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<math>G' (t,a,b) = \frac{a}{(2\pi)^{-1/2}}(t - b) e^{[\frac{-(t-b)^2}{2a^2}]}</math>
Once a "mother wavelet" is chosen, the continuous wavelet transform is carried out as a continuous, [[square-integrable
:<math>X_w(a,b)=\frac{1}{\sqrt{a}} \int_{-\infty}^{\infty} x(t)\psi^{\ast}\left(\frac{t-b}{a}\right)\, dt</math>
where <math>\psi(t)</math> is a continuous function in both the time ___domain and the frequency ___domain called the mother wavelet and <math>^{\ast}</math> represents the operation of
By calculating <math>X_w(a,b) </math> for subsequent wavelets that are derivatives of the mother wavelet, singularities can be identified. Successive derivative wavelets remove the contribution of lower order terms in the signal, allowing the maximum <math>h_i</math> to be detected. (Recall that when taking derivatives, lower order terms become 0.) This is the "modulus maxima".
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