PracticeVideosBlogFlashcards

20.3 Fundamental Theorem of Calculus, Net Signed Area & Geometric Applications

Key Takeaways

  • The definite integral ∫abf(x) dx\int_a^b f(x)\,dx is defined as the limit of Riemann sums and calculates the net signed area between y=f(x)y = f(x) and the xx-axis, treating regions above the axis as positive and regions below as negative.

  • The Fundamental Theorem of Calculus connects differentiation and integration: Part 1 asserts that ddx[∫axf(t) dt]=f(x)\frac{d}{dx}\left[\int_a^x f(t)\,dt\right] = f(x) (extended via Leibniz Rule and the Chain Rule), while Part 2 provides the evaluation formula ∫abf(x) dx=F(b)−F(a)\int_a^b f(x)\,dx = F(b) - F(a).

  • Total distance traveled by a moving particle is given by ∫t1t2∣v(t)∣ dt\int_{t_1}^{t_2} |v(t)|\,dt, which accounts for all directional reversals, in contrast to net displacement ∫t1t2v(t) dt=s(t2)−s(t1)\int_{t_1}^{t_2} v(t)\,dt = s(t_2) - s(t_1).

  • The area bounded between two curves y=f(x)y = f(x) and y=g(x)y = g(x) on [a,b][a, b] is given by ∫ab[f(x)−g(x)] dx\int_a^b [f(x) - g(x)]\,dx, where f(x)≥g(x)f(x) \ge g(x), requiring partitioning at intersection points if the curves cross.

  • Volumes of solids of revolution are evaluated using the Disk Method V=π∫ab[R(x)]2 dxV = \pi \int_a^b [R(x)]^2\,dx when the region is flush against the axis of revolution, and the Washer Method V=π∫ab([R(x)]2−[r(x)]2) dxV = \pi \int_a^b \left([R(x)]^2 - [r(x)]^2\right)\,dx when an interior cavity exists.

Last updated: September 2026

20.3 Fundamental Theorem of Calculus, Net Signed Area & Geometric Applications

Riemann Sums, Partitions & The Definite Integral

The definite integral formalizes the process of continuous accumulation. Let ff be a function defined on a closed bounded interval [a,b][a, b]. A partition PP divides [a,b][a, b] into nn subintervals by choosing points a=x0<x1<x2<⋯<xn=ba = x_0 < x_1 < x_2 < \dots < x_n = b. The length of the kk-th subinterval is Δxk=xk−xk−1\Delta x_k = x_k - x_{k-1}, and the norm of the partition, denoted ∥P∥\|P\|, is the maximum subinterval width: ∥P∥=max⁡1≤k≤nΔxk\|P\| = \max_{1 \le k \le n} \Delta x_k.

Choosing an arbitrary sample point xk∗∈[xk−1,xk]x_k^* \in [x_{k-1}, x_k] within each subinterval, the Riemann sum of ff associated with partition PP is:

Rn=∑k=1nf(xk∗)ΔxkR_n = \sum_{k=1}^n f(x_k^*) \Delta x_k

If ff is continuous on [a,b][a, b] (or piecewise continuous with finitely many jump discontinuities), the limit of Riemann sums as ∥P∥→0\|P\| \to 0 (n→∞n \to \infty) exists and is independent of the choice of partition or sample points. This limit defines the definite integral:

∫abf(x) dx=lim⁡∥P∥→0∑k=1nf(xk∗)Δxk\int_a^b f(x)\,dx = \lim_{\|P\| \to 0} \sum_{k=1}^n f(x_k^*) \Delta x_k

where aa is the lower limit of integration and bb is the upper limit of integration.


Net Signed Area vs. Total Geometric Area

Geometrically, the definite integral computes the net signed area bounded between the curve y=f(x)y = f(x) and the xx-axis over [a,b][a, b]:

  • Regions where f(x)≥0f(x) \ge 0 lie above the xx-axis and contribute positively to the integral: Aabove>0A_{\text{above}} > 0.
  • Regions where f(x)≤0f(x) \le 0 lie below the xx-axis and contribute negatively to the integral: Abelow<0A_{\text{below}} < 0.
∫abf(x) dx=Aabove−Abelow\int_a^b f(x)\,dx = A_{\text{above}} - A_{\text{below}}

If the objective is to find the total geometric area enclosed between the curve and the xx-axis, all area contributions must be taken as positive values. This requires integrating the absolute value of the function:

Total Area=∫ab∣f(x)∣ dx\text{Total Area} = \int_a^b |f(x)|\,dx

To evaluate this manually, one must find all real roots where f(x)=0f(x) = 0 on [a,b][a, b], partition the integral across these roots, and negate subintegrals where f(x)<0f(x) < 0.


