Chapter 12: Problem 4
The clipped response of a half-wave rectifier is the periodic function \(f(t)\) of period \(2 \pi\) defined over the period \(0 \leq t \leq 2 \pi\) by $$ f(t)=\left\\{\begin{array}{cl} 5 \sin t & (0 \leqslant t \leqslant \pi) \\ 0 & (\pi \leqslant t \leq 2 \pi) \end{array}\right. $$ Express \(f(t)\) as a Fourier series expansion.
Short Answer
Step by step solution
Calculate Fourier Coefficients
Calculate Coefficients a_n
Calculate Coefficients b_n
Express f(t) as a Fourier Series
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Rectifier Circuits
- In our exercise, the rectifier output is represented by the periodic function \( f(t) = \begin{cases} 5 \sin t & (0 \leq t \leq \pi) \ 0 & (\pi \leq t \leq 2\pi) \end{cases} \).
- This processed waveform is inherently periodic and forms an essential part of learning about how rectifiers function.
- The Fourier series lets us analyze and understand these functions, highlighting their transformation from time to frequency domain representation.
Periodic Functions
- The function \( f(t) \) in the problem has a period of \( 2\pi \), meaning it repeats its shape every \( 2\pi \) interval.
- Recognizing a function's periodicity is important for applying Fourier series, as it simplifies complex signals into a series of sinusoidal components.
- This simplification helps in easier analysis and synthesis of signals, making the frequency domain analysis vital for understanding real-world waveforms.
Fourier Coefficients
- In the exercise, Fourier coefficients \( a_n \) and \( b_n \) are calculated as the integrals of \( f(t) \) with \( \cos(nt) \) and \( \sin(nt) \), respectively, over a function's period.
- The coefficient \( a_0 \) is the average value or the DC component of the function, which was found to be zero in this case.
- The exercise showed that \( a_n \) values vanish due to orthogonality, leaving certain \( b_n \) values to represent the function.
Trigonometric Identities
- In the exercise, to find \( b_n \), the identity \( \sin A \sin B = \frac{1}{2} \left( \cos(A-B) - \cos(A+B) \right) \) is used. This helps in breaking down sine products into simpler components.
- Such identities reduce complex trigonometric expressions into a form that can be easier to integrate.
- Knowing how to apply these correctly is crucial for solving Fourier series problems efficiently, as seen in the step-by-step solution provided.