16.5
Parseval's Theorem
Parseval's theorem states that if a function is periodic, then the average power of the signal over one period equals the sum of the squared magnitudes of all the complex Fourier coefficients.
To validate Parseval's theorem, assume that the function has a complex Fourier series of a standard form. Substituting this and solving further gives the proof of the theorem.
Interestingly, Parseval's theorem can also be expressed in terms of the Fourier coefficients of the trigonometric Fourier series.
In audio processing, Parseval's theorem is used to compare the energy of an original sound wave with its compressed version.
The engineering interpretation of this theorem provides practical insights. If the function represents an electrical signal, such as current or voltage, then the square of the function represents the instantaneous power in a 1-ohm resistor.
This theorem also relates the energy dissipated in the resistor during one period to the Fourier series, providing two different expressions - one in terms of the trigonometric Fourier series and another in terms of the amplitude phase Fourier series.
Parseval's theorem is a fundamental concept in signal processing and harmonic analysis. It asserts that for a periodic function, the average power of the signal over one period equals the sum of the squared magnitudes of all its complex Fourier coefficients. This theorem, named after Marc-Antoine Parseval, provides a powerful tool for analyzing the energy distribution in signals.
Interestingly, Parseval's theorem also holds for the trigonometric form of the Fourier series, which expresses a function in terms of sine and cosine functions. Here, the Fourier coefficients can be related to the trigonometric series coefficients, allowing the theorem to be applied in this alternate form.
To validate Parseval's theorem, we start by considering a function x(t) with a complex Fourier series representation:
Where Cn are the complex Fourier coefficients, and ω0 is the fundamental angular frequency. The theorem states:
Where T is the period of the function. Substituting the Fourier series into the left-hand side and solving confirms the equality, thus proving the theorem.
Parseval's theorem is crucial in practical applications, particularly in audio processing. It allows for comparing the energy contained in an original sound wave to that in its compressed version. This comparison is essential in ensuring that the compression process does not significantly degrade the quality of the audio signal by losing too much energy.
From an engineering perspective, Parseval's theorem offers valuable insights. For instance, if the function in question represents an electrical signal such as current or voltage, then the square of this function represents the instantaneous power dissipated in a 1-ohm resistor. Consequently, the theorem links the energy dissipated in the resistor over one period to the Fourier series representation of the signal. This relationship is expressed in two different forms: one using the trigonometric Fourier series and the other using the amplitude-phase form of the Fourier series. Thus, Parseval's theorem not only serves as a powerful analytical tool but also bridges theoretical concepts with practical engineering applications.
Parseval's theorem states that if a function is periodic, then the average power of the signal over one period equals the sum of the squared magnitudes of all the complex Fourier coefficients.
To validate Parseval's theorem, assume that the function has a complex Fourier series of a standard form. Substituting this and solving further gives the proof of the theorem.
Interestingly, Parseval's theorem can also be expressed in terms of the Fourier coefficients of the trigonometric Fourier series.
In audio processing, Parseval's theorem is used to compare the energy of an original sound wave with its compressed version.
The engineering interpretation of this theorem provides practical insights. If the function represents an electrical signal, such as current or voltage, then the square of the function represents the instantaneous power in a 1-ohm resistor.
This theorem also relates the energy dissipated in the resistor during one period to the Fourier series, providing two different expressions - one in terms of the trigonometric Fourier series and another in terms of the amplitude phase Fourier series.
From Chapter 16:
Now Playing
16.5 : Parseval's Theorem
Fourier Series
1.6K Views
16.1 : Trigonometric Fourier series
Fourier Series
1.4K Views
16.2 : Exponential Fourier series
Fourier Series
1.3K Views
16.3 : Properties of Fourier series I
Fourier Series
1.1K Views
16.4 : Properties of Fourier series II
Fourier Series
923 Views
16.6 : Convergence of Fourier Series
Fourier Series
688 Views
16.7 : Discrete-Time Fourier Series
Fourier Series
1.1K Views