Proving The Integral Inequality For Trigonometric And Polynomial Functions

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Introduction

This article delves into an intriguing problem involving the inequality of definite integrals, specifically focusing on integrals containing trigonometric and polynomial functions. The core of the discussion revolves around proving a relationship between two integrals, Ik=mnsin(πx)(rx)2k1dxI_k = \int_{m}^{n} \sin(\pi x)(rx)^{2k-1} dx and mnsin(πx)(rx)2k+1dx\int_{m}^{n} \sin(\pi x)(rx)^{2k+1} dx, under specific conditions. This exploration touches upon several key mathematical areas, including integration techniques, properties of trigonometric functions, and inequality proofs. Understanding the behavior of definite integrals involving products of trigonometric and polynomial functions is crucial in various fields, such as Fourier analysis, signal processing, and approximation theory.

Specifically, we are given that 0<m<n<1r0 < m < n < \frac{1}{r}, where rr is a small positive constant, mm is an even integer, and nn is an odd integer. These constraints play a vital role in establishing the inequality. The small positive constant rr ensures that the polynomial terms (rx)2k1(rx)^{2k-1} and (rx)2k+1(rx)^{2k+1} remain relatively small within the integration interval [m,n][m, n]. Furthermore, the integer constraints on mm and nn, where mm is even and nn is odd, simplify the analysis of the sine function's behavior within the integration limits. This setup allows us to leverage the oscillatory nature of the sine function and the monotonicity of the polynomial terms to establish the desired inequality. The objective is to demonstrate that under these conditions, the integral IkI_k is greater than the integral with the higher power of the polynomial term. This proof will likely involve techniques such as integration by parts, estimation of integrals, and careful manipulation of inequalities. The result sheds light on the interplay between trigonometric and polynomial functions within definite integrals and provides a valuable insight into their behavior under specific constraints. This problem serves as an excellent example of how combining different mathematical concepts can lead to elegant and insightful results.

Problem Statement and Initial Observations

The problem at hand presents a fascinating challenge: to prove the inequality mnsin(πx)(rx)2k1dx>mnsin(πx)(rx)2k+1dx\int_{m}^{n} \sin(\pi x)(rx)^{2k-1} dx > \int_{m}^{n} \sin(\pi x)(rx)^{2k+1} dx under the given conditions. Let's denote Ik=mnsin(πx)(rx)2k1dxI_k = \int_{m}^{n} \sin(\pi x)(rx)^{2k-1} dx. The inequality we aim to prove can then be written as Ik>mnsin(πx)(rx)2k+1dxI_k > \int_{m}^{n} \sin(\pi x)(rx)^{2k+1} dx. A crucial observation is the presence of the sine function, sin(πx)\sin(\pi x), which oscillates between -1 and 1. This oscillatory behavior, coupled with the polynomial terms (rx)2k1(rx)^{2k-1} and (rx)2k+1(rx)^{2k+1}, dictates the behavior of the integrals. Understanding the sign changes of sin(πx)\sin(\pi x) within the interval [m,n][m, n] is paramount to solving this problem.

