Problem 14
Question
Suppose that \(h\) is integrable and that \(\int_{-1}^{1} h(r) d r=0\) and \(\int_{-1}^{3} h(r) d r=6 .\) Find A. \(\int_{1}^{3} h(r) d r\) B. \(-\int_{3}^{1} h(u) d u\)
Step-by-Step Solution
Verified Answer
A: 6, B: 6.
1Step 1: Understanding the Problem
We need to find two integration values based on the given integrals of the integrable function \( h(r) \). We have two pieces of information: \( \int_{-1}^{1} h(r) \, dr = 0 \) and \( \int_{-1}^{3} h(r) \, dr = 6 \). Using these, we can determine the other requested integrals.
2Step 1: Calculating \( \int_{1}^{3} h(r) \, dr \)
First, we use the property of definite integrals which states that \( \int_{a}^{c} f(x)\,dx = \int_{a}^{b} f(x)\,dx + \int_{b}^{c} f(x)\,dx \). In our problem, this gives us the equation\[\int_{-1}^{3} h(r) \, dr = \int_{-1}^{1} h(r) \, dr + \int_{1}^{3} h(r) \, dr.\]Substitute the known values:\[6 = 0 + \int_{1}^{3} h(r) \, dr.\]Thus, \( \int_{1}^{3} h(r) \, dr = 6 \).
3Step 2: Calculating \( -\int_{3}^{1} h(u) \, du \)
Recalling the property of definite integrals known as mutual reversal, \( \int_{a}^{b} f(x) \, dx = -\int_{b}^{a} f(x) \, dx \), we have:\[-\int_{3}^{1} h(u) \, du = \int_{1}^{3} h(u) \, du.\]Since we have already computed \( \int_{1}^{3} h(r) \, dr = 6 \), it follows that \[-\int_{3}^{1} h(u) \, du = 6.\]
Key Concepts
Integral PropertiesMutual ReversalIntegrable Function
Integral Properties
Integral properties are essential tools that help us solve and understand definite integrals. These properties simplify computations and provide deeper insights into the behavior of functions. Let’s delve into some crucial properties that were used in the problem:
- Linearity of integrals: This property states that the integral of a sum is the sum of the integrals. This allows us to break integrals into more manageable parts. For a function \( h(r) \), it uses the equation \[ \int_{a}^{c} h(r) \, dr = \int_{a}^{b} h(r) \, dr + \int_{b}^{c} h(r) \, dr \] as seen in the solution process.
- Additivity of intervals: Within linearity, the additivity of intervals allows us to evaluate an integral over a composite interval by adding integrals over sub-intervals. This was specifically used in the problem to split the integral from \(-1\) to \(3\) into two: from \(-1\) to \(1\) and from \(1\) to \(3\).
Mutual Reversal
The concept of mutual reversal in definite integrals reveals an interesting symmetry property. Mutual reversal states that reversing the limits of an integral changes the sign of the result:
- The integral \( \int_{a}^{b} h(x) \, dx \) is equal to \(-\int_{b}^{a} h(x) \, dx \).
Integrable Function
An integrable function is one for which a definite integral can be evaluated over a given interval. In simpler terms, it's a function that doesn't "misbehave" too much. For a function to be integrable on an interval, certain conditions must be met:
- The function should be bounded on the interval, meaning it doesn't go to infinity.
- There should be a finite number of discontinuities. Typically, it can still be integrated if these discontinuities are jump discontinuities.
Other exercises in this chapter
Problem 13
Evaluate the integrals. $$\int_{\pi / 2}^{0} \frac{1+\cos 2 t}{2} d t$$
View solution Problem 13
Express the sums in sigma notation. The form of your answer will depend on your choice of the lower limit of summation. $$\frac{1}{2}+\frac{1}{4}+\frac{1}{8}+\f
View solution Problem 14
Evaluate the indefinite integrals by using the given substitutions to reduce the integrals to standard form. $$\int \frac{1}{x^{2}} \cos ^{2}\left(\frac{1}{x}\r
View solution Problem 14
An object is shot straight upward from sea level with an initial velocity of \(400 \mathrm{ft} / \mathrm{sec}.\) a. Assuming that gravity is the only force acti
View solution