The Fundamental Theorem of Calculus

The Fundamental Theorem of Calculus (FTC) creates the profound bridge between differential calculus and integral calculus, demonstrating that differentiation and integration are inverse processes.

Part 1: Accumulation Functions & Differentiation

If ff is continuous on [a,b][a, b], the accumulation function defined by:

g(x)=∫axf(t) dtfor a≤x≤bg(x) = \int_a^x f(t)\,dt \quad \text{for } a \le x \le b

is continuous on [a,b][a, b], differentiable on the open interval (a,b)(a, b), and its derivative is simply the integrand evaluated at xx:

g′(x)=ddx[∫axf(t) dt]=f(x)g'(x) = \frac{d}{dx}\left[\int_a^x f(t)\,dt\right] = f(x)

When the limits of integration are functions of xx, applying the Chain Rule produces the Extended Leibniz Rule:

ddx[∫v(x)u(x)f(t) dt]=f(u(x))⋅u′(x)−f(v(x))⋅v′(x)\frac{d}{dx}\left[\int_{v(x)}^{u(x)} f(t)\,dt\right] = f(u(x)) \cdot u'(x) - f(v(x)) \cdot v'(x)

Part 2: The Evaluation Theorem

If ff is continuous on [a,b][a, b] and FF is any antiderivative of ff on [a,b][a, b] such that F′(x)=f(x)F'(x) = f(x), then:

∫abf(x) dx=F(b)−F(a)=[F(x)]ab\int_a^b f(x)\,dx = F(b) - F(a) = \left[ F(x) \right]_a^b

Part 2 eliminates the need to compute complex limits of Riemann sums, allowing exact calculation of definite integrals via algebraic antiderivatives.


Algebraic & Structural Properties of Definite Integrals

Definite integrals satisfy fundamental operational rules:

  1. Reversal of Bounds: ∫baf(x) dx=−∫abf(x) dx\int_b^a f(x)\,dx = -\int_a^b f(x)\,dx.
  2. Zero Width Interval: ∫aaf(x) dx=0\int_a^a f(x)\,dx = 0.
  3. Linearity: ∫ab[c1f(x)+c2g(x)] dx=c1∫abf(x) dx+c2∫abg(x) dx\int_a^b [c_1 f(x) + c_2 g(x)]\,dx = c_1 \int_a^b f(x)\,dx + c_2 \int_a^b g(x)\,dx.
  4. Interval Additivity: For any three numbers a,b,ca, b, c: ∫abf(x) dx+∫bcf(x) dx=∫acf(x) dx\int_a^b f(x)\,dx + \int_b^c f(x)\,dx = \int_a^c f(x)\,dx.
  5. Comparison Properties: If f(x)≥g(x)f(x) \ge g(x) for all x∈[a,b]x \in [a, b], then ∫abf(x) dx≥∫abg(x) dx\int_a^b f(x)\,dx \ge \int_a^b g(x)\,dx.
  6. Symmetry Properties:
    • If ff is an even function (f(−x)=f(x)f(-x) = f(x)): ∫−aaf(x) dx=2∫0af(x) dx\int_{-a}^a f(x)\,dx = 2 \int_0^a f(x)\,dx.
    • If ff is an odd function (f(−x)=−f(x)f(-x) = -f(x)): ∫−aaf(x) dx=0\int_{-a}^a f(x)\,dx = 0.

