Fast Forward Fourier Transformer

Time series Calculator

Explanation of FFT and IFFT

Fast Fourier Transform (FFT)

FFT is an algorithm used to compute the Discrete Fourier Transform (DFT) and its inverse efficiently. The DFT converts a sequence of values into components of different frequencies, which is useful in many fields such as signal processing, image analysis, and data compression.

Mathematical Formulation:

Given a sequence x[n] of length n, the DFT is defined by:

where:

X[k] is the k-th frequency component.

x[n] is the n-th time-domain sample.

  • N is the total number of samples.
  • j is the imaginary.

The FFT algorithm reduces the computational complexity of calculating the DFT from O(N2)  to O(Nlog⁡N). This is achieved by decomposing the DFT into smaller DFTs recursively, exploiting symmetries and periodicities in the Fourier coefficients.

Inverse Fast Fourier Transform (IFFT)

IFFT is used to convert data from the frequency domain back into the time domain. It is essentially the reverse operation of the FFT.

Mathematical Formulation:

Given the frequency domain sequence X[k], the IFFT x[n] is defined by:

where:

x[n] is the n-th time-domain sample.

X[k] is the k-th frequency component.

  • N is the total number of samples.

In practice, both FFT and IFFT are implemented efficiently in numerical libraries and software packages, making them essential tools for many digital signal processing tasks.

References:

  1. Numerical Recipes: The Art of Scientific Computing by William H. Press et al.

    • This book provides a comprehensive introduction to the algorithms used in FFT and IFFT, along with their implementation details.
  2. The Fast Fourier Transform and its Applications by E. Oran Brigham.

    • A classic text that covers the theory and applications of FFT, providing a detailed explanation of the algorithms and their use cases.
  3. Understanding Digital Signal Processing by Richard G. Lyons.

    • This book provides a practical approach to understanding FFT and IFFT, including numerous examples and exercises.
  4. Fourier Analysis and Its Applications by Gerald B. Folland.

    • A more mathematical approach to Fourier analysis, including a detailed exploration of the FFT and its theoretical underpinnings.

These resources provide a range of perspectives on FFT and IFFT, from practical implementation to theoretical foundations.

Description of Input Parameters for Time Series Generator

The following explains the inputs required for generating time-series data using various mathematical functions like cosine, sine, tangent, cotangent, and power functions. These inputs allow flexibility in defining the function and controlling the sampling rate and duration.

1. Function Type

Description: Specifies the type of mathematical function to generate the time series.
Accepted Values:

  • cos: Cosine function : \(a \cdot \cos(2 \cdot \pi \cdot b \cdot t + c)\)
  • sin: Sine function : \(a \cdot \sin(2 \cdot \pi \cdot b \cdot t + c)\)
  • tan: Tangent function : \(a \cdot \tan(2 \cdot \pi \cdot b \cdot t + c)\)
  • cot: Cotangent function : \(\frac{a}{\tan(2 \cdot \pi \cdot b \cdot t + c)}\)
  • pow: Power function : \(a \cdot t^b + c\)

2. Amplitude (a)

Description: Amplitude or scaling factor for the function.
Effect: Scales the output of the function by this value.
Example:

  • For cos: \(a = 2\), the function becomes \(2 \cdot \cos(…)\).
  • For pow: \(a = 3\), the function becomes \(3 \cdot t^b + c\).

3. Frequency or Exponent (b)

Description: Frequency parameter (in Hz) for trigonometric functions (cos, sin, tan, and cot). For pow, it represents the exponent.
Effect:

  • For trigonometric functions, a higher value of \(b\) increases the oscillation frequency.
  • For pow, it determines the exponent \(t^b\).

Example:

  • For cos: \(b = 2\), the function oscillates twice per second.
  • For pow: \(b = 2\), the function becomes \(t^2\).

4. Phase Offset or Constant (c)

Description: Phase offset for trigonometric functions or a constant for the power function.
Effect:

  • For trigonometric functions, shifts the waveform horizontally by \(c\) radians.
  • For pow, adds \(c\) to the computed value \(a \cdot t^b\).

Example:

  • For sin: \(c = \frac{\pi}{2}\), the waveform shifts by \(\frac{\pi}{2}\) radians.
  • For pow: \(c = 5\), the function becomes \(a \cdot t^b + 5\).

5. Sampling Rate

Description: The number of samples taken per second from the continuous function.
Effect: Determines the resolution of the generated time series. Higher values produce more precise data.
Constraints: Must be greater than 0.
Example:

  • \(\text{sampling rate} = 100\): 100 samples are taken every second.

6. Duration

Description: The total duration (in seconds) for which the time series is generated.
Effect: Controls the length of the time series.
Constraints: Must be greater than 0.
Example:

  • \(\text{duration} = 2\): Time series is generated for 2 seconds.












We are an experienced team for FEM analysis

Information

contact@idesignbest.com

4300 St. Valentin

Austria

This website uses cookies to provide you with the best browsing experience.

Accept
Decline