Given that .
- (i)
Show that .
- (ii)
Hence find the Maclaurin's series for , up to and including the term in . Give the coefficients in exact form.
- (iii)
Show that, if is sufficiently small for powers of above to be neglected, then , where and 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.
2. Rearrange the equation to avoid applying the quotient rule in the subsequent differentiation.
3. Differentiate both sides implicitly with respect to $x$ using the product rule.
4. Simplify the equation to obtain the required form.
Multiply both sides by :
(Shown)
(Shown)
1(ii)
1. Find the values of $y$ and $\frac{dy}{dx}$ at $x=0$.
When ,
At ,
2. Find the value of $\frac{d^2y}{dx^2}$ at $x=0$ using the result from part (i).
From part (i), we have:
Substituting ,
3. Differentiate the equation from part (i) to find the value of $\frac{d^3y}{dx^3}$ at $x=0$.
Differentiating implicitly with respect to :
Substituting ,
4. Form the Maclaurin's series up to the term in $x^3$.
The Maclaurin's series is given by:
Substituting the known values:
\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 .
Let .
When , .
.
From (proven in part i), substituting gives .
Thus, the Maclaurin series up to is:
.
2. Substitute the series into the exponential function and isolate the constant factor $e^{\pi^2/4}$.
Substitute the quadratic approximation into the exponent:
Using the laws of indices:
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 for small :
Expanding the squared term and neglecting powers of above (since , while cross terms and produce higher powers):
4. Equate coefficients to find $a$ and $b$.
Substitute this back into the original expression:
Comparing this with the given form , we get:
and .
,
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