Evaluating The Integral Sum I_n = ∫ Tan^n(x) Dx

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In the fascinating realm of calculus, integrals often present both challenges and opportunities for elegant solutions. The problem at hand, In=tannxdx{ I_n = \int \tan^n x \, dx }, delves into the world of trigonometric integrals, specifically those involving powers of the tangent function. Our goal is to evaluate a particular sum involving these integrals, namely I0+I1+2(I2+I3++I8)+I9+I10{ I_0 + I_1 + 2(I_2 + I_3 + \ldots + I_8) + I_9 + I_{10} }. This task requires us to not only understand the basic integral of tannx{ \tan^n x } but also to identify and exploit a recursive relationship that simplifies the overall computation. In this article, we will meticulously explore the properties of these integrals, derive the necessary recurrence relation, and then apply it to efficiently compute the desired sum. This exploration will not only showcase the power of calculus but also highlight the beauty of mathematical problem-solving through strategic simplification and pattern recognition. The journey begins with understanding the fundamental integral and how it behaves as the power n{ n } changes. We will then venture into the derivation of the recurrence relation, a crucial step in making the problem tractable. Finally, we will apply this relation to compute the sum, revealing the solution in a clear and concise manner. This exercise is a testament to the interconnectedness of mathematical concepts and the rewarding experience of unraveling complex problems through thoughtful analysis and application of established principles. By the end of this discussion, you will have a comprehensive understanding of how to approach and solve integrals of this nature, equipping you with valuable skills for further mathematical explorations.

Understanding the Base Cases: I0{ I_0 } and I1{ I_1 }

Before diving into the general formula for In{ I_n }, it is crucial to establish a firm understanding of the base cases, namely I0{ I_0 } and I1{ I_1 }. These integrals serve as the foundation upon which we will build our understanding of the more complex cases. I0{ I_0 } represents the integral of tan0x{ \tan^0 x }, which simplifies to the integral of 1. This is a fundamental integral, and its solution is straightforward. I1{ I_1 }, on the other hand, represents the integral of tanx{ \tan x }, which requires a slightly more nuanced approach. The integral of tanx{ \tan x } is not as immediately apparent as the integral of 1, but it is a well-known result that can be derived using basic trigonometric identities and substitution techniques. Understanding these base cases is not merely a preliminary step; it is essential for recognizing patterns and formulating a general solution for In{ I_n }. The simplicity of I0{ I_0 } provides a clear starting point, while the slightly increased complexity of I1{ I_1 } introduces us to the challenges that lie ahead. Moreover, these base cases often play a crucial role in recursive formulas, where the solution for a given n{ n } is expressed in terms of solutions for smaller values of n{ n }. Therefore, a thorough grasp of I0{ I_0 } and I1{ I_1 } is indispensable for tackling the overall problem. Let's begin by explicitly evaluating these integrals. The integral I0=tan0xdx=1dx=x+C{ I_0 = \int \tan^0 x \, dx = \int 1 \, dx = x + C }, where C{ C } is the constant of integration. This result is intuitive and serves as a solid starting point. Next, we consider I1=tanxdx{ I_1 = \int \tan x \, dx }. To solve this, we rewrite tanx{ \tan x } as sinxcosx{ \frac{\sin x}{\cos x} }. Now, the integral becomes sinxcosxdx{ \int \frac{\sin x}{\cos x} \, dx }. A simple substitution, letting u=cosx{ u = \cos x }, yields du=sinxdx{ du = -\sin x \, dx }, and the integral transforms to 1udu=lnu+C=lncosx+C{ -\int \frac{1}{u} \, du = -\ln |u| + C = -\ln |\cos x| + C }. We can also express this as lnsecx+C{ \ln |\sec x| + C }, which is a more conventional form. These results for I0{ I_0 } and I1{ I_1 } are not just isolated solutions; they are the cornerstones upon which our further analysis will be built. With these in hand, we are well-equipped to explore the recurrence relation that governs the behavior of In{ I_n } for higher values of n{ n }.

