Frequent assumption made (z R)

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In discussions about simplifying formulas involving different lengths, a common assumption is that smaller lengths can be ignored when they are significantly smaller than larger ones. For example, in the magnetic field equation, when the axial distance z is much greater than the radius R, the term involving R can be approximated away. This is typically justified through a Taylor expansion, where the small parameter R/z is treated as negligible. The distinction between "greater than" and "much greater than" is crucial, as it indicates that one term can be considered insignificant compared to the other. Overall, the process involves careful mathematical manipulation rather than mere deletion of terms.
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Frequently, when a length is bigger than another (say, an axial distance is bigger than the radius of something related) a certain assumption is made and the smaller length is "removed" from a formula. It's hard to describe, so let me show an example:

The magnetic field from a bobbin at an axial distance Z is:

B = \frac{\mu_0 i R^2}{2(R^2+z^2)^{3/2}}

But, according to my book, when z \gg R:

B = \frac{\mu_0 i R^2}{2z^3}

Even though this is just an example I've seen similar assumptions being made multiple times. How do I arrive at such conclusion? I hardly think that I must simply "delete" the smaller length (R^2) in the example, surely there must be a procedure to conclude that precisely?
 
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$$(R^2+z^2)^{\frac 3 2} = \left(z^2( \frac{R^2}{z^2}+1)\right)^{\frac 3 2}
\approx (z^2(0+1))^{\frac 3 2}=z^3$$
 
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Usually what is done, taking your example for clarity, is to write things in terms of the small quantity
<br /> \frac{R}{z}\ll 1.<br />
Then you do a Taylor expansion in terms of this small parameter (call it x). In this way you have a meaningful expansion that you can control. In your example:
<br /> B=\frac{\mu_0iR^2}{2z^3(1+x^2)^{3/2}}=\frac{\mu_0iR^2}{2z^3}+O(x).<br />
 
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By the way, z\gg R, and similarly, z/R\ll 1, do NOT just mean "z is greater than R" and "z/R is less than 1". They mean "z is much greater than R" and "z/R is much less than 1". "much greater" and "much less" is generally interpreted as "one can be ignored, compared to the other". That is if z\gg R, z+ R is "indistinguishable" from z, just as if you have $100,000,000, you can "ignore" $1!
 
kevinferreira said:
<br /> B=\frac{\mu_0iR^2}{2z^3(1+x^2)^{3/2}}=\frac{\mu_0iR^2}{2z^3}+O(x).<br />
Do you mean
<br /> =\frac{\mu_0iR^2}{2z^3}(1+O(x^2))<br />?
 
haruspex said:
Do you mean
<br /> =\frac{\mu_0iR^2}{2z^3}(1+O(x^2))<br />?

It doesn't really make a difference.
Yes, indeed, the first derivative vanishes at 0, but it doesn't make a difference because we're interested only in the zero order, so what I wrote holds anyway (an O(x^2) is an O(x) ).
Regarding the parenthesis, it makes no difference whatsoever, the notation O(x^a) is sufficiently ambiguous to allow many different notations where you let constants get in or not. I'm using the standard Taylor expansion notation, f(x)=f(0)+xf&#039;(0)+....
So, what I wrote definitely holds, as what you wrote.
 
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