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موجک
hosein بازدید : 221 چهارشنبه 13 شهریور 1392 نظرات (0)

موجک هار سری خاصی از توابع است که اکنون به عنوان اولین موجک شناخته می‌شود. این سری اولین بار توسط آلفرد هار، ریاضیدان مجاری در سال ۱۹۰۹ پیشنهاد شد[۱]. موجک هار ساده‌ترین موجک ممکن می‌باشد. مشکل این موجک این است که پیوسته نیست و در نتیجه مشتق‌پذیر نمی‌باشد. موجک مادر هار به شکل زیر تعریف می‌شود:

\psi(t) = \begin{cases}1 \quad & 0 \leq  t < 1/2,\\
 -1 & 1/2 \leq t < 1,\\0 &\mbox{otherwise.}\end{cases}

و تابع مقیاس‌کننده نیز برابر است با:

\phi(t) = \begin{cases}1 \quad & 0 \leq  t < 1,\\0 &\mbox{otherwise.}\end{cases}

hosein بازدید : 21 چهارشنبه 13 شهریور 1392 نظرات (0)

In continuous wavelet transforms, a given signal of finite energy is projected on a continuous family of frequency bands (or similar subspaces of the Lp function space L2(R) ). For instance the signal may be represented on every frequency band of the form [f, 2f] for all positive frequencies f > 0. Then, the original signal can be reconstructed by a suitable integration over all the resulting frequency components.

The frequency bands or subspaces (sub-bands) are scaled versions of a subspace at scale 1. This subspace in turn is in most situations generated by the shifts of one generating function ψ in L2(R), the mother wavelet. For the example of the scale one frequency band [1, 2] this function is

psi(t)=2,operatorname{sinc}(2t)-,operatorname{sinc}(t)=frac{sin(2pi t)-sin(pi t)}{pi t}

with the (normalized) sinc function. That, Meyer's, and two other examples of mother wavelets are:

The subspace of scale a or frequency band [1/a, 2/a] is generated by the functions (sometimes called child wavelets)

psi_{a,b} (t) = frac1{sqrt a }psi left( frac{t - b}{a} right),

where a is positive and defines the scale and b is any real number and defines the shift. The pair (a, b) defines a point in the right halfplane R+ × R.

The projection of a function x onto the subspace of scale a then has the form

x_a(t)=int_R WT_psi{x}(a,b)cdotpsi_{a,b}(t),db

with wavelet coefficients

WT_psi{x}(a,b)=langle x,psi_{a,b}rangle=int_R x(t){psi_{a,b}(t)},dt.

See a list of some Continuous wavelets.

For the analysis of the signal x, one can assemble the wavelet coefficients into a scaleogram of the signal.

hosein بازدید : 17 چهارشنبه 13 شهریور 1392 نظرات (0)

A wavelet is a wave-like oscillation with an amplitude that begins at zero, increases, and then decreases back to zero. It can typically be visualized as a "brief oscillation" like one might see recorded by a seismograph or heart monitor. Generally, wavelets are purposefully crafted to have specific properties that make them useful for signal processing. Wavelets can be combined, using a "reverse, shift, multiply and integrate" technique called convolution, with portions of a known signal to extract information from the unknown signal.

Seismic Wavelet

For example, a wavelet could be created to have a frequency of Middle C and a short duration of roughly a 32nd note. If this wavelet was to be convolved with a signal created from the recording of a song, then the resulting signal would be useful for determining when the Middle C note was being played in the song. Mathematically, the wavelet will resonate if the unknown signal contains information of similar frequency – just as a tuning fork physically resonates with sound waves of its specific tuning frequency. This concept of resonance is at the core of many practical applications of wavelet theory.

As a mathematical tool, wavelets can be used to extract information from many different kinds of data, including – but certainly not limited to – audio signals and images. Sets of wavelets are generally needed to analyze data fully. A set of "complementary" wavelets will decompose data without gaps or overlap so that the decomposition process is mathematically reversible. Thus, sets of complementary wavelets are useful in wavelet based compression/decompression algorithms where it is desirable to recover the original information with minimal loss.

In formal terms, this representation is a wavelet series representation of a square-integrable function with respect to either a complete, orthonormal set of basis functions, or an overcomplete set or frame of a vector space, for the Hilbert space of square integrable functions.

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