Boundedness Of The Series ∑[n=0 To ∞] Sin(x/2^n) An Exploration

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Hey guys! Ever stumbled upon a series that just makes you scratch your head and wonder about its behavior? Today, we're diving deep into one such fascinating series: n=0sinx2n\sum_{n=0}^{\infty} \sin\frac{x}{2^n}. This isn't just any series; it's a gateway to exploring the beautiful world of analysis and functions. We'll break it down, make it digestible, and by the end, you'll feel like a series-bounding boss!

Defining the Function and Absolute Convergence

So, let's kick things off by defining our function. We're calling it f(x)f(x), and it's the sum of our series:

f(x)=n=0sinx2nf(x) = \sum_{n=0}^{\infty} \sin\frac{x}{2^n}

The first thing we need to tackle is whether this series even makes sense. Does it converge? And if so, does it converge nicely? It turns out, it does! We can actually prove that for every real number xx, this infinite series converges absolutely. That's a fancy way of saying that if we take the absolute value of each term and sum those up, the series still converges. This is super important because absolute convergence implies regular convergence, meaning our series is well-behaved and we can work with it.

To truly grasp the absolute convergence of the series n=0sinx2n\sum_{n=0}^{\infty} \sin\frac{x}{2^n}, we need to delve into the nitty-gritty details. Remember, absolute convergence means that n=0sinx2n\sum_{n=0}^{\infty} |\sin\frac{x}{2^n}| converges. To demonstrate this, we often employ the comparison test, a powerful tool in our analytical arsenal. The comparison test essentially states that if we can find another series that we know converges and is always greater than or equal to our series in absolute value, then our series also converges absolutely. So, what series can we compare with? A brilliant choice here is to leverage the small-angle approximation of the sine function. For small values of θ\theta, sin(θ)\sin(\theta) is approximately equal to θ\theta. More formally, we know that sin(θ)θ|\sin(\theta)| \leq |\theta| for all real numbers θ\theta. Applying this to our series, we get:

sinx2nx2n|\sin\frac{x}{2^n}| \leq |\frac{x}{2^n}|

Now, we have a new series to contend with: n=0x2n=xn=012n\sum_{n=0}^{\infty} |\frac{x}{2^n}| = |x| \sum_{n=0}^{\infty} \frac{1}{2^n}. The series n=012n\sum_{n=0}^{\infty} \frac{1}{2^n} is a classic example of a geometric series. Geometric series have the general form n=0arn\sum_{n=0}^{\infty} ar^n, where aa is the first term and rr is the common ratio. A crucial property of geometric series is that they converge if and only if the absolute value of the common ratio, r|r|, is less than 1. In our case, r=12r = \frac{1}{2}, and since 12<1|\frac{1}{2}| < 1, the geometric series converges. Specifically, it converges to 11r=1112=2\frac{1}{1 - r} = \frac{1}{1 - \frac{1}{2}} = 2. Therefore, n=0x2n=xn=012n=2x\sum_{n=0}^{\infty} |\frac{x}{2^n}| = |x| \sum_{n=0}^{\infty} \frac{1}{2^n} = 2|x|, which is a finite value for any real number xx. By the comparison test, since n=0x2n\sum_{n=0}^{\infty} |\frac{x}{2^n}| converges, we can confidently conclude that n=0sinx2n\sum_{n=0}^{\infty} |\sin\frac{x}{2^n}| also converges. This establishes the absolute convergence of our series, laying a solid foundation for further analysis.

The Million-Dollar Question: Is the Function Bounded?

Now, here's where things get interesting. We know our function f(x)f(x) exists for all real numbers, but is it bounded? In simpler terms, can we find some upper and lower limits that f(x)f(x) will never exceed? This is a crucial question because boundedness tells us a lot about the function's overall behavior. A bounded function won't go shooting off to infinity or negative infinity; it'll stay within a certain range. Think of it like a cozy little function that knows its limits.

The quest for boundedness often leads us down fascinating mathematical paths. We might try to find clever inequalities, use trigonometric identities, or even resort to some calculus magic. The beauty of this problem lies in the fact that there isn't one single way to crack it. It's a puzzle, and we get to use our mathematical toolbox to solve it. So, let's put on our thinking caps and explore some strategies!

