Limits, Continuity & Differentiability
Second Derivatives & Implicit Functions
Grade 12
<p>For the curve <span class="math">\sin x + \sin y = 1</span> lying in the first quadrant, there exists a constant <span class="math">a</span> for which <span class="math">\lim_{x \to 0} x^a \frac{d^2y}{dx^2} = L</span> (not zero). Find <span class="math">2a</span>.</p>
Step-by-Step Solution
Key Concept: We need to find the behavior of the second derivative near x = 0 using implicit differentiation. The curve sin x + sin y = 1 near x = 0 requires analyzing y's Taylor expansion to determine what power of x makes the limit finite and non-zero.
Step 1: Determine the initial conditions at $x=0$.
We are given the equation $\sin x + \sin y = 1$. To find the value of $y$ when $x=0$, we substitute $x=0$ into the equation.
$$ \sin(0) + \sin y = 1 $$
$$ 0 + \sin y = 1 $$
$$ \sin y = 1 $$
For $y$ in the first quadrant, this implies $y = \frac{\pi}{2}$.
So, at $x=0$, we have $y=\frac{\pi}{2}$.
Step 2: Differentiate the given equation implicitly with respect to $x$ to find $\frac{dy}{dx}$.
Differentiating $\sin x + \sin y = 1$ with respect to $x$:
$$ \frac{d}{dx}(\sin x) + \frac{d}{dx}(\sin y) = \frac{d}{dx}(1) $$
$$ \cos x + \cos y \cdot \frac{dy}{dx} = 0 $$
Now, we solve for $\frac{dy}{dx}$:
$$ \cos y \cdot \frac{dy}{dx} = -\cos x $$
$$ \frac{dy}{dx} = -\frac{\cos x}{\cos y} $$
Let's evaluate $\frac{dy}{dx}$ at $x=0$ (where $y=\frac{\pi}{2}$):
$$ \frac{dy}{dx} \Big|_{x=0} = -\frac{\cos(0)}{\cos(\frac{\pi}{2})} = -\frac{1}{0} $$
This indicates that $\frac{dy}{dx}$ is undefined at $x=0$, suggesting that we need to use series expansions to properly analyze the behavior near $x=0$.
Step 3: Express $\sin y$ using the constraint and introduce a substitution for $y$ near $\frac{\pi}{2}$.
From the given equation, $\sin y = 1 - \sin x$.
We use the Maclaurin series expansion for $\sin x$:
$$ \sin x = x - \frac{x^3}{3!} + \frac{x^5}{5!} - \dots = x - \frac{x^3}{6} + O(x^5) $$
Substituting this into the expression for $\sin y$:
$$ \sin y = 1 - \left(x - \frac{x^3}{6} + O(x^5)\right) = 1 - x + \frac{x^3}{6} + O(x^5) $$
Since $y \to \frac{\pi}{2}$ as $x \to 0$, let $y = \frac{\pi}{2} + u$, where $u$ is a small quantity that approaches $0$ as $x \to 0$.
Now, express $\sin y$ in terms of $u$:
$$ \sin y = \sin\left(\frac{\pi}{2} + u\right) = \cos u $$
Using the Maclaurin series expansion for $\cos u$:
$$ \cos u = 1 - \frac{u^2}{2!} + \frac{u^4}{4!} - \dots = 1 - \frac{u^2}{2} + \frac{u^4}{24} + O(u^6) $$
Step 4: Equate the two series expansions for $\sin y$ to find $u$ in terms of $x$.
By equating the two expressions for $\sin y$ from Step 3:
$$ 1 - \frac{u^2}{2} + \frac{u^4}{24} + O(u^6) = 1 - x + \frac{x^3}{6} + O(x^5) $$
Subtracting $1$ from both sides:
$$ -\frac{u^2}{2} + \frac{u^4}{24} + O(u^6) = -x + \frac{x^3}{6} + O(x^5) $$
For small $x$, the dominant term on the right is $-x$. This implies that the dominant term for $-\frac{u^2}{2}$ must be $-x$.
$$ -\frac{u^2}{2} \approx -x \implies u^2 \approx 2x $$
So, $u$ is of the order $\sqrt{x}$. We can approximate $u^4$ as $(2x)^2 = 4x^2$.
