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The Fundamental Theorem of Calculus

Evaluating an integral exactly as F(b) - F(a) through any antiderivative, and reading the integral of a rate as the total change it accumulates.

Active Calculus, The Fundamental Theorem of Calculus

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5 exercises

Activity 4.4.2

Use the Fundamental Theorem of Calculus to evaluate each of the following integrals exactly. For each, sketch a graph of the integrand on the relevant interval and write one sentence that explains the meaning of the value of the integral in terms of the (net signed) area bounded by the curve.

  1. ∫−14(2−2x) dx\int_{-1}^4 (2-2x) \, dx

  2. ∫0π2sin⁡(x) dx\int_{0}^{\frac{\pi}{2}} \sin(x) \, dx

  3. ∫01ex dx\int_0^1 e^x \, dx

  4. ∫−11x5 dx\int_{-1}^{1} x^5 \, dx

  5. ∫02(3x3−2x2−ex) dx\int_0^2 (3x^3 - 2x^2 - e^x) \, dx

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Activity 4.4.3

Use your knowledge of derivatives of basic functions to complete Table of antiderivatives. For each entry, your task is to find a function FF whose derivative is the given function ff. When finished, use the FTC and the results in the table to evaluate the three given definite integrals.

  1. ∫01(x3−x−ex+2) dx\displaystyle \int_0^1 \left(x^3 - x - e^x + 2\right) \,dx

  2. ∫0π/3(2sin⁡(t)−4cos⁡(t)+sec⁡2(t)−π) dt\displaystyle \int_0^{\pi/3} (2\sin (t) - 4\cos(t) + \sec^2(t) - \pi) \, dt

  3. ∫01(x−x2) dx\displaystyle \int_0^1 (\sqrt{x}-x^2) \, dx

2.5

Exercise 13

When an aircraft attempts to climb as rapidly as possible, its climb rate (in feet per minute) decreases as altitude increases, because the air is less dense at higher altitudes. Given below is a table showing performance data for a certain single engine aircraft, giving its climb rate at various altitudes, where c(h)c(h) denotes the climb rate of the airplane at an altitude hh.

Let a new function called m(h)m(h)…

2.5

Exercise 14

In Chapter, we showed that for an object moving along a straight line with position function s(t)s(t), the object's “average velocity on the interval [a,b][a,b] ” is given by .

More recently in Chapter, we found that for an object moving along a straight line with velocity function v(t)v(t), the object's “average value of its velocity function on [a,b][a,b] ” is .

Are the “average velocity on the interval [a,b][a,b] ” and the “average valu…

2.5

Exercise 15

In Table in Activity, we noted that for x>0x \gt 0, an antiderivative of f(x)=1xf(x) = \frac{1}{x} is F(x)=ln⁡(x)F(x) = \ln(x). Here we observe that a key difference between f(x)f(x) and F(x)F(x) is that ff is defined for all x≠0x \ne 0, while FF is only defined for x>0x \gt 0, and see how we can actually define an antiderivative of ff for all values of xx.

  1. Suppose that x<0x \lt 0, and let G(x)=ln⁡(−x)G(x) = \ln(-x). Compute G′(x)G'(x).

  2. Explain why GG is an antiderivative of ff for x<0x \lt 0.

  3. Let H(x)=ln⁡(∣x∣)H(x) = \ln(|x|), and recall that . Explain why H(x)=G(x)H(x) = G(x) for x<0x \lt 0 and H(x)=F(x)H(x) = F(x)…

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Adapted from Active Calculus © 2012–2025 Matthew Boelkins. Licensed under CC BY-SA 4.0. Source: Active Calculus. Imported at revision dc86ba3.