To determine whether the function f(x)=n=0sinx2nf(x) = \sum_{n=0}^{\infty} \sin\frac{x}{2^n} is bounded, we need to explore some strategies that go beyond the simple convergence proof. While absolute convergence tells us the series doesn't blow up, it doesn't directly tell us if the function itself is confined within specific bounds. One powerful approach involves using trigonometric identities to manipulate the series into a more manageable form. Let's consider the identity:

2sin(a)cos(a)=sin(2a)2\sin(a)\cos(a) = \sin(2a)

This identity suggests a telescoping product approach. If we can somehow introduce a cosine term into our series, we might be able to use this identity to simplify the sum. A clever trick is to multiply and divide the series by cos(x21)\cos(\frac{x}{2^1}), then by cos(x22)\cos(\frac{x}{2^2}), and so on. However, we need to be cautious about cases where these cosine terms might be zero. For now, let's assume xx is not of the form kπk\pi where kk is an integer power of 2, so that we avoid these zeroes.

Let's multiply f(x)f(x) by cos(x21)cos(x21)\frac{\cos(\frac{x}{2^1})}{\cos(\frac{x}{2^1})}, which is equal to 1 as long as cos(x21)0\cos(\frac{x}{2^1}) \neq 0:

f(x)=1cos(x2)n=0sin(x2n)cos(x2)f(x) = \frac{1}{\cos(\frac{x}{2})} \sum_{n=0}^{\infty} \sin(\frac{x}{2^n}) \cos(\frac{x}{2})

Now, consider the first term of the sum, where n=0n = 0: sin(x)cos(x2)\sin(x)\cos(\frac{x}{2}). Using the product-to-sum identity, we can rewrite this. However, a more strategic approach is to use the double-angle identity in reverse. We'll multiply and divide by 22 and use 2sin(x2n)cos(x2n)=sin(x2n1)2\sin(\frac{x}{2^n})\cos(\frac{x}{2^n}) = \sin(\frac{x}{2^{n-1}}):

f(x)=n=0sin(x2n)=1sin(x2N)n=0Nsin(x2n)k=1N2cos(x2k)f(x) = \sum_{n=0}^{\infty} \sin(\frac{x}{2^n}) = \frac{1}{\sin(\frac{x}{2^N})} \sum_{n=0}^N \sin(\frac{x}{2^n}) \prod_{k=1}^N 2\cos(\frac{x}{2^k})

This manipulation is aimed at creating a telescoping product. By repeatedly applying the double-angle formula, we hope to collapse the sum into a more manageable expression. This is a common technique when dealing with trigonometric series, and it often leads to elegant solutions. Keep in mind, the key here is to recognize the pattern and strategically apply the trigonometric identities to simplify the expression. This process may seem a bit daunting at first, but with practice, it becomes a powerful tool in your mathematical arsenal. The goal is to rewrite the infinite sum into a form where we can easily identify its bounds, ultimately answering our question about the boundedness of f(x)f(x).

Unveiling the Boundedness: A Telescoping Product Approach

Let’s dive deeper into this telescoping product strategy. We've hinted at multiplying and dividing by cosine terms, and now it's time to see how that unfolds. The core idea is to create a chain reaction where terms cancel each other out, leaving us with a simpler expression. Remember, the double-angle identity 2sin(a)cos(a)=sin(2a)2\sin(a)\cos(a) = \sin(2a) is our guiding star here.

Let's start by multiplying f(x)f(x) by cos(x2)cos(x2)\frac{\cos(\frac{x}{2})}{\cos(\frac{x}{2})}, assuming cos(x2)0\cos(\frac{x}{2}) \neq 0:

f(x)=1cos(x2)n=0sin(x2n)cos(x2)f(x) = \frac{1}{\cos(\frac{x}{2})} \sum_{n=0}^{\infty} \sin(\frac{x}{2^n}) \cos(\frac{x}{2})

Now, focus on the term where n=0n=0: sin(x)cos(x2)\sin(x)\cos(\frac{x}{2}). This doesn't directly fit our double-angle identity, so we need to be a bit more strategic. Instead of just multiplying by one cosine term, let's consider multiplying by a series of them:

cos(x2)cos(x4)cos(x8)...cos(x2)cos(x4)cos(x8)...\frac{\cos(\frac{x}{2})\cos(\frac{x}{4})\cos(\frac{x}{8})...}{\cos(\frac{x}{2})\cos(\frac{x}{4})\cos(\frac{x}{8})...}

This might seem like overkill, but it's a clever way to set up the telescoping product. Let's look at the partial product of cosines in the denominator:

PN=k=1Ncos(x2k)=cos(x2)cos(x4)...cos(x2N)P_N = \prod_{k=1}^{N} \cos(\frac{x}{2^k}) = \cos(\frac{x}{2})\cos(\frac{x}{4})...\cos(\frac{x}{2^N})

Now, we multiply and divide PNP_N by sin(x2N)\sin(\frac{x}{2^N}):

PN=sin(x2N)sin(x2N)k=1Ncos(x2k)=sin(x2N)cos(x2)cos(x4)...cos(x2N)sin(x2N)P_N = \frac{\sin(\frac{x}{2^N})}{\sin(\frac{x}{2^N})} \prod_{k=1}^{N} \cos(\frac{x}{2^k}) = \frac{\sin(\frac{x}{2^N}) \cos(\frac{x}{2})\cos(\frac{x}{4})...\cos(\frac{x}{2^N})}{\sin(\frac{x}{2^N})}

Applying the double-angle identity repeatedly, we get:

sin(x2N)cos(x2N)=12sin(x2N1)\sin(\frac{x}{2^N})\cos(\frac{x}{2^N}) = \frac{1}{2}\sin(\frac{x}{2^{N-1}})

12sin(x2N1)cos(x2N1)=122sin(x2N2)\frac{1}{2}\sin(\frac{x}{2^{N-1}})\cos(\frac{x}{2^{N-1}}) = \frac{1}{2^2}\sin(\frac{x}{2^{N-2}}) and so on.

Continuing this process, we eventually arrive at:

PN=12Nsin(x)sin(x2N)P_N = \frac{1}{2^N} \frac{\sin(x)}{\sin(\frac{x}{2^N})}

This is a fantastic result! We've transformed the product of cosines into a simple expression involving sines. Now, let's bring this back to our original series. We can rewrite f(x)f(x) as:

f(x)=n=0sin(x2n)=limN1PNn=0sin(x2n)sin(x)2Nsin(x2N)f(x) = \sum_{n=0}^{\infty} \sin(\frac{x}{2^n}) = \lim_{N \to \infty} \frac{1}{P_N} \sum_{n=0}^{\infty} \sin(\frac{x}{2^n}) \frac{\sin(x)}{2^N \sin(\frac{x}{2^N})}

Substituting our expression for PNP_N, we get:

$f(x) = \lim_{N \to \infty} \frac{\sin(\frac{x}{2^N})}{\sin(x)} \sum_{n=0}^{\infty} \sin(\frac{x}{2^n}) $

As NN approaches infinity, x2N\frac{x}{2^N} approaches 0, and we can use the approximation sin(θ)θ\sin(\theta) \approx \theta for small θ\theta. Thus, sin(x2N)x2N\sin(\frac{x}{2^N}) \approx \frac{x}{2^N}. Plugging this in, we get:

limNsin(x2N)x2N=1\lim_{N \to \infty} \frac{\sin(\frac{x}{2^N})}{\frac{x}{2^N}} = 1

Therefore, our expression simplifies to:

$f(x) = \frac{\sin(x)}{\sin(x)} \lim_{N \to \infty} x \frac{\sin(\frac{x}{2N})}{\frac{x}{2N}} $

Now, this gives 2x2x almost everywhere, specifically when xx is not a multiple of π\pi. When xx is a multiple of π\pi, we require a different argument.

This is a significant breakthrough! We've managed to rewrite our infinite series in a closed form. This closed form will be instrumental in determining the boundedness of f(x)f(x). Remember, the goal is to find upper and lower limits for f(x)f(x), and this new expression brings us much closer to that goal. The next step is to carefully analyze this closed form and extract the information we need about the boundedness of our function.

The Grand Finale: Boundedness Revealed!

Alright, guys, we've reached the final stretch! We've transformed our series into a closed form, and now it's time to unveil the boundedness of f(x)f(x). Remember, our closed form expression is:

f(x)=2xsin(x)xf(x) = 2x \frac{\sin(x)}{x}

This expression holds true for all xx not equal to 2kπ2k\pi, where kk is an integer (to avoid division by zero in the original telescoping product argument). For the sake of discussion, let's focus on these values of xx first. The function sin(x)x\frac{\sin(x)}{x} is a well-known function called the sinc function, often denoted as sinc(x)(x). It has a value of 1 at x=0x = 0 and oscillates with decreasing amplitude as x|x| increases. A crucial property of the sinc function is that it is bounded between -1 and 1. That is, 1sin(x)x1-1 \leq \frac{\sin(x)}{x} \leq 1 for all xx.

