Infinite Series Sum: Unlocking 1+3+5+.../(n!)

by Andrew McMorgan 46 views

Hey guys, ready to dive deep into the fascinating world of infinite series? Today, we're tackling a cool problem that involves a series where the numerator is the sum of consecutive odd numbers. We're looking to find the sum of

∑n=1∞1+3+5+⋯+(2n−1)n! \sum_{n=1}^{\infty} \frac{1+3+5+\cdots+(2n-1)}{n!}

Or, written out, it looks like this:

1+1+32!+1+3+53!+⋯ 1+\frac{1+3}{2!}+\frac{1+3+5}{3!}+\cdots

This type of problem is a classic in sequences and series, and it's super rewarding when you crack it. Let's break it down step by step. The key here is to first find a closed-form expression for the general term of the series. Your approach is spot on – by inspecting the pattern, we can see that the numerator, 1+3+5+⋯+(2n−1)1+3+5+\cdots+(2n-1), is the sum of the first nn odd numbers. Do you guys remember the formula for the sum of the first nn odd numbers? It's simply n2n^2! So, the general term, TrT_r, can indeed be written as r2r!\frac{r^2}{r!}. This is a crucial first step because it simplifies the series significantly. Now we have:

∑n=1∞n2n! \sum_{n=1}^{\infty} \frac{n^2}{n!}

This looks a lot more manageable, right? The n!n! in the denominator hints that we might need to use some properties of factorials and perhaps Taylor series expansions. The journey to finding the sum of an infinite series often involves manipulating the terms to fit known series, like the exponential function's Taylor series, ex=∑n=0∞xnn!e^x = \sum_{n=0}^{\infty} \frac{x^n}{n!}. Since we have n2n^2 in the numerator, we need to figure out how to break that down. One common trick when dealing with n2n^2 in series involving n!n! is to express n2n^2 in terms of falling factorials or to split the term strategically. Let's explore how we can manipulate n2n!\frac{n^2}{n!} to make it easier to sum. Remember, we're dealing with the sum starting from n=1n=1. This is important because if n=0n=0, the term 020!\frac{0^2}{0!} would be 01=0\frac{0}{1}=0, so including or excluding n=0n=0 doesn't change the sum if the numerator is n2n^2. However, it's good practice to always check the starting index.

Deconstructing the General Term: From n2n^2 to Simpler Forms

Alright, fam, now that we've established our general term is n2n!\frac{n^2}{n!}, the next big challenge is figuring out how to sum this beast up to infinity. The n2n^2 part can be a bit tricky. We want to manipulate it so that we can cancel out terms with the n!n! in the denominator, ideally leading us to something related to the exponential series. A common and super effective strategy here is to rewrite n2n^2 in a way that plays nicely with factorials. Think about how n!=n×(n−1)!n! = n \times (n-1)!. We can use this to our advantage. Let's try expressing n2n^2 using terms like nn and n(n−1)n(n-1). Why these? Because if we have nn in the numerator, we can cancel one nn from n!n! to get (n−1)!(n-1)! in the denominator. If we have n(n−1)n(n-1), we can cancel two factors from n!n! to get (n−2)!(n-2)! in the denominator. This process often simplifies the series into a sum of geometric series or related known series.

So, how can we write n2n^2 in terms of nn and n(n−1)n(n-1)? Let's play around: we know n2=n×nn^2 = n \times n. We can write n2=A⋅n+B⋅n(n−1)n^2 = A \cdot n + B \cdot n(n-1) for some constants AA and BB. Expanding the right side gives An+Bn2−BnAn + Bn^2 - Bn. Rearranging, we get Bn2+(A−B)nBn^2 + (A-B)n. For this to be equal to n2n^2, we need B=1B=1 (to match the n2n^2 coefficient) and A−B=0A-B=0 (to match the nn coefficient, which is zero). If B=1B=1, then A−1=0A-1=0, which means A=1A=1. So, we can write n2=1⋅n+1⋅n(n−1)n^2 = 1 \cdot n + 1 \cdot n(n-1). That's it! We've found our magical decomposition: n2=n+n(n−1)n^2 = n + n(n-1).