Deriving the Recurrence Relation for In{ I_n }

The heart of solving this problem lies in discovering and utilizing a recurrence relation for the integral In=tannxdx{ I_n = \int \tan^n x \, dx }. A recurrence relation expresses In{ I_n } in terms of Ik{ I_k } where k<n{ k < n }, allowing us to break down a complex integral into simpler ones. To derive this relation, we begin by manipulating the integrand tannx{ \tan^n x } strategically. We can rewrite tannx{ \tan^n x } as tann2xtan2x{ \tan^{n-2} x \cdot \tan^2 x }. This seemingly simple step is crucial because it allows us to leverage the trigonometric identity tan2x=sec2x1{ \tan^2 x = \sec^2 x - 1 }. Substituting this identity, we get tannx=tann2x(sec2x1){ \tan^n x = \tan^{n-2} x (\sec^2 x - 1) }, which can be further expanded to tannx=tann2xsec2xtann2x{ \tan^n x = \tan^{n-2} x \sec^2 x - \tan^{n-2} x }. Now, when we integrate In=tannxdx{ I_n = \int \tan^n x \, dx }, we can split the integral into two parts using the rewritten integrand: In=(tann2xsec2xtann2x)dx=tann2xsec2xdxtann2xdx{ I_n = \int (\tan^{n-2} x \sec^2 x - \tan^{n-2} x) \, dx = \int \tan^{n-2} x \sec^2 x \, dx - \int \tan^{n-2} x \, dx }. Notice that the second integral is simply In2{ I_{n-2} }. The first integral, tann2xsec2xdx{ \int \tan^{n-2} x \sec^2 x \, dx }, can be solved using a straightforward substitution. Let u=tanx{ u = \tan x }, then du=sec2xdx{ du = \sec^2 x \, dx }. The integral then becomes un2du{ \int u^{n-2} \, du }, which is a simple power rule integration: un1n1+C=tann1xn1+C{ \frac{u^{n-1}}{n-1} + C = \frac{\tan^{n-1} x}{n-1} + C }. Thus, we have In=tann1xn1In2{ I_n = \frac{\tan^{n-1} x}{n-1} - I_{n-2} }. This is the recurrence relation we were seeking. It elegantly connects In{ I_n } to In2{ I_{n-2} }, allowing us to express higher-order integrals in terms of lower-order ones. This relation is the key to efficiently computing the sum in the original problem. By repeatedly applying this recurrence, we can express all the integrals in the sum in terms of I0{ I_0 } and I1{ I_1 }, which we have already evaluated. The beauty of this approach is that it transforms a seemingly daunting problem into a manageable sequence of steps. The recurrence relation not only simplifies the calculation but also provides deeper insight into the structure of these integrals. It reveals a fundamental relationship between integrals of different orders, showcasing the interconnectedness of mathematical concepts. With this powerful tool in hand, we are now ready to tackle the main problem and compute the desired sum.

Computing the Sum: I0+I1+2(I2+I3++I8)+I9+I10{ I_0 + I_1 + 2(I_2 + I_3 + \ldots + I_8) + I_9 + I_{10} }

Now that we have derived the recurrence relation In=tann1xn1In2{ I_n = \frac{\tan^{n-1} x}{n-1} - I_{n-2} }, and established the base cases I0=x+C{ I_0 = x + C } and I1=lnsecx+C{ I_1 = \ln |\sec x| + C }, we are well-equipped to compute the given sum: I0+I1+2(I2+I3++I8)+I9+I10{ I_0 + I_1 + 2(I_2 + I_3 + \ldots + I_8) + I_9 + I_{10} }. The strategy here is to apply the recurrence relation to each term in the sum, expressing them in terms of I0{ I_0 } and I1{ I_1 }, and then look for patterns and cancellations that simplify the overall expression. Let's begin by applying the recurrence to the terms within the parentheses. For I2{ I_2 }, we have I2=tanx1I0=tanxI0{ I_2 = \frac{\tan x}{1} - I_0 = \tan x - I_0 }. For I3{ I_3 }, we have I3=tan2x2I1{ I_3 = \frac{\tan^2 x}{2} - I_1 }. We continue this process for each term up to I8{ I_8 }. To make the computation more manageable, let's write out the first few terms and see if a pattern emerges:

  • I2=tanxI0{ I_2 = \tan x - I_0 }
  • I3=tan2x2I1{ I_3 = \frac{\tan^2 x}{2} - I_1 }
  • I4=tan3x3I2=tan3x3(tanxI0){ I_4 = \frac{\tan^3 x}{3} - I_2 = \frac{\tan^3 x}{3} - (\tan x - I_0) }
  • I5=tan4x4I3=tan4x4(tan2x2I1){ I_5 = \frac{\tan^4 x}{4} - I_3 = \frac{\tan^4 x}{4} - (\frac{\tan^2 x}{2} - I_1) }

We can see that each In{ I_n } term involves a tann1xn1{ \frac{\tan^{n-1} x}{n-1} } term and a In2{ -I_{n-2} } term. Now, let's consider the sum 2(I2+I3++I8){ 2(I_2 + I_3 + \ldots + I_8) }. When we substitute the recurrence relation for each term, we get a series of tann1xn1{ \frac{\tan^{n-1} x}{n-1} } terms and a series of Ik{ I_k } terms. The key observation is that many of these Ik{ I_k } terms will cancel out due to the alternating signs in the recurrence relation. For instance, the I0{ -I_0 } from I2{ I_2 } will be canceled by the I0{ I_0 } that appears in I4{ I_4 }. Similarly, the I1{ -I_1 } from I3{ I_3 } will be canceled by the I1{ I_1 } that appears in I5{ I_5 }. This pattern of cancellation continues throughout the sum. Now, let's apply the recurrence relation to I9{ I_9 } and I10{ I_{10} } as well:

  • I9=tan8x8I7{ I_9 = \frac{\tan^8 x}{8} - I_7 }
  • I10=tan9x9I8{ I_{10} = \frac{\tan^9 x}{9} - I_8 }

With all the terms expressed using the recurrence relation, we can rewrite the entire sum as: I0+I1+2(tanxI0+tan2x2I1+tan3x3I2++tan7x7I6)+tan8x8I7+tan9x9I8{ I_0 + I_1 + 2(\tan x - I_0 + \frac{\tan^2 x}{2} - I_1 + \frac{\tan^3 x}{3} - I_2 + \ldots + \frac{\tan^7 x}{7} - I_6) + \frac{\tan^8 x}{8} - I_7 + \frac{\tan^9 x}{9} - I_8 }. After careful observation and pattern matching, we can write out the sum as follows:

I0+I1+2n=28In+I9+I10=I0+I1+2n=28(tann1(x)n1In2)+tan8(x)8I7+tan9(x)9I8{I_0 + I_1 + 2\sum_{n=2}^{8} I_n + I_9 + I_{10} = I_0 + I_1 + 2\sum_{n=2}^{8} \left( \frac{\tan^{n-1}(x)}{n-1} - I_{n-2} \right) + \frac{\tan^8(x)}{8} - I_7 + \frac{\tan^9(x)}{9} - I_8}

Now let's look at expanding the summation and combining terms. The summation becomes:

2n=28tann1(x)n12n=28In2{2\sum_{n=2}^{8} \frac{\tan^{n-1}(x)}{n-1} - 2\sum_{n=2}^{8} I_{n-2}}

The first part of the sum is easy to handle. For the second part, we need to re-index the summation:

2n=28In2=2(I0+I1+I2+I3+I4+I5+I6){2\sum_{n=2}^{8} I_{n-2} = 2(I_0 + I_1 + I_2 + I_3 + I_4 + I_5 + I_6)}

So the whole expression becomes:

I0+I1+2n=28tann1(x)n12(I0+I1+I2+I3+I4+I5+I6)+tan8(x)8I7+tan9(x)9I8{I_0 + I_1 + 2\sum_{n=2}^{8} \frac{\tan^{n-1}(x)}{n-1} - 2(I_0 + I_1 + I_2 + I_3 + I_4 + I_5 + I_6) + \frac{\tan^8(x)}{8} - I_7 + \frac{\tan^9(x)}{9} - I_8}

We express the terms I2{ I_2 } through I8{ I_8 } using the recurrence relation. After substituting and simplifying, most of the integral terms will cancel out, and we're left with:

n=192tann(x)n+x+lnsec(x){\sum_{n=1}^{9} \frac{2 \tan^{n}(x)}{n} + x + \ln|\sec(x)|}

So, after simplification, the final result is:

tanx+2tan2x2+2tan3x3++2tan7x7+tan8x8+tan9x9(I0+I1){\tan x + \frac{2\tan^2 x}{2} + \frac{2\tan^3 x}{3} + \dots + \frac{2\tan^7 x}{7} + \frac{\tan^8 x}{8} + \frac{\tan^9 x}{9} - (I_0 + I_1)}

Substituting I0=x{ I_0 = x } and I1=lnsecx{ I_1 = \ln|\sec x| }, the sum simplifies to:

tanx+tan2x+23tan3x+12tan4x+25tan5x+13tan6x+27tan7x+18tan8x+19tan9xxlnsecx+C{\tan x + \tan^2 x + \frac{2}{3} \tan^3 x + \frac{1}{2} \tan^4 x + \frac{2}{5} \tan^5 x + \frac{1}{3} \tan^6 x + \frac{2}{7} \tan^7 x + \frac{1}{8} \tan^8 x + \frac{1}{9} \tan^9 x - x - \ln|\sec x| + C}

Where C{ C } is the constant of integration.

Conclusion

In this comprehensive exploration, we have successfully evaluated the sum I0+I1+2(I2+I3++I8)+I9+I10{ I_0 + I_1 + 2(I_2 + I_3 + \ldots + I_8) + I_9 + I_{10} }, where In=tannxdx{ I_n = \int \tan^n x \, dx }. The journey began with understanding the base cases, I0{ I_0 } and I1{ I_1 }, and then progressed to deriving the crucial recurrence relation In=tann1xn1In2{ I_n = \frac{\tan^{n-1} x}{n-1} - I_{n-2} }. This recurrence relation served as the cornerstone of our solution, allowing us to express higher-order integrals in terms of lower-order ones. By repeatedly applying this relation and carefully observing the patterns and cancellations that emerged, we were able to simplify the complex sum into a manageable form. The final result, tanx+tan2x+23tan3x+12tan4x+25tan5x+13tan6x+27tan7x+18tan8x+19tan9xxlnsecx+C{ \tan x + \tan^2 x + \frac{2}{3} \tan^3 x + \frac{1}{2} \tan^4 x + \frac{2}{5} \tan^5 x + \frac{1}{3} \tan^6 x + \frac{2}{7} \tan^7 x + \frac{1}{8} \tan^8 x + \frac{1}{9} \tan^9 x - x - \ln|\sec x| + C }, showcases the power of strategic problem-solving in calculus. This exercise not only reinforces the importance of recurrence relations in simplifying integrals but also highlights the beauty of mathematical interconnectedness. The ability to break down a complex problem into smaller, more manageable parts is a skill that extends far beyond the realm of calculus, making this exploration a valuable learning experience. Furthermore, the process of identifying patterns and exploiting cancellations is a fundamental aspect of mathematical reasoning, and this problem provides an excellent example of how these techniques can be applied effectively. In conclusion, the solution to this problem demonstrates the elegance and efficiency of calculus techniques, reinforcing the idea that even the most daunting mathematical challenges can be overcome with a combination of fundamental knowledge, strategic thinking, and careful execution. The journey through this problem has not only provided us with a specific answer but has also enriched our understanding of mathematical problem-solving in general.