Foundations to FrontierPart III: Calculus IBezhig

Module 17: The Fundamental Theorem, substitution, and area

8 exercises, each with a complete solution. 2 figures.

On this page
  1. A. Prerequisites and observable goals
  2. B. The central idea: accumulation and differentiation undo each other
  3. C. Two parts of the theorem, and their conditions
  4. D. Why an accumulation has the original rate
  5. E. A decision procedure
  6. F. Worked teaching examples
  7. Computing bridge: Accumulation and a loop invariant
  8. G. Independent practice
  9. H. Complete solutions: Module 17
  10. I. Retention and readiness

A. Prerequisites and observable goals#

Before

Antiderivatives, Riemann sums, chain rule, and algebraic sign charts.

After

Differentiate an accumulation function, evaluate a definite integral, change variables with correct bounds, and separate area from signed accumulation.

B. The central idea: accumulation and differentiation undo each other#

Let A(x)=∫axf(t) dtA(x)=\int_a^x f(t)\dd t. The input xx moves the upper boundary of an accumulation; tt is a dummy variable used inside the integral. Increasing xx by a small hh adds a thin strip. If the rate is continuous, that strip’s average height approaches f(x)f(x), so A′(x)=f(x)A'(x)=f(x). This connects the integral’s definition by sums with the practical evaluation of antiderivatives.

C. Two parts of the theorem, and their conditions#

These are convenient sufficient hypotheses for the Fundamental Theorem of Calculus (FTC). An integral of a discontinuous function may still exist, but differentiability of its accumulation needs examination at a discontinuity. [O1FTC]

The chain rule gives

 d dx∫ag(x)f(t) dt=f(g(x))g′(x),\frac{\dd}{\dd x}\int_a^{g(x)}f(t)\dd t=f(g(x))g'(x),

where the relevant continuity and differentiability hold. For two moving bounds, subtract the corresponding lower-bound term. The variable tt disappears when the integral has been differentiated.

Substitution is the chain rule reversed. If u=g(x)u=g(x), then the differential shorthand  du=g′(x) dx\dd u=g'(x)\dd x records a change in the variable of integration. For definite integrals,

∫abF(g(x))g′(x) dx=∫g(a)g(b)F(u) du\int_a^b F(g(x))g'(x)\dd x=\int_{g(a)}^{g(b)}F(u)\dd u

under appropriate continuity and differentiability assumptions. These oriented bounds already account for whether gg increases or decreases; this one-dimensional chain-rule substitution does not require gg to be globally one-to-one.

Geometric area between continuous graphs is ∫ab∣f−g∣ dx\int_a^b|f-g|\dd x. Solve for intersections and determine the upper graph on each subinterval. Integrating “top minus bottom” without checking their order can subtract away real area.

D. Why an accumulation has the original rate#

For small nonzero hh,

A(x+h)−A(x)h=1h∫xx+hf(t) dt.\frac{A(x+h)-A(x)}h=\frac1h\int_x^{x+h}f(t)\dd t.

This is the average height over a shrinking interval, with orientation handled by both the integral and hh. Continuity makes all nearby heights close to f(x)f(x), so the quotient tends to f(x)f(x). Then A−FA-F has derivative zero and is constant. Evaluating at aa gives A(x)=F(x)−F(a)A(x)=F(x)-F(a), and at bb yields the evaluation formula. This argument explains both parts rather than treating bracket notation as the definition of integration.

E. A decision procedure#

First decide whether the problem asks for a derivative of an integral, an integral value, or geometric area. For a derivative, apply FTC and then chain rules for moving bounds. For an integral, simplify algebraically and look for a nested expression whose derivative is also present. In substitution, write uu,  du\dd u, and either transformed bounds or a clear return to xx. Never use xx-bounds on a uu-antiderivative. For area, draw or compare the graphs before choosing a sign.

F. Worked teaching examples#

A moving endpoint. If A(x)=∫1x21+t3 dtA(x)=\int_1^{x^2}\sqrt{1+t^3}\dd t on a neighborhood where the integrand is real and continuous, then A′(x)=2x1+x6A'(x)=2x\sqrt{1+x^6}. There is no need to find an elementary antiderivative of the square root. FTC can answer a derivative question even when integration is difficult.