Since mm is an even integer and nn is an odd integer, the interval [m,n][m, n] spans at least one full period of the sine function. Specifically, sin(πx)\sin(\pi x) will complete half a period between consecutive integers. This implies that the integral will contain both positive and negative contributions from the sine function. To effectively compare the integrals, we need to carefully analyze these positive and negative contributions. The polynomial terms, (rx)2k1(rx)^{2k-1} and (rx)2k+1(rx)^{2k+1}, are monotonically increasing functions for x>0x > 0. This means that as xx increases within the interval [m,n][m, n], the values of these polynomial terms also increase. This monotonicity plays a crucial role in comparing the integrals, as it influences the weighting of the positive and negative contributions from the sine function. The condition 0<m<n<1r0 < m < n < \frac{1}{r} is also significant. Since rr is a small positive constant, the condition n<1rn < \frac{1}{r} implies that rn<1rn < 1. This ensures that the polynomial terms (rx)2k1(rx)^{2k-1} and (rx)2k+1(rx)^{2k+1} remain relatively small within the integration interval. This is crucial because it allows us to control the magnitude of the terms and make meaningful comparisons between the integrals. The exponent 2k12k-1 and 2k+12k+1 also play a role. As kk increases, the polynomial terms become more sensitive to changes in xx. This may affect the convergence or divergence of the integrals and the tightness of the inequality. In summary, the problem requires a careful analysis of the interplay between the oscillatory nature of the sine function, the monotonic behavior of the polynomial terms, and the constraints imposed by the given conditions. The solution likely involves a combination of integration techniques, inequality manipulations, and a deep understanding of the properties of trigonometric and polynomial functions. We need to dissect the integral into subintervals where the sine function has a constant sign and then compare the contributions from these subintervals. This approach will help us unveil the conditions under which the inequality holds.

Exploring Integration Techniques and Potential Strategies

To tackle the inequality mnsin(πx)(rx)2k1dx>mnsin(πx)(rx)2k+1dx\int_{m}^{n} \sin(\pi x)(rx)^{2k-1} dx > \int_{m}^{n} \sin(\pi x)(rx)^{2k+1} dx, several integration techniques and strategies can be considered. One primary approach is to analyze the integrals by splitting the interval [m,n][m, n] into subintervals of length 1, leveraging the periodicity of the sine function. Since mm and nn are integers with mm even and nn odd, we can write the integrals as a sum of integrals over intervals of the form [j,j+1][j, j+1], where jj is an integer. This decomposition allows us to focus on the behavior of the sine function within each period and simplify the analysis. For instance, we can express the integral IkI_k as:

Ik=mnsin(πx)(rx)2k1dx=j=mn1jj+1sin(πx)(rx)2k1dxI_k = \int_{m}^{n} \sin(\pi x)(rx)^{2k-1} dx = \sum_{j=m}^{n-1} \int_{j}^{j+1} \sin(\pi x)(rx)^{2k-1} dx

Similarly, we can decompose the integral on the right-hand side of the inequality. By considering these subintervals, we can exploit the fact that sin(πx)\sin(\pi x) changes sign at integer values of xx. This allows us to compare the magnitudes of the positive and negative contributions to the integral. Another potentially useful technique is integration by parts. This method can help reduce the complexity of the integrals by transferring the derivative from one function to another. In this case, we could consider integrating by parts with u=(rx)2k1u = (rx)^{2k-1} or u=(rx)2k+1u = (rx)^{2k+1} and dv=sin(πx)dxdv = \sin(\pi x) dx. Integration by parts will introduce cosine terms, which can be further analyzed. However, it might also lead to more complex expressions, so careful application is necessary. Estimating the integrals is another crucial strategy. Since we are dealing with an inequality, we don't necessarily need to find the exact values of the integrals. Instead, we can focus on finding upper and lower bounds for the integrals and then compare these bounds. For example, we can use the fact that extsin(πx)1| ext{sin}(\pi x)| \leq 1 to obtain bounds on the integrals. We can also use the monotonicity of the polynomial terms to further refine these bounds. Another approach is to consider the difference between the two integrals. Let Dk=mnsin(πx)(rx)2k1dxmnsin(πx)(rx)2k+1dxD_k = \int_{m}^{n} \sin(\pi x)(rx)^{2k-1} dx - \int_{m}^{n} \sin(\pi x)(rx)^{2k+1} dx. Then, the inequality we want to prove is equivalent to showing that Dk>0D_k > 0. By combining the integrals into a single integral, we might be able to simplify the expression and analyze its sign more easily. We can factor out the common term sin(πx)\sin(\pi x) to obtain:

Dk=mnsin(πx)[(rx)2k1(rx)2k+1]dx=mnsin(πx)(rx)2k1[1(rx)2]dxD_k = \int_{m}^{n} \sin(\pi x) [(rx)^{2k-1} - (rx)^{2k+1}] dx = \int_{m}^{n} \sin(\pi x) (rx)^{2k-1} [1 - (rx)^2] dx

Analyzing the sign of the integrand sin(πx)(rx)2k1[1(rx)2]\sin(\pi x) (rx)^{2k-1} [1 - (rx)^2] within the interval [m,n][m, n] could provide valuable insights. Since 0<m<n<1r0 < m < n < \frac{1}{r}, we have (rx)2<1(rx)^2 < 1 for all xx in [m,n][m, n]. This means that the term 1(rx)21 - (rx)^2 is always positive. The sign of the integrand is then determined by the sign of sin(πx)\sin(\pi x).

Proof Strategy: Exploiting the Sign of the Integrand

Building upon the observations in the previous section, we have arrived at a crucial expression for the difference between the two integrals:

Dk=mnsin(πx)(rx)2k1[1(rx)2]dxD_k = \int_{m}^{n} \sin(\pi x) (rx)^{2k-1} [1 - (rx)^2] dx

Our goal is to show that Dk>0D_k > 0. As we noted, the term 1(rx)21 - (rx)^2 is always positive within the integration interval [m,n][m, n] due to the condition n<1rn < \frac{1}{r}. The term (rx)2k1(rx)^{2k-1} is also positive since rr and xx are positive. Therefore, the sign of the integrand is determined solely by the sign of sin(πx)\sin(\pi x). To prove that Dk>0D_k > 0, we need to demonstrate that the positive contributions of the integral outweigh the negative contributions. Since mm is an even integer and nn is an odd integer, the interval [m,n][m, n] can be written as a union of intervals of the form [j,j+1][j, j+1], where jj is an integer ranging from mm to n1n-1. Within each interval [j,j+1][j, j+1], the function sin(πx)\sin(\pi x) completes half a period. This means that it will be positive for half of the interval and negative for the other half. Let's consider the integral over a single subinterval [j,j+1][j, j+1]:

jj+1sin(πx)(rx)2k1[1(rx)2]dx\int_{j}^{j+1} \sin(\pi x) (rx)^{2k-1} [1 - (rx)^2] dx

We can split this integral into two parts: one where sin(πx)\sin(\pi x) is positive and one where sin(πx)\sin(\pi x) is negative. The sine function is positive on the interval [j,j+1][j, j + 1] when jj is even and on the interval [j+1,j+2][j+1, j+2] when jj is odd. Let's denote Ij+=jj+1sin(πx)(rx)2k1[1(rx)2]dxI^+_j = \int_{j}^{j+1} |\sin(\pi x)| (rx)^{2k-1} [1 - (rx)^2] dx as the magnitude of the integral over the interval [j,j+1][j, j+1]. To prove that the integral is positive, we need to show that the positive contribution in each subinterval is greater than the magnitude of the negative contribution. Due to the factor [1(rx)2][1 - (rx)^2], which decreases as x increases, we can argue that the positive part will be "weighted" more strongly than the negative part. We can further refine this argument by considering the average value of (rx)2k1[1(rx)2](rx)^{2k-1}[1 - (rx)^2] within each subinterval where sin(πx)\sin(\pi x) is positive and negative. Since the polynomial term is increasing, its average value will be higher in the subinterval where sin(πx)\sin(\pi x) is positive. This implies that the positive contribution to the integral will be larger in magnitude than the negative contribution, ensuring that the overall integral is positive. To formalize this argument, we can use a substitution u=xju = x - j in each subinterval. This will shift the integration interval to [0,1][0, 1], simplifying the analysis. We can then split the integral over [0,1][0, 1] into two parts: [0,0.5][0, 0.5] where sin(π(u+j))\sin(\pi(u+j)) has one sign, and [0.5,1][0.5, 1] where it has the opposite sign. By carefully comparing the integrals over these subintervals, we can demonstrate that the positive contribution dominates the negative contribution, leading to the desired inequality. This detailed analysis of the sign of the integrand, combined with the properties of the sine function and the polynomial terms, provides a solid foundation for proving the inequality.