Now, let's substitute this back into our general term n2n!\frac{n^2}{n!}:

n2n!=n+n(n−1)n!=nn!+n(n−1)n! \frac{n^2}{n!} = \frac{n + n(n-1)}{n!} = \frac{n}{n!} + \frac{n(n-1)}{n!}

This looks promising! We can simplify each of these fractions:

For the first term, nn!\frac{n}{n!}: If n=1n=1, this is 11!=1\frac{1}{1!} = 1. If n>1n > 1, we can write n!=n×(n−1)!n! = n \times (n-1)!, so nn!=nn×(n−1)!=1(n−1)!\frac{n}{n!} = \frac{n}{n \times (n-1)!} = \frac{1}{(n-1)!}.

For the second term, n(n−1)n!\frac{n(n-1)}{n!}: If n=1n=1, the numerator is 1(0)=01(0)=0, so the term is 0. If n=2n=2, the numerator is 2(1)=22(1)=2, and n!=2!=2n!=2!=2, so the term is 22=1\frac{2}{2}=1. If n>1n > 1, we can write n!=n×(n−1)×(n−2)!n! = n \times (n-1) \times (n-2)!. So, n(n−1)n!=n(n−1)n×(n−1)×(n−2)!=1(n−2)!\frac{n(n-1)}{n!} = \frac{n(n-1)}{n \times (n-1) \times (n-2)!} = \frac{1}{(n-2)!} for n≥2n \ge 2.

So, our general term n2n!\frac{n^2}{n!} can be rewritten piece by piece. Let's re-examine the sum:

∑n=1∞n2n!=∑n=1∞(nn!+n(n−1)n!) \sum_{n=1}^{\infty} \frac{n^2}{n!} = \sum_{n=1}^{\infty} \left( \frac{n}{n!} + \frac{n(n-1)}{n!} \right)

We can split this into two separate sums:

∑n=1∞nn!+∑n=1∞n(n−1)n! \sum_{n=1}^{\infty} \frac{n}{n!} + \sum_{n=1}^{\infty} \frac{n(n-1)}{n!}

Let's evaluate each sum. Remember, our simplifications for nn!\frac{n}{n!} and n(n−1)n!\frac{n(n-1)}{n!} were valid for n>1n > 1 and n≥2n \ge 2 respectively. We need to be careful with the starting terms.

Consider the first sum: ∑n=1∞nn!\sum_{n=1}^{\infty} \frac{n}{n!}. For n=1n=1, the term is 11!=1\frac{1}{1!} = 1. For n>1n>1, the term is 1(n−1)!\frac{1}{(n-1)!}. So, the sum is 1+∑n=2∞1(n−1)!1 + \sum_{n=2}^{\infty} \frac{1}{(n-1)!}. Let k=n−1k = n-1. When n=2n=2, k=1k=1. When n=∞n=\infty, k=∞k=\infty. So the sum becomes 1+∑k=1∞1k!1 + \sum_{k=1}^{\infty} \frac{1}{k!}. We know the Taylor series for exe^x is ex=∑n=0∞xnn!=1+x+x22!+x33!+⋯e^x = \sum_{n=0}^{\infty} \frac{x^n}{n!} = 1 + x + \frac{x^2}{2!} + \frac{x^3}{3!} + \cdots. For x=1x=1, we have e=∑n=0∞1n!=1+1+12!+13!+⋯e = \sum_{n=0}^{\infty} \frac{1}{n!} = 1 + 1 + \frac{1}{2!} + \frac{1}{3!} + \cdots. So, ∑k=1∞1k!=e−1\sum_{k=1}^{\infty} \frac{1}{k!} = e - 1. Therefore, the first sum is 1+(e−1)=e1 + (e-1) = e. Pretty neat!

