Taylor Series Expansion for the Relativistic Factor of Momentum

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SUMMARY

The discussion focuses on deriving the Taylor series expansion for the relativistic factor γ, specifically for small velocities (v) around v = 0, using the equation γ = 1/SQRT(1 - V²/C²). Participants clarify that substituting X = V/C transforms the equation to γ = 1/SQRT(1 - X²). The correct expansion involves calculating derivatives at X = 0, leading to the Maclaurin series representation. Key corrections include ensuring accurate derivative calculations to avoid sign errors in the series expansion.

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  • Understanding of Taylor series and Maclaurin series
  • Familiarity with the concept of relativistic momentum
  • Knowledge of calculus, specifically differentiation
  • Basic understanding of the Lorentz factor γ in special relativity
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leejqs
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Homework Statement


Using the technique of Taylor expansion, find an approximate expression for the relativistic factor γ for small v (i.e., expanded around v = 0) that is correct to order v2.


Homework Equations


γ=1/SQRT(1+ V2/C2). But in class, my professor just substituted X=V/C, so the equation became γ=1/SQRT(1-X2).


The Attempt at a Solution


I tried to expand the function γ(v) with v at 0...
γ(v)=1+γ'(0)(X-0)+(1/2)γ''(0)(X-0)2
However, this expression wasn't correct. I'm not really sure how else to expand it! Any help would be much, much appreciated, thanks!
 
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leejqs said:

Homework Statement


Using the technique of Taylor expansion, find an approximate expression for the relativistic factor γ for small v (i.e., expanded around v = 0) that is correct to order v2.


Homework Equations


γ=1/SQRT(1+ V2/C2). But in class, my professor just substituted X=V/C, so the equation became γ=1/SQRT(1-X2).
With that substitution, you get y = 1/sqrt(1 + x2).
leejqs said:

The Attempt at a Solution


I tried to expand the function γ(v) with v at 0...
γ(v)=1+γ'(0)(X-0)+(1/2)γ''(0)(X-0)2
This is really y(x) with x at 0. If v = 0, then x = 0. It's very likely that the sign error above is affecting what you got for your Maclaurin series.
leejqs said:
However, this expression wasn't correct. I'm not really sure how else to expand it! Any help would be much, much appreciated, thanks!
 
Sorry for that typo! The actual function is y=1/SQRT(1-V2/C2).

In finding the parts of this maclaurin series, I have...
y(0)=1/SQRT(1-X2)(X-0)0=1
y'(0)=(1/2)(1-X2)(-3/2)*X2
y''(0)=(1/2)(1-X2)(-3/2)*X2+(1-X2)(-3/2)*(1-X2)(-5/2)*3X4

Sorry for my lack of showing my work, but I believe those expressions are right
when using the yn(v)=[f(n)(X0(X-X0)n]/n!
 
how to Put the Boolean function q'r + p'q' + pq'r' into DNF and find a simpler representation for the function using a Karnaugh map. Show the output of this simpler function is the same as in question 1 for p = 1, q = 1, r = 0.
 
leejqs said:
Sorry for that typo! The actual function is y=1/SQRT(1-V2/C2).

In finding the parts of this maclaurin series, I have...
y(0)=1/SQRT(1-X2)(X-0)0=1
y'(0)=(1/2)(1-X2)(-3/2)*X2
y''(0)=(1/2)(1-X2)(-3/2)*X2+(1-X2)(-3/2)*(1-X2)(-5/2)*3X4

Sorry for my lack of showing my work, but I believe those expressions are right
when using the yn(v)=[f(n)(X0(X-X0)n]/n!
Your derivatives are wrong because you're mixing in stuff from the series expansion. You should have:

y(X)=1/\sqrt{1-X^2} \rightarrow y(0)=1
y'(X)=X/(1-X^2)^{-3/2} \rightarrow y'(0)=0

and so on. You then plug these values for y(0), y'(0), y''(0) into the series expansion.
 

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