$$ \frac{u^2}{2} = x - \frac{x^3}{6} + O(x^5) $$
$$ u^2 = 2x - \frac{x^3}{3} + O(x^5) $$
Now, take the square root to find $u$:
$$ u = \sqrt{2x - \frac{x^3}{3} + O(x^5)} $$
Factor out $2x$:
$$ u = \sqrt{2x \left(1 - \frac{x^2}{6} + O(x^4)\right)} $$
$$ u = \sqrt{2x} \left(1 - \frac{x^2}{6} + O(x^4)\right)^{1/2} $$
Using the generalized binomial theorem $(1+z)^\alpha \approx 1 + \alpha z$ for small $z$:
$$ u = \sqrt{2x} \left(1 + \frac{1}{2}\left(-\frac{x^2}{6}\right) + O(x^4)\right) $$
$$ u = \sqrt{2x} \left(1 - \frac{x^2}{12} + O(x^4)\right) $$
$$ u = \sqrt{2x} - \frac{x^2\sqrt{2x}}{12} + O(x^{4}\sqrt{x}) $$
$$ u = \sqrt{2}x^{1/2} - \frac{\sqrt{2}}{12}x^{5/2} + O(x^{9/2}) $$
Step 5: Compute $\frac{dy}{dx}$ using the series expansion of $u$.
Since $y = \frac{\pi}{2} + u$, we have $\frac{dy}{dx} = \frac{du}{dx}$.
Differentiate the expression for $u$ found in Step 4:
$$ \frac{dy}{dx} = \frac{d}{dx} \left(\sqrt{2}x^{1/2} - \frac{\sqrt{2}}{12}x^{5/2} + O(x^{9/2})\right) $$
$$ \frac{dy}{dx} = \sqrt{2} \cdot \frac{1}{2}x^{-1/2} - \frac{\sqrt{2}}{12} \cdot \frac{5}{2}x^{3/2} + O(x^{7/2}) $$
$$ \frac{dy}{dx} = \frac{\sqrt{2}}{2\sqrt{x}} - \frac{5\sqrt{2}}{24}x^{3/2} + O(x^{7/2}) $$
$$ \frac{dy}{dx} = \frac{1}{\sqrt{2x}} - \frac{5\sqrt{2}}{24}x^{3/2} + O(x^{7/2}) $$
Step 6: Compute $\frac{d^2y}{dx^2}$ by differentiating $\frac{dy}{dx}$.
Differentiate the expression for $\frac{dy}{dx}$ from Step 5:
$$ \frac{d^2y}{dx^2} = \frac{d}{dx} \left(\frac{1}{\sqrt{2}}x^{-1/2} - \frac{5\sqrt{2}}{24}x^{3/2} + O(x^{7/2})\right) $$
$$ \frac{d^2y}{dx^2} = \frac{1}{\sqrt{2}} \cdot \left(-\frac{1}{2}\right)x^{-3/2} - \frac{5\sqrt{2}}{24} \cdot \frac{3}{2}x^{1/2} + O(x^{5/2}) $$
$$ \frac{d^2y}{dx^2} = -\frac{1}{2\sqrt{2}}x^{-3/2} - \frac{5\sqrt{2}}{16}x^{1/2} + O(x^{5/2}) $$
The dominant term as $x \to 0$ is the term with the most negative power of $x$:
$$ \frac{d^2y}{dx^2} \approx -\frac{1}{2\sqrt{2}}x^{-3/2} $$
Step 7: Determine the constant $a$ such that $\lim_{x \to 0} x^a \frac{d^2y}{dx^2}$ is a non-zero finite value $L$.
We have $\frac{d^2y}{dx^2} \approx -\frac{1}{2\sqrt{2}}x^{-3/2}$.
We need to find $a$ such that the limit of $x^a \cdot \left(-\frac{1}{2\sqrt{2}}x^{-3/2}\right)$ as $x \to 0$ is a non-zero constant.
$$ \lim_{x \to 0} x^a \left(-\frac{1}{2\sqrt{2}}x^{-3/2}\right) = \lim_{x \to 0} \left(-\frac{1}{2\sqrt{2}}x^{a - 3/2}\right) $$
For this limit to be finite and non-zero, the exponent of $x$ must be $0$:
$$ a - \frac{3}{2} = 0 $$
$$ a = \frac{3}{2} $$
With this value of $a$, the limit $L = -\frac{1}{2\sqrt{2}}$, which is non-zero.
Step 8: Calculate the value of $2a$.
Given $a = \frac{3}{2}$, we calculate $2a$:
$$ 2a = 2 \times \frac{3}{2} = 3 $$
The final answer is $\boxed{3}$.
Correct Answer: 2