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Question

The coefficient of $e^{ikx}$ in the Fourier expansion of $u(x) = A\sin^2(ax)$ for $k = -2a$ is

The correct answer is
$-A/4$

Find Fourier Expansion Coefficient for $A\sin^2(ax)$

This solution details finding the coefficient of the complex exponential term $e^{ikx}$ within the Fourier expansion of the function $u(x) = A\sin^2(ax)$, specifically for the case where $k = -2a$. We will use trigonometric identities to simplify the function and express it in terms of complex exponentials.

Trigonometric Simplification

First, rewrite $u(x)$ using the identity $\sin^2(\theta) = \frac{1 - \cos(2\theta)}{2}$:

$u(x) = A \left( \frac{1 - \cos(2ax)}{2} \right)$

$u(x) = \frac{A}{2} - \frac{A}{2}\cos(2ax)$

Expressing in Complex Exponentials

Next, use the identity $\cos(\phi) = \frac{e^{i\phi} + e^{-i\phi}}{2}$ to convert the cosine term:

$\cos(2ax) = \frac{e^{i(2ax)} + e^{-i(2ax)}}{2}$

Substitute this back into the expression for $u(x)$:

$u(x) = \frac{A}{2} - \frac{A}{2} \left( \frac{e^{i(2ax)} + e^{-i(2ax)}}{2} \right)$

Simplify the expression:

$u(x) = \frac{A}{2} - \frac{A}{4} e^{i(2ax)} - \frac{A}{4} e^{-i(2ax)}$

This can be written in the general form $u(x) = \sum c_k e^{ikx}$ as:

$u(x) = \frac{A}{2}e^{i(0)x} - \frac{A}{4}e^{i(2a)x} - \frac{A}{4}e^{i(-2a)x}$

Identifying the Specific Coefficient

The Fourier expansion represents the function as a sum of terms $c_k e^{ikx}$. We are looking for the coefficient corresponding to $k = -2a$. In the derived expression:

$u(x) = \frac{A}{2}e^{i(0)x} - \frac{A}{4}e^{i(2a)x} - \frac{A}{4}e^{i(-2a)x}$

The term with $k = -2a$ is $- \frac{A}{4}e^{i(-2a)x}$.

Therefore, the coefficient of $e^{ikx}$ for $k = -2a$ is $ - \frac{A}{4}$.

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Important Questions from Fourier Series

  1. If we use the Fourier transform ϕ(x, y) =  \(\int {{{\rm{e}}^{{\rm{ikx}}}}} {ϕ _{\rm{k}}}\left( {\rm{y}} \right){\rm{dk}}\)  to solve the partial differential equation  \({\rm{ - }}\frac{{{\partial ^2}ϕ \left( {x,y} \right)}}{{\partial {y^2}}}\, - \,\frac{1}{{{y^2}}}\frac{{{\partial ^2}ϕ \left( {x,y} \right)}}{{\partial {x^2}}} + \frac{{{m^2}}}{{{y^2}}}ϕ \left( {x,y} \right) = 0\)  in the half-plane {(x, y) : -∞ < x < ∞, 0 < y < ∞} the Fourier modes ϕ k(y) depend on y as y α  and y β . The values of α and β are  

  2. When a time-domain signal is converted into its Fourier representation, which of the following is/are conserved?

    I. Energy

    II. Power

  3. The trigonometric Fourier series of a periodic time function can have

  4. The Fourier series expansion of x3 in the interval −1 ≤ x < 1 with periodic continuation has

  5. The Fourier series to represent x-x2 for –π ≤ x ≤ π is given by \(x - {x^2} = \frac{{{a_0}}}{2} + \mathop \sum \limits_{n = 1}^\infty {a_n}cosnx + \mathop \sum \limits_{n = 1}^\infty {b_n}sinnx\)

    The value of a0 (round off to two decimal places), is
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