Fractional Calculus on Sinusoidal functions

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Discussion Overview

The discussion revolves around the application of fractional calculus to sinusoidal functions, specifically exploring the phase dependence of these functions when subjected to non-integer derivatives. Participants are examining the implications of fractional derivatives in signal analysis and the mathematical properties associated with them.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant inquires about the phase dependence of sinusoidal functions under non-integer derivatives, seeking a formula for the phase shift.
  • Another participant presents a formula suggesting that the fractional derivative of a sine function results in a phase shift proportional to the derivative order.
  • Some participants express surprise at the simplicity of the results, while others propose more complex relationships involving the derivative order and phase shifts.
  • A participant challenges the assumption that fractional derivatives follow the index law, providing counterexamples and emphasizing the need for clarity on the type of fractional derivative used.
  • There is mention of the Riemann-Liouville fractional derivative and its implications for the exponential function, indicating that different definitions may yield different results.
  • Several participants highlight the importance of specifying the base point and the domain of the function when discussing fractional derivatives.
  • One participant suggests using a specific form of function for calculating fractional derivatives, referencing historical studies by Liouville.
  • Another participant seeks clarification on the concept of the base point and its relevance to their calculations.

Areas of Agreement / Disagreement

Participants express a range of views on the properties and implications of fractional derivatives, with no consensus reached on the correct approach or definition to use. Some participants agree on the simplicity of certain results, while others emphasize the complexity and variability based on definitions and contexts.

Contextual Notes

Limitations include the need for clarity on the definition of fractional derivatives being used, the significance of the base point, and how the domain of the sine function affects the results. These factors contribute to the complexity of the discussion and the absence of a definitive answer.

Who May Find This Useful

This discussion may be of interest to those studying fractional calculus, signal analysis, and the mathematical properties of sinusoidal functions, particularly in advanced applications within physics and engineering.

TheDestroyer
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Hello guys :),

I have a question which I think is very advanced and weird. But I need the answer for some signal analysis purpose.

As we know, the derivative of a sine function, per se, shifts the phase, by Pi/2; i.e.,

f(x) = A sin (w t)
df(x)/dt = A sin (w t + Pi/2) = A cos(w t)

and of course, the integral does the opposite:
Integral(f(x) dx) = A sin(w t - Pi/2) = - A cos(w t).

As we know, there's something called fractional calculus, which involves taking derivates in non-integer orders. So for example the derivative of

g(x) = x

of the order 1/2, would be something like

(d^(1/2) g(x))/(dx^(1/2)) = Gamma(1/2) x^(1/2),

where Gamma(1/2) is the Euler gamma function (I'm not sure whether inside gamma is over 1/2 or 3/2, but whatever).

------------

My question:

So my question is, could you guys help me in finding the phase dependence of sinusoidal functions on non-integer derivatives? so I'm looking for something like:

d^(n) f(x)/dx^n = A sin(w t + k(n)),

where n is a real number, and k(n) is the phase dependence on the derivative order, n, that I'm looking for.

Thank you for any efforts :)
 
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[itex]\frac{d^{\alpha}Asin(t)}{dt} = Asin(t + \alpha\pi/2)[/itex], this fractional derivative is for w=1.
 
Thank you for your answer.

Is it linear like that? I'm surprised! it's so simple! I thought it would be a little but more complicated! The results from the signal shifting I'm doing gives it something like

Phi = Pi/2 * ArcTan(1 - Exp(n))

proportionality between for n=[0,1] with some coefficients, where n is the derivative order...

Any explanation?
 
Yes is as simple as that. If you believe you have a different shift try the following test:

- compute the half derivative of sin(t), [itex]g(t) = \frac{d^{\frac{1}{2}}sin(t)}{dt}[/itex]
- compute the half derivative of g(t), [itex]h(t) = \frac{d^{\frac{1}{2}}g(t)}{dt}[/itex]

In the end you should have [itex]h(t) = sin(t+\pi/2)[/itex] hecause h(t) is the first derivative of sin(t)

With the simple formula you get [itex]g(t) = sin(t+\pi/4)[/itex] and [itex]h(t) = sin(t+\pi/4 + \pi/4) = sin(t+\pi/2)[/itex]

You can obtain the shift formula by playing with the fractional derivative of the exponential function.
 
atomthick said:
Yes is as simple as that.

Absolutely not!

First, fractional derivatives do not satisfy the index law in general. For example take f(x) = 1 and then [itex]D^{\frac12} \frac{d}{dx} 1 = 0[/itex] but [itex]\frac{d}{dx} D^{\frac12}1 = \frac{d}{dx} \frac{1}{\sqrt{\pi x}} \neq 0[/itex]. In general [itex]D^p D^q \neq D^q D^p[/itex].