A definite substitution. Evaluate ∫012xex2 dx\int_0^1 2x e^{x^2}\dd x. Let u=x2u=x^2, so  du=2x dx\dd u=2x\dd x, and the bounds become 0,10,1. The integral is ∫01eu du=e−1\int_0^1e^u\dd u=e-1. The 2x2x has become part of  du\dd u; it is not an extra factor to retain.

Signed area versus total area. For f(x)=x−1f(x)=x-1 on [0,3][0,3], the triangular portion below the axis has area 1/21/2 and the portion above has area 22. Thus the integral is −1/2+2=3/2-1/2+2=3/2, while geometric area is 1/2+2=5/21/2+2=5/2. The accumulation A(x)=x2/2−xA(x)=x^2/2-x initially decreases, reaches its minimum at x=1x=1, and then increases.

Exact rate f(x)=x−1f(x)=x-1 on [0,3][0,3]. Shaded portions contribute with opposite signs to the integral. The accumulation decreases while this rate is negative, even though the rate itself is increasing.
Exact accumulation graph for A(x)=∫0x(t−1) dtA(x)=\int_0^x(t-1)\dd t. Compare with the signed-area diagram: AA decreases while the integrand is negative, reaches its minimum at x=1x=1, and returns to zero at x=2x=2 when positive and negative contributions balance.

Computing bridge: Accumulation and a loop invariant#

A program approximating total distance from sampled velocity might maintain Sk=∑i=0k−1v(ti)ΔtS_k=\sum_{i=0}^{k-1}v(t_i)\Delta t. Its loop invariant is that the accumulator equals the contributions processed so far; its physical units are velocity times time. The program can satisfy that invariant perfectly while its approximation is poor because the sampling is coarse or the velocity model is wrong. Calculus separates the exact integral from this finite sum, and J04 separates implementation verification from model validation.

G. Independent practice#

F foundation C standard course work T transfer S optional stretch L runnable lab or project. Attempt the complete set before opening its solutions.

M17.01FSolution

Evaluate ∫−12(3x2−2x) dx\int_{-1}^2(3x^2-2x)\dd x.

M17.02CSolution

Differentiate A(x)=∫0x3cos⁡(t2) dtA(x)=\int_0^{x^3}\cos(t^2)\dd t.

M17.03CSolution

Differentiate B(x)=∫x2x(1+t2) dtB(x)=\int_x^{2x}(1+t^2)\dd t in two ways.

M17.04CSolution

Evaluate ∫xx2+4 dx\int x\sqrt{x^2+4}\dd x and check by differentiation.

M17.05TSolution

Evaluate ∫0π/2sin⁡x ecos⁡x dx\int_0^{\pi/2}\sin x\,e^{\cos x}\dd x using transformed bounds.

M17.06CSolution

Find the geometric area between y=2xy=2x and y=x2y=x^2.

M17.07TSolution

For v(t)=t2−4v(t)=t^2-4 m/s on [0,3][0,3], find displacement, total distance, and average velocity.

M17.08SSolution

Let A(x)=∫0x∣t∣ dtA(x)=\int_0^x|t|\dd t. Find a piecewise formula, determine A′(0)A'(0), and decide whether A′′(0)A''(0) exists.

Optional small hints

For M17.03, moving lower bounds subtract. For M17.05, increasing xx makes u=cos⁡xu=\cos x decrease. For M17.08, an integral from zero to a negative endpoint has reversed orientation.

H. Complete solutions: Module 17#

Compare the first step where your work differs. A corrected answer is not yet an independent success.

M17.01Show solution

Upper evaluation minus lower evaluation

An antiderivative is F(x)=x3−x2F(x)=x^3-x^2. Thus F(2)=4F(2)=4 and F(−1)=−2F(-1)=-2. The integral is 4−(−2)=64-(-2)=\boxed6. Subtracting the entire lower evaluation prevents a common sign error. No arbitrary constant is needed in a definite numerical answer.

