1} x)^2 = \frac{\pi^2}{4} + (-\pi)x + \frac{2}{2!}x^2 + \frac{-\pi}{3!}x^3 + \dots
(cos⁡−1x)2=π24−πx+x2−π6x3+…(\cos^{-1} x)^2 = \frac{\pi^2}{4} - \pi x + x^2 - \frac{\pi}{6}x^3 + \dots

Answer

\frac{\pi^2}{4} - \pi x + x^2 - \frac{\pi}{6}x^3

1(iii)

1. Obtain the Maclaurin series for $(\cos^{-1} x)^2$ up to the term in $x^2$.

To use the result from part (ii), we calculate the required derivatives at x=0x=0.
Let y=(cos⁡−1x)2y = (\cos^{-1} x)^2.
When x=0x=0, y=(cos⁡−10)2=(π2)2=π24y = (\cos^{-1} 0)^2 = \left(\frac{\pi}{2}\right)^2 = \frac{\pi^2}{4}.
dydx=2(cos⁡−1x)(−11−x2)  ⟹  dydx∣x=0=2(π2)(−1)=−π\frac{dy}{dx} = 2(\cos^{-1} x)\left(-\frac{1}{\sqrt{1-x^2}}\right) \implies \left.\frac{dy}{dx}\right|_{x=0} = 2\left(\frac{\pi}{2}\right)(-1) = -\pi.
From (1−x2)d2ydx2−xdydx=2(1-x^2)\frac{d^2y}{dx^2}-x\frac{dy}{dx}=2 (proven in part i), substituting x=0x=0 gives (1)d2ydx2−0=2  ⟹  d2ydx2∣x=0=2(1)\frac{d^2y}{dx^2} - 0 = 2 \implies \left.\frac{d^2y}{dx^2}\right|_{x=0} = 2.
Thus, the Maclaurin series up to x2x^2 is:
(cos⁡−1x)2≈π24−πx+22!x2=π24−πx+x2(\cos^{-1} x)^2 \approx \frac{\pi^2}{4} - \pi x + \frac{2}{2!}x^2 = \frac{\pi^2}{4} - \pi x + x^2.

2. Substitute the series into the exponential function and isolate the constant factor $e^{\pi^2/4}$.

Substitute the quadratic approximation into the exponent:
e(cos⁡−1x)2≈eπ24−πx+x2e^{(\cos^{-1} x)^2} \approx e^{\frac{\pi^2}{4} - \pi x + x^2}
Using the laws of indices:
eπ24−πx+x2=eπ24e−πx+x2e^{\frac{\pi^2}{4} - \pi x + x^2} = e^{\frac{\pi^2}{4}} e^{-\pi x + x^2}

3. Expand $e^{-\pi x + x^2}$ using the standard Maclaurin series for $e^u$, neglecting powers of $x$ above $x^2$.

Using the standard series expansion eu≈1+u+u22!e^u \approx 1 + u + \frac{u^2}{2!} for small uu:
e−πx+x2≈1+(−πx+x2)+(−πx+x2)22e^{-\pi x + x^2} \approx 1 + (-\pi x + x^2) + \frac{(-\pi x + x^2)^2}{2}
Expanding the squared term and neglecting powers of xx above x2x^2 (since (−πx)2=π2x2(-\pi x)^2 = \pi^2 x^2, while cross terms and (x2)2(x^2)^2 produce higher powers):
e−πx+x2≈1−πx+x2+12(π2x2)e^{-\pi x + x^2} \approx 1 - \pi x + x^2 + \frac{1}{2}(\pi^2 x^2)
=1−πx+(1+π22)x2= 1 - \pi x + \left(1 + \frac{\pi^2}{2}\right)x^2

4. Equate coefficients to find $a$ and $b$.

Substitute this back into the original expression:
e(cos⁡−1x)2≈eπ24[1−πx+(1+π22)x2]e^{(\cos^{-1} x)^2} \approx e^{\frac{\pi^2}{4}} \left[ 1 - \pi x + \left(1 + \frac{\pi^2}{2}\right)x^2 \right]
Comparing this with the given form eπ2/4(1+ax+bx2)e^{\pi^2/4}(1+ax+bx^2), we get:
a=−πa = -\pi and b=1+π22b = 1 + \frac{\pi^2}{2}.

Answer

a=−πa = -\pi, b=1+π22b = 1 + \frac{\pi^2}{2}

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