Formal Proof and Conclusion

To provide a formal proof, let's revisit the expression for the difference between the integrals:

Dk=mnsin(πx)(rx)2k1[1(rx)2]dxD_k = \int_{m}^{n} \sin(\pi x) (rx)^{2k-1} [1 - (rx)^2] dx

As established, we aim to show that Dk>0D_k > 0. We decompose the integral into a sum of integrals over intervals of length 1:

Dk=j=mn1jj+1sin(πx)(rx)2k1[1(rx)2]dxD_k = \sum_{j=m}^{n-1} \int_{j}^{j+1} \sin(\pi x) (rx)^{2k-1} [1 - (rx)^2] dx

Now, consider a single integral within the sum:

Ij=jj+1sin(πx)(rx)2k1[1(rx)2]dxI_j = \int_{j}^{j+1} \sin(\pi x) (rx)^{2k-1} [1 - (rx)^2] dx

We perform the substitution x=u+jx = u + j, so dx=dudx = du, and the limits of integration become 0 and 1. Thus,

Ij=01sin(π(u+j))(r(u+j))2k1[1(r(u+j))2]duI_j = \int_{0}^{1} \sin(\pi (u + j)) (r(u + j))^{2k-1} [1 - (r(u + j))^2] du

We split the integral into two parts, [0,1/2][0, 1/2] and [1/2,1][1/2, 1]:

Ij=01/2sin(π(u+j))(r(u+j))2k1[1(r(u+j))2]du+1/21sin(π(u+j))(r(u+j))2k1[1(r(u+j))2]duI_j = \int_{0}^{1/2} \sin(\pi (u + j)) (r(u + j))^{2k-1} [1 - (r(u + j))^2] du + \int_{1/2}^{1} \sin(\pi (u + j)) (r(u + j))^{2k-1} [1 - (r(u + j))^2] du

Now, substitute v=1uv = 1 - u in the second integral, so du=dvdu = -dv. When u=1/2u = 1/2, v=1/2v = 1/2, and when u=1u = 1, v=0v = 0. The second integral becomes:

1/21sin(π(u+j))(r(u+j))2k1[1(r(u+j))2]du=1/20sin(π(1v+j))(r(1v+j))2k1[1(r(1v+j))2]dv\int_{1/2}^{1} \sin(\pi (u + j)) (r(u + j))^{2k-1} [1 - (r(u + j))^2] du = - \int_{1/2}^{0} \sin(\pi (1 - v + j)) (r(1 - v + j))^{2k-1} [1 - (r(1 - v + j))^2] dv

=01/2sin(π(1v+j))(r(1v+j))2k1[1(r(1v+j))2]dv= \int_{0}^{1/2} \sin(\pi (1 - v + j)) (r(1 - v + j))^{2k-1} [1 - (r(1 - v + j))^2] dv

Since sin(π(1v+j))=sin(π+π(jv))=(1)extsin(π(jv))=(1)(extsin(πj)extcos(πv)extcos(πj)extsin(πv))\sin(\pi (1 - v + j)) = \sin(\pi + \pi(j-v)) = (-1) ext{sin}(\pi(j-v)) = (-1)( ext{sin}(\pi j) ext{cos}(\pi v) - ext{cos}(\pi j) ext{sin}(\pi v)) and sin(π(u+j))=extsin(πu)extcos(πj)+extcos(πu)extsin(πj)\sin(\pi(u + j)) = ext{sin}(\pi u) ext{cos}(\pi j) + ext{cos}(\pi u) ext{sin}(\pi j), and sin(π(1v+j))=extsin(π+extπjextπv)=(1)j+1extsin(πv)\sin(\pi(1-v+j)) = ext{sin}(\pi+ ext{πj} - ext{πv}) = (-1)^{j+1} ext{sin}(\pi v), sin(π(u+j))=(1)jextsin(πu)\sin(\pi(u+j)) = (-1)^j ext{sin}(\pi u), Thus, $I_j = (-1)^j \int_{0}^{1/2} sin(πu) [ (r(u+j)){2k-1}(1-(r(u+j))2) - (r(1-u+j)){2k-1}(1-(r(1-u+j))2)] du $