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M17.02Show solution

Use FTC before trying to integrate

The integrand is continuous everywhere and the upper endpoint is differentiable. FTC plus the chain rule gives

A′(x)=cos⁡((x3)2) 3x2=3x2cos⁡(x6).\boxed{A'(x)=\cos((x^3)^2)\,3x^2=3x^2\cos(x^6)}.

Replacing tt by xx rather than by the actual endpoint x3x^3 would lose the composition.

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M17.03Show solution

Two moving boundaries

Directly, B′=2[1+(2x)2]−[1+x2]=1+7x2B'=2[1+(2x)^2]-[1+x^2]=\boxed{1+7x^2}. Alternatively, B=[t+t3/3]x2x=x+7x3/3B=[t+t^3/3]_x^{2x}=x+7x^3/3, whose derivative is the same. Both computations remain valid for negative xx, where the integral’s orientation is reversed automatically.

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M17.04Show solution

A nested expression with its derivative nearby

Let u=x2+4u=x^2+4. Then  du=2x dx\dd u=2x\dd x, so x dx= du/2x\dd x=\dd u/2. The integral becomes 12∫u1/2 du=u3/2/3+C\tfrac12\int u^{1/2}\dd u=u^{3/2}/3+C. Return to the original variable:

(x2+4)3/23+C.\boxed{\frac{(x^2+4)^{3/2}}3+C}.

Differentiating yields (1/3)(3/2)(x2+4)1/2(2x)=xx2+4(1/3)(3/2)(x^2+4)^{1/2}(2x)=x\sqrt{x^2+4}. The radicand is positive for every real xx.

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M17.05Show solution

Let the transformed bounds carry the reversal

Choose u=cos⁡xu=\cos x, so  du=−sin⁡x dx\dd u=-\sin x\dd x. At x=0x=0, u=1u=1; at x=π/2x=\pi/2, u=0u=0. Therefore the integral is −∫10eu du=∫01eu du=e−1-\int_1^0e^u\dd u=\int_0^1e^u\dd u=\boxed{e-1}. The answer is positive, agreeing with a nonnegative original integrand.

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M17.06Show solution

Find where the graphs enclose the region

Solve 2x=x22x=x^2: the intersections have inputs 0,20,2. On (0,2)(0,2), 2x−x2=x(2−x)>02x-x^2=x(2-x)>0, so the line is above the parabola. Thus

A=∫02(2x−x2) dx=[x2−x3/3]02=4/3A=\int_0^2(2x-x^2)\dd x=[x^2-x^3/3]_0^2=\boxed{4/3}

in square units. The signed difference is already positive on this interval.

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M17.07Show solution

Split distance where velocity changes sign

An antiderivative of velocity is F(t)=t3/3−4tF(t)=t^3/3-4t. Displacement is F(3)−F(0)=9−12=−3F(3)-F(0)=9-12=\boxed{-3} m, giving average velocity −3/3=−1-3/3=\boxed{-1} m/s. Velocity is negative on [0,2)[0,2) and positive on (2,3](2,3]. Since F(2)=−16/3F(2)=-16/3, distance is 16/3+[−3−(−16/3)]=23/316/3+[-3-(-16/3)]=\boxed{23/3} m. The direction change, not the zero of position, sets the split.

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M17.08Show solution

Integrating a corner smooths one level

For x≥0x\ge0, A=x2/2A=x^2/2. For x<0x<0, the integrand on [x,0][x,0] is −t-t, and reversing the bounds gives A=−x2/2A=-x^2/2. Hence A=x∣x∣/2A=x|x|/2. The quotient (A(h)−A(0))/h=∣h∣/2(A(h)-A(0))/h=|h|/2 tends to zero, so A′(0)=0A'(0)=0. More generally FTC gives A′=∣x∣A'=|x| because the integrand is continuous. Its derivative fails at zero, so A′′(0)A''(0) does not exist. Continuity of the rate guarantees one derivative of accumulation, not arbitrarily many.

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I. Retention and readiness#

Retrieve M16.04, M10.07, and M12.01. Explain why the dummy variable is not a free variable in the final answer. Advance when you can choose between FTC, substitution, and a sign-based area split without the method being named.