Normalising a velocity spectrum

In summary, the normalisation condition for a velocity distribution is that the area under the graph (the integral of the function w.r.t. velocity) is equal to 1.
  • #1
natski
267
2
For any given velocity distribution, you have a y-axis with probability and an x-axis of velocity. Without really thinking much about it, I had assumed the normalisation condition was that the area under the graph (the integral of the function w.r.t. velocity) would be equal to 1. Of course, the area under the graph has the dimensions of velocity and so it doesn't make sense to set the area to 1.

So my question is, what IS the normalisation condition for a velocity distribution??
 
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  • #2
The y-axis is the PROBABILITY, not the velocity, so normalize to 1.
 
  • #3
This is what I said? The y-axis is probability.

But I don't think it is right to set the mean velocity to a probability of 1 because now the total probability under the graph will be greater than 1.
 
  • #4
\int Pdx=1, where P is the probability distribution. P is on the y axis.
\int vPdx=<v>.
 
  • #5
natski,

The y-axis is the probability distribution (say f), not the probability (say P).
The probability distribution with respect to the velocity v is defined such that

dp = f(v) dv​

gives the probability that the velocity is in the interval [v,v+dv].

The probability that the velocity is between v1 and v2 may be obtained by integration:

[tex]P(v1,v2) = \int_{v1}^{v2} f(v') dv'[/tex]​

This last expression is also a probability, also called cumulated probability.

The dimensions of f(v) are the inverse of the dimensions of a velocity.
The dimensions of P(v1,v2) are those of a simple number, no dimension.

In practical applications, like particle size analysis in the industry or sales statistics or reliability data ..., I prefer to use the cumulated probability. The probability density is not convenient in these practical situations. For example the area under a curve is not really a visible data while the value of the cumulated probability along the y-axis is a clear information. And of course, there is this problem with "strange" units for f . In theoretical physics of course the probability density is more convenient.

Michel
 
Last edited:
  • #6
Just wanted to say thanks for your help on this. Problem now solved.
 

Related to Normalising a velocity spectrum

1. What is normalising a velocity spectrum?

Normalising a velocity spectrum is the process of adjusting the velocity values in a spectrum to a common scale. This is done to remove any variations or biases in the data and make it easier to compare different spectra.

2. Why is normalisation necessary for velocity spectra?

Normalisation is necessary because velocity spectra can have different units or scales, making it difficult to compare them directly. By normalising the spectra, we can remove these differences and focus on the underlying patterns and trends in the data.

3. How is normalisation done for velocity spectra?

Normalisation is typically done by dividing each velocity value in a spectrum by the maximum value in that spectrum. This results in all spectra having a maximum value of 1, making them directly comparable.

4. What are the benefits of normalising a velocity spectrum?

Normalising a velocity spectrum allows for a more accurate and meaningful comparison between different spectra. It also helps to improve the overall clarity and readability of the data, making it easier to identify important patterns and trends.

5. Are there any limitations to normalising a velocity spectrum?

While normalising a velocity spectrum can be useful, it should not be the only method of analysis. It is important to also consider other factors such as the underlying physics and any potential biases in the data. Additionally, normalisation may not be appropriate for all types of velocity spectra, so it is important to carefully consider the data and its context before applying normalisation techniques.

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