Applications of the Binomial Theorem

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The binomial series can be derived using Taylor's expansion theorem, specifically for the function f(ε) = (1 + ε)^v, resulting in the series (1 + ε)^v = Σ(κ=0 to ∞) binom(v, k) ε^k. When v is a positive integer n, the series terminates because binom(n, k) is zero for k > n, leading to a finite sum. The binomial theorem is indeed a special case of the binomial series when v is a positive integer. Additionally, the binomial series has applications in special relativity, particularly in approximating expressions involving the Lorentz factor γ by expanding around small values of ε.
courtrigrad
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How would you quickly derive the binomial series? Would you have to use Taylor's Theorem/ Taylor Series? And does the Binomial Theorem follow from the binomial series? Are there any applications at all of the binomial series/ Binomial Theorem to special relativity? I know the binomial series is (x+a)^{v} = \sum_{k=0}^{\infty}\binom{v}{k} x^{k}a^{v-k}. v is a real number. But I guess when v is a positive integer n we get (x+a)^{n} = \sum_{k=0}^{\infty}\binom{n}{k} x^{k}a^{n-k}. Why does the series terminate at n = v?

Thanks
 
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That's a lot of question! Take your breath! :-p

courtrigrad said:
How would you quickly derive the binomial series?
It is not quick and painless but it is simply a result of applying Taylor's expansion theorem to the function of one variable f(\epsilon)=(1+\epsilon)^v. The resulting series is

(1+\epsilon)^{v} = \sum_{k=0}^{\infty}\binom{v}{k} \epsilon^{k}

and its radius of convergence is found to be 1. One can then decide to set \epsilon = x/a and multiply both sides of the equation by a^v to get

(x+a)^{v} = \sum_{k=0}^{\infty}\binom{v}{k} x^{k}a^{v-k}

of radius of convergence 'a'.
courtrigrad said:
And does the Binomial Theorem follow from the binomial series?
Yes; in the particular case v=n, a positive integer, the series is finite (the series "terminate" at k=n) and equals the binomial sum. More on that later.

courtrigrad said:
Are there any applications at all of the binomial series/ Binomial Theorem to special relativity?
The binomial series is useful for approximations. When we have an expression of the form (1+\epsilon)^{v} where |\epsilon |<1, we can write it as its Taylor series (which is in this case, the binomial series) and make the approximation that (1+\epsilon)^{v} is equal to only the first few terms of the series. You should be able to see why this is reasonable in the scope of 0<|\epsilon|<1.

In special relativity, the factor \gamma is of the above form, with \epsilon =-(v/c)^2 and v=-½, so a series expansion is possible and we can make the approximation of keeping only the first few terms in in order to ease our calculations or get insights into the equations.

courtrigrad said:
I know the binomial series is (x+a)^{v} = \sum_{k=0}^{\infty}\binom{v}{k} x^{k}a^{v-k}. v is a real number. But I guess when v is a positive integer n we get (x+a)^{n} = \sum_{k=0}^{\infty}\binom{n}{k} x^{k}a^{n-k}. Why does the series terminate at n = v?

Watch what happens to \binom{n}{k} for k>n*. It vanishes. So all terms of the binomial series past k=n are zero.

*The definition of \binom{n}{k} used is this: http://en.wikipedia.org/wiki/Binomial_series
 
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Question: A clock's minute hand has length 4 and its hour hand has length 3. What is the distance between the tips at the moment when it is increasing most rapidly?(Putnam Exam Question) Answer: Making assumption that both the hands moves at constant angular velocities, the answer is ## \sqrt{7} .## But don't you think this assumption is somewhat doubtful and wrong?

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