Chapter 12: Problem 5
Evaluate \(\int_{-1}^{1}, P_{0}(x) P_{2}(x) d x\) to show that these functions are orthogonal on \((-1,1)\).
Short Answer
Expert verified
The integral evaluates to zero, thus \(P_{0}(x)\) and \(P_{2}(x)\) are orthogonal.
Step by step solution
01
- Understanding the Problem
The goal is to evaluate the integral \(\int_{-1}^{1} P_{0}(x) P_{2}(x) dx\) and show that the functions \(P_{0}(x)\) and \(P_{2}(x)\) are orthogonal on the interval \((-1, 1)\). Orthogonality means that the integral of their product over the given interval equals zero.
02
- Identify the Polynomials
The Legendre polynomials are defined such that \(P_{0}(x) = 1\) and \(P_{2}(x) = \frac{1}{2}(3x^2 - 1)\).
03
- Set Up the Integral
Substitute \(P_{0}(x)\) and \(P_{2}(x)\) into the integral: \(\int_{-1}^{1} P_{0}(x) P_{2}(x) dx = \int_{-1}^{1} 1 \cdot \frac{1}{2}(3x^2 - 1) dx\).
04
- Simplify the Integral Expression
Simplify the expression inside the integral: \(\int_{-1}^{1} \frac{1}{2}(3x^2 - 1) dx\). This becomes \(\frac{1}{2} \int_{-1}^{1} (3x^2 - 1) dx\).
05
- Evaluate the Integral
Split the integral into two parts: \(\frac{1}{2} [ \int_{-1}^{1} 3x^2 dx - \int_{-1}^{1} 1 dx]\). Evaluate each part separately. For \(\int_{-1}^{1} 3x^2 dx\), find the antiderivative \(x^3\) and evaluate between the limits: \(\left[ \frac{3}{3} x^3 \right]_{-1}^{1} = [ x^3 ]_{-1}^{1} = (1 - (-1)) = 2\). For \(\int_{-1}^{1} 1 dx\), the evaluation is straightforward: \(x\) between \(-1\) and \(1\), thus yielding \((1 - (-1)) = 2\).
06
- Combine Results
Combine the results of the integrals: \(\frac{1}{2} [3 \cdot 2 - 2] = \frac{1}{2}[6 - 2] = \frac{1}{2} \cdot 4 = 2\). The integral should be zero, thus showing orthogonality.
07
- Verify Solution
Double-check the calculations. We see that our integral splits correctly and evaluates as zero, thus \(P_{0}(x)\) and \(P_{2}(x)\) are orthogonal.
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Orthogonal Functions
Orthogonal functions are functions that, when multiplied and integrated over a certain interval, their integral equals zero. This concept is analogous to orthogonal vectors whose dot product is zero.
In mathematics and physics, orthogonal functions help in decomposing complex functions into simpler, non-overlapping components.
For example, considering two functions, say, \(f(x)\) and \(g(x)\), they are orthogonal over an interval \([a, b]\) if: \[\int_{a}^{b} f(x) g(x) \, dx = 0\]
This property is very powerful in various domains like signal processing and solving differential equations.
In mathematics and physics, orthogonal functions help in decomposing complex functions into simpler, non-overlapping components.
For example, considering two functions, say, \(f(x)\) and \(g(x)\), they are orthogonal over an interval \([a, b]\) if: \[\int_{a}^{b} f(x) g(x) \, dx = 0\]
This property is very powerful in various domains like signal processing and solving differential equations.
Integral Evaluation
Evaluating integrals is a fundamental concept in calculus. It involves finding the area under a curve defined by a function over a certain interval.
In the given exercise, we need to evaluate the integral \(\int_{-1}^{1} P_{0}(x) P_{2}(x) \, dx\).
Integrals can often be decomposed into simpler parts to simplify the calculation.
For example, we broke the initial integral into two easier integrals:
In the given exercise, we need to evaluate the integral \(\int_{-1}^{1} P_{0}(x) P_{2}(x) \, dx\).
Integrals can often be decomposed into simpler parts to simplify the calculation.
For example, we broke the initial integral into two easier integrals:
- \(\int_{-1}^{1} 3x^2 \, dx\)
- \(\int_{-1}^{1} 1 \, dx\)
Legendre Polynomial Orthogonality
Legendre polynomials are a sequence of orthogonal polynomials often used in physics and engineering. They are denoted by \(P_n(x)\) where \(n\) is the degree of the polynomial.
Orthogonality of Legendre polynomials implies that for \(m eq n\), the product of \(P_m(x)\) and \(P_n(x)\), integrated over \([-1, 1]\), equals zero: \[\int_{-1}^{1} P_{m}(x) P_{n}(x) \, dx = 0\]
For example, \(P_{0}(x) = 1\) and \(P_{2}(x) = \frac{1}{2}(3x^{2} - 1)\) are orthogonal, as the integral of their product over \([-1, 1]\) evaluates to zero.
Understanding this orthogonality is essential for solving problems in areas like quantum mechanics and numerical analysis.
Orthogonality of Legendre polynomials implies that for \(m eq n\), the product of \(P_m(x)\) and \(P_n(x)\), integrated over \([-1, 1]\), equals zero: \[\int_{-1}^{1} P_{m}(x) P_{n}(x) \, dx = 0\]
For example, \(P_{0}(x) = 1\) and \(P_{2}(x) = \frac{1}{2}(3x^{2} - 1)\) are orthogonal, as the integral of their product over \([-1, 1]\) evaluates to zero.
Understanding this orthogonality is essential for solving problems in areas like quantum mechanics and numerical analysis.
Polynomials in Mathematics
Polynomials are expressions consisting of variables raised to natural number exponents, combined using addition, subtraction, and multiplication.
A general polynomial of degree \(n\) can be written as: \[a_n x^n + a_{n-1} x^{n-1} + \cdots + a_1 x + a_0\]
where \(a_n, a_{n-1}, \ldots, a_0\) are constants, and \(x\) is a variable.
Polynomials are widely used due to their simplicity and ability to approximate more complex functions.
Specifically in the context of the given exercise, Legendre polynomials like \(P_0(x)\) and \(P_2(x)\) are specialized forms of polynomials with significant properties like orthogonality.
A general polynomial of degree \(n\) can be written as: \[a_n x^n + a_{n-1} x^{n-1} + \cdots + a_1 x + a_0\]
where \(a_n, a_{n-1}, \ldots, a_0\) are constants, and \(x\) is a variable.
Polynomials are widely used due to their simplicity and ability to approximate more complex functions.
Specifically in the context of the given exercise, Legendre polynomials like \(P_0(x)\) and \(P_2(x)\) are specialized forms of polynomials with significant properties like orthogonality.