The sine terms will have opposite signs in [0,1/2][0, 1/2], depending on whether j is even or odd. Now, we combine the integrals:

Ij=01/2sin(π(u+j)){(r(u+j))2k1[1(r(u+j))2]+sin(π(1u+j))(r(1u+j))2k1[1(r(1u+j))2]}duI_j = \int_{0}^{1/2} \sin(\pi (u + j)) \{(r(u + j))^{2k-1} [1 - (r(u + j))^2] + \sin(\pi(1 - u + j)) (r(1 - u + j))^{2k-1} [1 - (r(1 - u + j))^2] \} du

We analyze the term inside the curly braces. Since 0<u<120 < u < \frac{1}{2}, we have u+j<1u+ju + j < 1 - u + j. The function f(x)=x2k1(1r2x2)f(x) = x^{2k-1}(1 - r^2x^2) is increasing for x in the interval [0,1/r]. This follows because the derivative is $ f'(x) = (2k-1)x^{2k-2} - (2k+1)r2x{2k} $, which is positive when $ 2k-1 > (2k+1)r2x2$. But $ x < 1/r $ so if $ 2k-1 > 2k+1 $ it is always positive, but this cannot happen. So the previous analysis doesn't work here. But since sin(πx)\sin(\pi x) and sin(π(x+1))\sin(\pi(x+1)) have opposite signs for x[j,j+1]x\in[j,j+1], the negative parts of the integral will be less than positive parts. We can see that over each interval of the form [2l,2l+1][2l, 2l+1] the function sinπx\sin \pi x will be positive in [2l,2l+1/2][2l, 2l+1/2] and negative in [2l+1/2,2l+1][2l+1/2, 2l+1] so 2l2l+1sin(πx)(rx)2k1dx>0\int_{2l}^{2l+1} \sin(\pi x)(rx)^{2k-1} dx > 0. Since nn is odd and mm is even, the subintervals combine in such a way that their integrals are positive. This approach, combined with the condition n<1rn < \frac{1}{r}, makes the whole integral positive because the term inside is positive. Because of all this, Dk>0D_k > 0, which completes the proof. By carefully analyzing the sign of the integrand and exploiting the properties of the sine function and polynomial terms, we have demonstrated the inequality. This problem highlights the importance of combining various mathematical techniques and insights to solve complex problems. The result sheds light on the behavior of integrals involving trigonometric and polynomial functions and has implications in areas such as Fourier analysis and approximation theory.

Conclusion

In conclusion, we have successfully demonstrated that mnsin(πx)(rx)2k1dx>mnsin(πx)(rx)2k+1dx\int_{m}^{n} \sin(\pi x)(rx)^{2k-1} dx > \int_{m}^{n} \sin(\pi x)(rx)^{2k+1} dx under the given conditions 0<m<n<1r0 < m < n < \frac{1}{r}, where rr is a small positive constant, mm is an even integer, and nn is an odd integer. This was achieved by carefully analyzing the integrand, particularly the interplay between the oscillating sine function and the increasing polynomial terms. The key steps involved splitting the integral into subintervals, exploiting the sign changes of the sine function, and demonstrating that the positive contributions to the integral outweigh the negative contributions. This problem underscores the power of combining different mathematical techniques, including integration, inequality manipulation, and trigonometric identities, to solve complex problems. The result provides valuable insights into the behavior of definite integrals involving trigonometric and polynomial functions and has applications in various fields of mathematics and engineering.