Definite Integral Properties & Geometric Volume Formulas

Concept / TechniqueMathematical FormulaConditions & Geometric Description
FTC Part 1 (Leibniz Rule)ddx[∫v(x)u(x)f(t) dt]=f(u(x))u′(x)−f(v(x))v′(x)\frac{d}{dx}\left[\int_{v(x)}^{u(x)} f(t)\,dt\right] = f(u(x))u'(x) - f(v(x))v'(x)Differentiable boundary functions u(x),v(x)u(x), v(x)
FTC Part 2 (Evaluation)∫abf(x) dx=F(b)−F(a)\int_a^b f(x)\,dx = F(b) - F(a)F′(x)=f(x)F'(x) = f(x) continuous on [a,b][a, b]
Net DisplacementΔs=∫t1t2v(t) dt=s(t2)−s(t1)\Delta s = \int_{t_1}^{t_2} v(t)\,dt = s(t_2) - s(t_1)Change in position; signs can cancel
Total DistanceDtotal=∫t1t2∣v(t)∣ dtD_{\text{total}} = \int_{t_1}^{t_2} \vert v(t)\vert\,dtCumulative path length; always non-negative
Area Between Curves (in xx)A=∫ab[ftop(x)−gbottom(x)] dxA = \int_a^b [f_{\text{top}}(x) - g_{\text{bottom}}(x)]\,dxf(x)≥g(x)f(x) \ge g(x) over [a,b][a, b]
Area Between Curves (in yy)A=∫cd[fright(y)−gleft(y)] dyA = \int_c^d [f_{\text{right}}(y) - g_{\text{left}}(y)]\,dyf(y)≥g(y)f(y) \ge g(y) over [c,d][c, d]
Disk Method (about xx-axis)V=π∫ab[R(x)]2 dxV = \pi \int_a^b [R(x)]^2\,dxSolid cross-section flush against axis
Disk Method (about yy-axis)V=π∫cd[R(y)]2 dyV = \pi \int_c^d [R(y)]^2\,dyHorizontal radius function R(y)R(y) flush to axis
Washer Method (horizontal axis)V=π∫ab([R(x)]2−[r(x)]2) dxV = \pi \int_a^b \left([R(x)]^2 - [r(x)]^2\right)\,dxOuter radius R(x)R(x), inner cavity radius r(x)r(x)
Washer Method (vertical axis)V=π∫cd([R(y)]2−[r(y)]2) dyV = \pi \int_c^d \left([R(y)]^2 - [r(y)]^2\right)\,dyOuter radius R(y)R(y), inner cavity radius r(y)r(y)

Kinematics: Net Displacement vs. Total Distance

In kinematics, the distinction between signed accumulation and absolute accumulation is critical:

  • Net Displacement: The net change in position over time interval [t1,t2][t_1, t_2] is given by ∫t1t2v(t) dt=s(t2)−s(t1)\int_{t_1}^{t_2} v(t)\,dt = s(t_2) - s(t_1). Positive velocity (forward motion) and negative velocity (backward motion) cancel out algebraically.
  • Total Distance Traveled: The actual length of the path traversed is given by ∫t1t2∣v(t)∣ dt\int_{t_1}^{t_2} |v(t)|\,dt. Because distance is cumulative, intervals of negative velocity must be integrated with negated signs so all contributions are positive.

Planar Area Between Curves

To calculate the area of a bounded region enclosed between two curves y=f(x)y = f(x) and y=g(x)y = g(x):

  1. Find intersection points by setting f(x)=g(x)f(x) = g(x) and solving for xx. These roots establish the integration bounds [a,b][a, b].
  2. Determine which curve is the upper boundary (ftopf_{\text{top}}) and which is the lower boundary (gbottomg_{\text{bottom}}) on [a,b][a, b] by testing an interior test value.
  3. Integrate the difference: A=∫ab[ftop(x)−gbottom(x)] dxA = \int_a^b [f_{\text{top}}(x) - g_{\text{bottom}}(x)]\,dx

When boundaries are expressed more naturally as functions of yy, integrate horizontally from the left boundary to the right boundary:

A=∫cd[fright(y)−gleft(y)] dyA = \int_c^d [f_{\text{right}}(y) - g_{\text{left}}(y)]\,dy

Volumes of Solids of Revolution: Disk & Washer Methods

When a two-dimensional planar region is revolved 360∘360^\circ around an axis of rotation, it sweeps out a three-dimensional solid of revolution.

The Disk Method

If the revolving region is flush against the axis of rotation, perpendicular cross-sections are solid circular disks with area A=πR2A = \pi R^2. The volume is obtained by integrating cross-sectional circular disks:

  • Revolved about the horizontal axis y=ky = k: V=π∫ab[R(x)]2 dxV = \pi \int_a^b [R(x)]^2\,dx, where R(x)=∣f(x)−k∣R(x) = |f(x) - k|.
  • Revolved about the vertical axis x=hx = h: V=π∫cd[R(y)]2 dyV = \pi \int_c^d [R(y)]^2\,dy, where R(y)=∣g(y)−h∣R(y) = |g(y) - h|.

The Washer Method

If the revolving region has an open space or cavity between itself and the axis of rotation, perpendicular cross-sections are circular washers (annuli). The area of a washer cross-section is A=πRouter2−πrinner2=π(R2−r2)A = \pi R_{\text{outer}}^2 - \pi r_{\text{inner}}^2 = \pi (R^2 - r^2):

  • Revolved about the xx-axis: V=π∫ab([R(x)]2−[r(x)]2) dxV = \pi \int_a^b \left([R(x)]^2 - [r(x)]^2\right)\,dx
  • Revolved about the yy-axis: V=π∫cd([R(y)]2−[r(y)]2) dyV = \pi \int_c^d \left([R(y)]^2 - [r(y)]^2\right)\,dy

Worked Exemplar: Area Between Curves & Solid of Revolution

Problem:

  1. Determine the exact area of the planar region bounded between the parabola y=x2y = x^2 and the line y=2x+3y = 2x + 3.
  2. Compute the volume of the solid generated by revolving the region bounded by y=xy = \sqrt{x}, the horizontal line y=0y = 0 (xx-axis), and the vertical line x=4x = 4 around the xx-axis.