Now, consider the second sum: ∑n=1∞n(n−1)n!\sum_{n=1}^{\infty} \frac{n(n-1)}{n!}. For n=1n=1, the term is 1(0)1!=0\frac{1(0)}{1!} = 0. For n=2n=2, the term is 2(1)2!=22=1\frac{2(1)}{2!} = \frac{2}{2} = 1. For n≥2n \ge 2, the term simplifies to 1(n−2)!\frac{1}{(n-2)!}. So, the sum is 0+∑n=2∞1(n−2)!0 + \sum_{n=2}^{\infty} \frac{1}{(n-2)!}. Let m=n−2m = n-2. When n=2n=2, m=0m=0. When n=∞n=\infty, m=∞m=\infty. So the sum becomes ∑m=0∞1m!\sum_{m=0}^{\infty} \frac{1}{m!}. This is exactly the series for e1e^1, which is ee!

So, putting it all together:

∑n=1∞n2n!=(∑n=1∞nn!)+(∑n=1∞n(n−1)n!)=e+e=2e \sum_{n=1}^{\infty} \frac{n^2}{n!} = \left( \sum_{n=1}^{\infty} \frac{n}{n!} \right) + \left( \sum_{n=1}^{\infty} \frac{n(n-1)}{n!} \right) = e + e = 2e

But wait, let's double check the splitting and indices. The decomposition n2=n+n(n−1)n^2 = n + n(n-1) is valid for all nn. So n2n!=nn!+n(n−1)n!\frac{n^2}{n!} = \frac{n}{n!} + \frac{n(n-1)}{n!}. Let's evaluate the sums directly using the simplified forms, being mindful of the terms where the simplification is not directly applicable or when nn or n−1n-1 are zero.

Sum 1: ∑n=1∞nn!\sum_{n=1}^{\infty} \frac{n}{n!} We can write nn!=1(n−1)!\frac{n}{n!} = \frac{1}{(n-1)!} for nless0n less 0. Since nless1n less 1, for n=1n=1, 1(1−1)!=10!=1\frac{1}{(1-1)!} = \frac{1}{0!} = 1. For n>1n>1, it's also 1(n−1)!\frac{1}{(n-1)!}. So, ∑n=1∞nn!=∑n=1∞1(n−1)!\sum_{n=1}^{\infty} \frac{n}{n!} = \sum_{n=1}^{\infty} \frac{1}{(n-1)!}. Let k=n−1k=n-1. This becomes ∑k=0∞1k!=e\sum_{k=0}^{\infty} \frac{1}{k!} = e. This part is correct.

Sum 2: ∑n=1∞n(n−1)n!\sum_{n=1}^{\infty} \frac{n(n-1)}{n!} For n=1n=1, the term 1(0)1!=0\frac{1(0)}{1!} = 0. For n=2n=2, the term 2(1)2!=1\frac{2(1)}{2!} = 1. For n≥2n \ge 2, n(n−1)n!=n(n−1)n(n−1)(n−2)!=1(n−2)!\frac{n(n-1)}{n!} = \frac{n(n-1)}{n(n-1)(n-2)!} = \frac{1}{(n-2)!}. So, ∑n=1∞n(n−1)n!=0+∑n=2∞1(n−2)!\sum_{n=1}^{\infty} \frac{n(n-1)}{n!} = 0 + \sum_{n=2}^{\infty} \frac{1}{(n-2)!}. Let m=n−2m=n-2. This becomes ∑m=0∞1m!=e\sum_{m=0}^{\infty} \frac{1}{m!} = e. This part is also correct.

Thus, the total sum is e+e=2ee + e = 2e. This seems correct.