Using this property, we can write:

2x2xsin(x)x2x-|2x| \leq 2x\frac{\sin(x)}{x} \leq |2x|

This inequality tells us that f(x)f(x) is bounded by 2x|2x|. However, this bound depends on xx, which means it's not a uniform bound. A uniform bound would be a constant value that f(x)f(x) never exceeds, regardless of the value of xx. To find a uniform bound, we need to delve a little deeper.

Let's revisit our original series: f(x)=n=0sin(x2n)f(x) = \sum_{n=0}^{\infty} \sin(\frac{x}{2^n}). We know that sin(θ)θ|\sin(\theta)| \leq |\theta| for all θ\theta. Applying this inequality to each term in the series, we get:

sin(x2n)x2n|\sin(\frac{x}{2^n})| \leq |\frac{x}{2^n}|

Summing both sides over all nn, we have:

f(x)=n=0sin(x2n)n=0sin(x2n)n=0x2n=xn=012n|f(x)| = |\sum_{n=0}^{\infty} \sin(\frac{x}{2^n})| \leq \sum_{n=0}^{\infty} |\sin(\frac{x}{2^n})| \leq \sum_{n=0}^{\infty} |\frac{x}{2^n}| = |x|\sum_{n=0}^{\infty} \frac{1}{2^n}

The series n=012n\sum_{n=0}^{\infty} \frac{1}{2^n} is a geometric series that converges to 2. Therefore, we have:

f(x)2x|f(x)| \leq 2|x|

Again, this gives us a bound that depends on xx. However, it's a crucial stepping stone. To get a constant bound, we need to employ a different trick. Let's go back to the telescoping product result. We had:

f(x)=limNxsin(x2N)x2Nf(x) = \lim_{N \to \infty} x \frac{\sin(\frac{x}{2^N})}{\frac{x}{2^N}}

Using L'Hôpital's Rule in the limit, we get 2x2x

However this limit approach has problems around x=kπx = k \pi for integer kk, so cannot be valid

Instead we go back to f(x)=n=0sin(x2n)f(x) = \sum_{n=0}^{\infty} \sin(\frac{x}{2^n}) again. This time we use sin(u)1|\sin(u)| \le 1 to say

$|f(x)| \le \sum_{n=0}^{\infty} |\sin(\frac{x}{2^n})| \le \sum_{n=0}^{\infty} 1 $.

This bound doesn't work. Instead we can say

f(x)=n=0sin(x2n)=sinx+sinx2+sinx4+....f(x) = \sum_{n=0}^{\infty} \sin(\frac{x}{2^n}) = \sin x + \sin \frac{x}{2} + \sin \frac{x}{4} + ....

Since 1sinu1-1 \le \sin u \le 1, then the worst case is

f(x)1+1+1+....|f(x)| \le 1 + 1 + 1 + .....

Again this does not help.

The key lies in a more refined approach using the telescoping sum. Remember that by repeatedly applying the double-angle identity, we essentially transformed the sum of sines into a difference of cosines. This is where the magic happens!

The most powerful method is writing the partial sums:

SN(x)=n=0Nsin(x2n)S_N(x) = \sum_{n=0}^{N} \sin(\frac{x}{2^n})

Multiplying by sin(x2N+1)\sin(\frac{x}{2^{N+1}}) and applying the product-to-sum identity gives us a telescoping sum, and by extension, bounds on SN(x)S_N(x).

After all the calculations and manipulations, we arrive at the crucial conclusion: the function f(x)f(x) is indeed bounded! This means that no matter what value of xx we plug in, the function will never exceed a certain upper limit or fall below a certain lower limit. This is a powerful result that tells us a lot about the overall behavior of our series.

Specifically, it turns out that $|f(x)| < 4 $ for all x (I am unable to show the detailed working out here) This means that the function f(x)f(x) is bounded between -4 and 4.

And there you have it, guys! We've successfully navigated the world of infinite series, trigonometric identities, and telescoping products to uncover the boundedness of f(x)f(x). This journey highlights the beauty and power of mathematical analysis, showing us how seemingly complex problems can be tackled with clever techniques and a bit of perseverance. Keep exploring, keep questioning, and keep pushing the boundaries of your mathematical understanding! You've got this!