Secondly, the Riemann-Liouville fractional derivative of the exponential function with base point a=0 leads to the http://en.wikipedia.org/wiki/Mittag-Leffler_function" , not another exponential.

In fractional calculus you must be explicit in which fractional derivative you use (yes there is more than one) and specify the base point where appropriate.
 
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Thank you guys for your answers.

pwsnafu said:
Absolutely not!

First, fractional derivatives do not satisfy the index law in general. For example take f(x) = 1 and then [itex]D^{\frac12} \frac{d}{dx} 1 = 0[/itex] but [itex]\frac{d}{dx} D^{\frac12}1 = \frac{d}{dx} \frac{1}{\sqrt{\pi x}} \neq 0[/itex]. In general [itex]D^p D^q \neq D^q D^p[/itex].

Secondly, the Riemann-Liouville fractional derivative of the exponential function with base point a=0 leads to the http://en.wikipedia.org/wiki/Mittag-Leffler_function" , not another exponential.

In fractional calculus you must be explicit in which fractional derivative you use (yes there is more than one) and specify the base point where appropriate.

So what's the correct answer please, if I have to use such a function? is it like the guys have said, concerning this a special simple case, or is it more complicated?
 
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TheDestroyer said:
So what's the correct answer please, if I have to use such a function? is it like the guys have said, concerning this a special simple case, or is it more complicated?

I can't answer because you haven't given enough information. You need to specify
  1. What the definition of fractional derivative you intend to use,
  2. If there is a base point, you need to specify that,
  3. The domain of the function you intend to integrate/differentiate.

And yes they are all significant. If you treat sine as a function whose domain is [0,2pi] you will get a different result to sine with domain over all reals, which is different again compared to sine with domain of the unit circle.

There is no "correct" answer.
You just choose the definition which has the properties you want in the application. The only advice I can give you is read lots of papers in your field. The convention used in one field will differ from others.
 
For index values a with 0 < a < 1 the fractional derivative is comutative and additive.
 
atomthick said:
For index values a with 0 < a < 1 the fractional derivative is comutative and additive.

For Riemann-Liouville yes. Don't know if it is true for all one parameter fractional derivatives though. For two or more parameter operators, obviously not.
 
  • #10
Thank you for your replies guys!

I'm not that familiar with fractional derivatives to understand all the terms you mentioned. The thing I can tell you is that the purpose of the derivatives is shifting the phase between -Pi/2 and Pi/2; i.e, the derivative order has to be

-1 <= a <= 1

What's inside the sin is a real number, and I don't really know what basepoint mean. Could you please explain more so that I can provide sufficient information?
 
  • #11
I've based my calculations on functions of a special form for which Liouville began his studies on fractional derivatives.

[itex]f(x)=\sum^{\infty}_{n=0}c_{n}e^{a_{n}x}, Re(a_{n}) > 0[/itex]

for which the fractional derivatives are

[itex]D^{\alpha}f(x)=\sum^{\infty}_{n=0}c_{n}a_{n}^{\alpha}e^{a_{n}x}, Re(a_{n}) > 0[/itex]

You can write [itex]sin(x)=\frac{1}{2i}e^{ix} - \frac{1}{2i}e^{-ix}[/itex] and try to use the above formula to find out the derivative but you have to take a limit case because Re(i) = 0

Here is a link http://www.umw.edu/cas/math/students/documents/damian1.pdf
 
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  • #12
Thanks a lot. I'll try :)
 
  • #13
TheDestroyer said:
thing I can tell you is that the purpose of the derivatives is shifting the phase between -Pi/2 and Pi/2; i.e, the derivative order has to be
In that case, yep atom's answer is what you want.

What's inside the sin is a real number, and I don't really know what basepoint mean. Could you please explain more so that I can provide sufficient information?

The most standard definition of fractional calculus is the Riemann-Liouville. Given a function [itex]f:[a,b]\rightarrow[/itex] we define the fractional integral of order [itex]Re \alpha>0[/itex] as
[tex]D^\alpha_{a+}f(x) := \frac{1}{\Gamma(\alpha)}\int_a^x (x-t)^{\alpha-1} f(t) dt.[/tex]
The base point refers to that a. Different choices of a result in different different answers when you calculate the integral. The Liouville definition above corresponds to [itex]a\rightarrow -\infty[/itex]. This is why it is a limit.
 
  • #14
Thanks a lot mate :)

I'll go for that as well ^^
 

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