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Exponential series – "Math for Non-Geeks"

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The exponential series has the form e=∑k=0∞1k!. We will see that he limit e indeed exists and is given by Euler's number, which we encountered first within the article Monotonicity criterion. There, it was defined as the limit of the sequences ((1+1n)n)n∈ℕ and ((1+1n)n+1)n∈ℕ. In this article, we will show the limit equivalence limn→∞(1+1n)n=limn→∞(1+1n)n+1=e=∑k=0∞1k! which is far from obvious. Later, we will investigate a generalized form of the exponential series ∑k=0∞xkk!.

Convergence of the exponential series

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At first, we need to show that the exponential series converges at all:

Theorem (convergence of the exponential series)

The series ∑k=0∞1k! converges.

Proof (convergence of the exponential series)

We need to prove that the partial sums (sn)n∈ℕ=(∑k=0n1k!)n∈ℕ converges. This can be done using the monotonicity criterion for sequences, where the partial sums (sn) form the sequence which we want to investigate.

Monotonicity is easy to see. Series elements are positive, so

sn+1=∑k=0n+11k!=∑k=0n1k!+1(n+1)!⏟≥0≥∑k=0n1k!=sn

Hence, (sn) is monotonically increasing.

Boundedness from above can be shown by comparison to a geometric series with q=12<1. For partial sums, we have

∑k=0n1k!=∑k=0n11⋅2⋅3⋅…⋅(k−1)⋅k=∑k=0n12⋅3⋅…⋅(k−1)⋅k↓ 12,13,…1k−1,1k≤12≤∑k=0n12⋅2⋅…⋅2⋅2⏟(k−1) times=∑k=0n(12)k−1=2⋅∑k=0n(12)k≤2⋅∑k=0∞(12)k↓ geometric series with q=12=2⋅11−12=2⋅2=4

Hence, (sn) is bounded from above by 4 . So the monotonicity criterion implies convergence.

Limit of the exponential series

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Now, we show that the exponential series indeed converges towards Euler's number e. This is done using the squeeze theorem by "squeezing" the partial sums (sn)n∈ℕ=(∑k=0n1k!)n∈ℕ between the sequences ((1+1n)n)n∈ℕ and ((1+1n)n+1)n∈ℕ . Both bounding sequences converge to e , so we get the desired result.

That means, we need to show: (1+1n)n≤∑k=0n1k!≤(1+1n)n+1

Theorem (limit of the exponential series)

There is ∑k=0∞1k!=e.

Proof (limit of the exponential series)

We show (1+1n)n≤∑k=0n1k!≤(1+1n)n+1 and use the squeeze theorem:

1st inequality: (1+1n)n≤∑k=0n1k!. This is easier to establish than the second one. We need the binomial theorem (1+x)n=∑k=0n(nk)xk with x=1n.

(1+1n)n=binomialtheorem∑k=0n(nk)1nk=∑k=0nn⋅(n−1)⋅(n−2)⋅…⋅(n−k+1)k!⋅1nk=∑k=0nn⋅(n−1)⋅(n−2)⋅…⋅(n−k+1)n⋅n⋅n⋅…⋅n⋅1k!=∑k=0nnn⋅n−1n⋅n−2n⋅…⋅n−k+1n⏟≤1⋅1k!≤∑k=0n1k!

2nd inequality: (1+1n)n+1≥∑k=0n1k!. Her, we additionally need the Bernoulli inequality (1+x)n≥1+nx for x≥−1. In addition, a telescoping sum will appear in the end of the proof.

(1+1n)n+1=binomialtheorem∑k=0n+1(n+1k)1nk=1+∑k=1n+1(n+1k)1nk↓ index shift=1+∑k=0n(n+1k+1)1nk+1=1+∑k=0n(n+1)⋅n⋅(n−1)⋅…⋅(n−k+1)(k+1)!⋅1nk+1=1+∑k=0n(n+1)⋅n⋅(n−1)⋅…⋅(n−(k−1))n⋅n⋅n⋅…⋅n⋅1(k+1)!↓ n+1,n,n−1,…n−(k−1)≥n−(k−1)≥1+∑k=0n(n−(k−1))k+1nk+1⋅1(k+1)!=1+∑k=0n(1−k−1n)k+1⋅1(k+1)!↓ Bernoulli's inequality with x=−k−1n≥−1≥1+∑k=0n(1−(k+1)(k−1)n)⋅1(k+1)!↓ Linearity of the sum=1+∑k=0n1(k+1)!−1n∑k=0n(k+1)(k−1)(k+1)!↓ Index shift (1st sum), cancellation (2nd sum)=1+∑k=1n+11k!−1n∑k=0n(k−1)k!↓ 1=11! and factor out the n+1-th summand of the sum for k=0 and k=1 for the 2nd sum.=∑k=0n1k!+1(n+1)!⏟≥0−1n[−1+0+∑k=2n(k−1)k!]↓ re-formulate the fraction within the 2nd sum and use kk!=1(k−1)!≥∑k=0n1k!−1n[−1+∑k=2n(1(k−1)!−1k!)]↓ telescoping sum∑k=2n(1(k−1)!−1k!)=1−1n!=∑k=0n1k!−1n[−1+1−1n!]=∑k=0n1k!+1n⋅n!⏟≥0≥∑k=0n1k!

In addition, we established (1+1n)n≤∑k=0n1k!≤(1+1n)n+1 . Since limn→∞(1+1n)n=limn→∞(1+1n)n+1=e, the squeeze theorem implies limn→∞∑k=0n1k!=∑k=0∞1k!=e.

Remarks

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  • Alternatively, one may show lim infn→∞∑k=0n1k!≤e≤lim supn→∞∑k=0n1k! , which also implies ∑k=0∞1k!=e.
  • Further, the sequences an=∑k=0n1k! and bn=∑k=0n1k!+1n⋅n! define nested intervals (In)n∈ℕ=([an,bn])n∈ℕ, where the real number included in all intervals is exactly e.
  • The advantage if the exponential series compared to the sequences defining e is that one can achieve much faster convergence. For instance, with 10 elements ∑k=0101k!≈2.7182818011 which is an approximation precise up to 7 digits: e=2.718281828. By contrast, the 1000-th sequence element (1+11000)1000=2.7169239 is precise to only 2 digits after the comma.

Outlook: generalized exponential series

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As remarked in the introduction, there is a generalization to the exponential series, which reads ∑k=0∞xkk! . This series can be shown to converge for all x∈ℝ . Therefore, it serves for a real-valued exponential function exp⁡:ℝ→ℝ . Even complex arguments are possible! However, exp⁡(x) is a priori not the same as a power ex. So the computation rules for powers, like exp⁡(x+y)=exp⁡(x)exp⁡(y), must be shown explicitly.

The series considered within this article is a special case with x=1:

exp⁡(1)=∑k=0∞1kk!=∑k=0∞1k!=e