Alternative Approach: Using the Properties of exe^x

Let's try another way to confirm our result, guys. Sometimes, breaking down the numerator isn't the only path. We can also think about how to manipulate the series ∑n=1∞n2n!\sum_{n=1}^{\infty} \frac{n^2}{n!} to directly relate it to the exponential function. Recall ex=∑n=0∞xnn!e^x = \sum_{n=0}^{\infty} \frac{x^n}{n!}.

We are interested in ∑n=1∞n2n!\sum_{n=1}^{\infty} \frac{n^2}{n!}. Notice that for n=0n=0, the term 020!=0\frac{0^2}{0!} = 0, so ∑n=1∞n2n!=∑n=0∞n2n!\sum_{n=1}^{\infty} \frac{n^2}{n!} = \sum_{n=0}^{\infty} \frac{n^2}{n!}.

Consider the function f(x)=ex=∑n=0∞xnn!f(x) = e^x = \sum_{n=0}^{\infty} \frac{x^n}{n!}. If we differentiate f(x)f(x) with respect to xx, we get: f′(x)=ex=∑n=1∞nxn−1n!f'(x) = e^x = \sum_{n=1}^{\infty} \frac{nx^{n-1}}{n!}. Multiply by xx: xex=∑n=1∞nxnn!xe^x = \sum_{n=1}^{\infty} \frac{nx^n}{n!}. Now, differentiate again with respect to xx: (xex)′=ex+xex=∑n=1∞n2xn−1n!(xe^x)' = e^x + xe^x = \sum_{n=1}^{\infty} \frac{n^2x^{n-1}}{n!}. Multiply by xx again: x(ex+xex)=xex+x2ex=∑n=1∞n2xnn!x(e^x + xe^x) = x e^x + x^2 e^x = \sum_{n=1}^{\infty} \frac{n^2x^n}{n!}.

This is amazing! The right-hand side is exactly the form of our series, but with xnx^n instead of just 1. To find our sum, we just need to evaluate this expression at x=1x=1.

Setting x=1x=1 in the equation xex+x2ex=∑n=1∞n2xnn!x e^x + x^2 e^x = \sum_{n=1}^{\infty} \frac{n^2x^n}{n!}, we get:

1⋅e1+12⋅e1=∑n=1∞n2(1)nn!1 \cdot e^1 + 1^2 \cdot e^1 = \sum_{n=1}^{\infty} \frac{n^2(1)^n}{n!}

e+e=∑n=1∞n2n!e + e = \sum_{n=1}^{\infty} \frac{n^2}{n!}

2e=∑n=1∞n2n!2e = \sum_{n=1}^{\infty} \frac{n^2}{n!}

So, the sum of the series is indeed 2e2e. This method using differentiation of the power series is super powerful and confirms our previous result. It's a bit more abstract but very elegant.

Final Thoughts and Conclusion

So there you have it, folks! We've successfully found the sum of the infinite series ∑n=1∞1+3+5+⋯+(2n−1)n!\sum_{n=1}^{\infty} \frac{1+3+5+\cdots+(2n-1)}{n!}. By first identifying the general term as n2n!\frac{n^2}{n!}, we explored two robust methods to find its sum. The first involved algebraic manipulation of the numerator n2n^2 into n+n(n−1)n + n(n-1), which allowed us to split the series into parts that neatly summed to ee each, resulting in a total sum of 2e2e. The second method utilized the power of differentiation on the Taylor series of exe^x, providing an elegant and direct route to the same answer, 2e2e.

This problem is a fantastic example of how understanding the properties of factorials and the Taylor series for exe^x can unlock solutions to seemingly complex series. Remember these techniques, guys! Breaking down numerators or using differentiation are go-to strategies when you see factorials in the denominator, especially with polynomial terms like n2n^2. Keep practicing, and you'll find these problems become second nature. The world of sequences and series is full of these hidden gems, and each one you solve builds your mathematical toolkit. Keep exploring, keep calculating, and most importantly, have fun with it!

Stay tuned for more cool math challenges here on Plastik Magazine!