Step 1: Find Intersection Points for Area. Set the two equations equal to determine intersection points:

x2=2x+3  ⟹  x2−2x−3=0  ⟹  (x−3)(x+1)=0x^2 = 2x + 3 \implies x^2 - 2x - 3 = 0 \implies (x - 3)(x + 1) = 0

The integration bounds are x=−1x = -1 and x=3x = 3.

Step 2: Establish Boundary Orientation. Test x=0∈(−1,3)x = 0 \in (-1, 3): line value is 2(0)+3=32(0) + 3 = 3, parabola value is 02=00^2 = 0. Because 3>03 > 0, the line y=2x+3y = 2x + 3 is the upper boundary and the parabola y=x2y = x^2 is the lower boundary across the entire interval [−1,3][-1, 3].

Step 3: Integrate to Evaluate Enclosed Area. Apply the area formula:

A=∫−13[(2x+3)−x2] dx=∫−13(−x2+2x+3) dxA = \int_{-1}^3 \left[(2x + 3) - x^2\right]\,dx = \int_{-1}^3 (-x^2 + 2x + 3)\,dx

Find the antiderivative and evaluate at bounds:

A=[−x33+x2+3x]−13A = \left[ -\frac{x^3}{3} + x^2 + 3x \right]_{-1}^3

Evaluate at upper bound x=3x = 3:

(−273+(3)2+3(3))=−9+9+9=9\left(-\frac{27}{3} + (3)^2 + 3(3)\right) = -9 + 9 + 9 = 9

Evaluate at lower bound x=−1x = -1:

(−(−1)33+(−1)2+3(−1))=13+1−3=−53\left(-\frac{(-1)^3}{3} + (-1)^2 + 3(-1)\right) = \frac{1}{3} + 1 - 3 = -\frac{5}{3}

Subtract the evaluated bounds:

A=9−(−53)=273+53=323A = 9 - \left(-\frac{5}{3}\right) = \frac{27}{3} + \frac{5}{3} = \frac{32}{3}

Step 4: Formulate Volume of Solid of Revolution. For the region bounded by y=xy = \sqrt{x}, y=0y = 0, and x=4x = 4 revolved about the xx-axis:

  • The axis of revolution is the xx-axis (y=0y = 0).
  • The region is flush against the xx-axis from x=0x = 0 to x=4x = 4.
  • The radius of each cross-sectional disk is R(x)=x−0=xR(x) = \sqrt{x} - 0 = \sqrt{x}.
  • Cross-sectional area is A(x)=π[R(x)]2=π(x)2=πxA(x) = \pi [R(x)]^2 = \pi (\sqrt{x})^2 = \pi x.

Step 5: Integrate for Volume via the Disk Method. Set up and evaluate the definite integral:

V=π∫04x dx=π[x22]04=π(422−0)=π(162)=8πV = \pi \int_0^4 x\,dx = \pi \left[ \frac{x^2}{2} \right]_0^4 = \pi \left( \frac{4^2}{2} - 0 \right) = \pi \left(\frac{16}{2}\right) = 8\pi

The exact volume of the paraboloid solid is 8π cubic units8\pi\text{ cubic units}.

Test Your Knowledge

If F(x) = integral from 2 to x^3 of sqrt(t^2 + 7) dt, what is the exact value of the derivative F'(x) evaluated at x = 2?

A

12 * sqrt(71)

B

sqrt(71)

C

24 * sqrt(71)

D

12 * sqrt(11)

Test Your Knowledge

A particle moves along a straight coordinate axis with velocity v(t) = 3t^2 - 12 meters per second for 0 <= t <= 3. What are the particle's net displacement and total distance traveled over this time interval?

A

Net displacement = -9 meters; Total distance = 9 meters

B

Net displacement = 23 meters; Total distance = 23 meters

C

Net displacement = -9 meters; Total distance = 23 meters

D

Net displacement = 16 meters; Total distance = 25 meters

Test Your Knowledge

What is the exact area of the planar region completely enclosed between the parabola y = 6x - x^2 and the line y = 2x?

A

64/3

B

32/3

C

16

D

16/3

Test Your Knowledge

What is the volume of the solid generated by revolving the region bounded by y = sqrt(x), the horizontal line y = 2, and the y-axis (x = 0) about the y-axis?

A

16*pi / 3

B

8*pi

C

64*pi / 5

D

32*pi / 5

Sections you finish are checked off in the contents.