20.3 Fundamental Theorem of Calculus, Net Signed Area & Geometric Applications
Key Takeaways
- The definite integral $\int_a^b f(x)\,dx$ is defined as the limit of Riemann sums and calculates the net signed area between $y = f(x)$ and the $x$-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 $\frac{d}{dx}\left[\int_a^x f(t)\,dt\right] = f(x)$ (extended via Leibniz Rule and the Chain Rule), while Part 2 provides the evaluation formula $\int_a^b f(x)\,dx = F(b) - F(a)$.
- Total distance traveled by a moving particle is given by $\int_{t_1}^{t_2} |v(t)|\,dt$, which accounts for all directional reversals, in contrast to net displacement $\int_{t_1}^{t_2} v(t)\,dt = s(t_2) - s(t_1)$.
- The area bounded between two curves $y = f(x)$ and $y = g(x)$ on $[a, b]$ is given by $\int_a^b [f(x) - g(x)]\,dx$, where $f(x) \ge g(x)$, requiring partitioning at intersection points if the curves cross.
- Volumes of solids of revolution are evaluated using the Disk Method $V = \pi \int_a^b [R(x)]^2\,dx$ when the region is flush against the axis of revolution, and the Washer Method $V = \pi \int_a^b \left([R(x)]^2 - [r(x)]^2\right)\,dx$ when an interior cavity exists.
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 $f$ be a function defined on a closed bounded interval $[a, b]$. A partition $P$ divides $[a, b]$ into $n$ subintervals by choosing points $a = x_0 < x_1 < x_2 < \dots < x_n = b$. The length of the $k$-th subinterval is $\Delta x_k = x_k - x_{k-1}$, and the norm of the partition, denoted $|P|$, is the maximum subinterval width: $|P| = \max_{1 \le k \le n} \Delta x_k$.
Choosing an arbitrary sample point $x_k^* \in [x_{k-1}, x_k]$ within each subinterval, the Riemann sum of $f$ associated with partition $P$ is:
If $f$ is continuous on $[a, b]$ (or piecewise continuous with finitely many jump discontinuities), the limit of Riemann sums as $|P| \to 0$ ($n \to \infty$) exists and is independent of the choice of partition or sample points. This limit defines the definite integral: where $a$ is the lower limit of integration and $b$ 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 $y = f(x)$ and the $x$-axis over $[a, b]$:
- Regions where $f(x) \ge 0$ lie above the $x$-axis and contribute positively to the integral: $A_{\text{above}} > 0$.
- Regions where $f(x) \le 0$ lie below the $x$-axis and contribute negatively to the integral: $A_{\text{below}} < 0$.
If the objective is to find the total geometric area enclosed between the curve and the $x$-axis, all area contributions must be taken as positive values. This requires integrating the absolute value of the function: To evaluate this manually, one must find all real roots where $f(x) = 0$ on $[a, b]$, partition the integral across these roots, and negate subintegrals where $f(x) < 0$.
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 $f$ is continuous on $[a, b]$, the accumulation function defined by: is continuous on $[a, b]$, differentiable on the open interval $(a, b)$, and its derivative is simply the integrand evaluated at $x$:
When the limits of integration are functions of $x$, applying the Chain Rule produces the Extended Leibniz Rule:
Part 2: The Evaluation Theorem
If $f$ is continuous on $[a, b]$ and $F$ is any antiderivative of $f$ on $[a, b]$ such that $F'(x) = f(x)$, then: 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:
- Reversal of Bounds: $\int_b^a f(x),dx = -\int_a^b f(x),dx$.
- Zero Width Interval: $\int_a^a f(x),dx = 0$.
- Linearity: $\int_a^b [c_1 f(x) + c_2 g(x)],dx = c_1 \int_a^b f(x),dx + c_2 \int_a^b g(x),dx$.
- Interval Additivity: For any three numbers $a, b, c$: $\int_a^b f(x),dx + \int_b^c f(x),dx = \int_a^c f(x),dx$.
- Comparison Properties: If $f(x) \ge g(x)$ for all $x \in [a, b]$, then $\int_a^b f(x),dx \ge \int_a^b g(x),dx$.
- Symmetry Properties:
- If $f$ is an even function ($f(-x) = f(x)$): $\int_{-a}^a f(x),dx = 2 \int_0^a f(x),dx$.
- If $f$ is an odd function ($f(-x) = -f(x)$): $\int_{-a}^a f(x),dx = 0$.
Definite Integral Properties & Geometric Volume Formulas
| Concept / Technique | Mathematical Formula | Conditions & Geometric Description |
|---|---|---|
| FTC Part 1 (Leibniz Rule) | $\frac{d}{dx}\left[\int_{v(x)}^{u(x)} f(t),dt\right] = f(u(x))u'(x) - f(v(x))v'(x)$ | Differentiable boundary functions $u(x), v(x)$ |
| FTC Part 2 (Evaluation) | $\int_a^b f(x),dx = F(b) - F(a)$ | $F'(x) = f(x)$ continuous on $[a, b]$ |
| Net Displacement | $\Delta s = \int_{t_1}^{t_2} v(t),dt = s(t_2) - s(t_1)$ | Change in position; signs can cancel |
| Total Distance | $D_{\text{total}} = \int_{t_1}^{t_2} |v(t)|,dt$ | Cumulative path length; always non-negative |
| Area Between Curves (in $x$) | $A = \int_a^b [f_{\text{top}}(x) - g_{\text{bottom}}(x)],dx$ | $f(x) \ge g(x)$ over $[a, b]$ |
| Area Between Curves (in $y$) | $A = \int_c^d [f_{\text{right}}(y) - g_{\text{left}}(y)],dy$ | $f(y) \ge g(y)$ over $[c, d]$ |
| Disk Method (about $x$-axis) | $V = \pi \int_a^b [R(x)]^2,dx$ | Solid cross-section flush against axis |
| Disk Method (about $y$-axis) | $V = \pi \int_c^d [R(y)]^2,dy$ | Horizontal radius function $R(y)$ flush to axis |
| Washer Method (horizontal axis) | $V = \pi \int_a^b \left([R(x)]^2 - [r(x)]^2\right),dx$ | Outer radius $R(x)$, inner cavity radius $r(x)$ |
| Washer Method (vertical axis) | $V = \pi \int_c^d \left([R(y)]^2 - [r(y)]^2\right),dy$ | Outer radius $R(y)$, inner cavity radius $r(y)$ |
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 $[t_1, t_2]$ is given by $\int_{t_1}^{t_2} v(t),dt = s(t_2) - s(t_1)$. 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 $\int_{t_1}^{t_2} |v(t)|,dt$. 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 $y = f(x)$ and $y = g(x)$:
- Find intersection points by setting $f(x) = g(x)$ and solving for $x$. These roots establish the integration bounds $[a, b]$.
- Determine which curve is the upper boundary ($f_{\text{top}}$) and which is the lower boundary ($g_{\text{bottom}}$) on $[a, b]$ by testing an interior test value.
- Integrate the difference:
When boundaries are expressed more naturally as functions of $y$, integrate horizontally from the left boundary to the right boundary:
Volumes of Solids of Revolution: Disk & Washer Methods
When a two-dimensional planar region is revolved $360^\circ$ 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 $A = \pi R^2$. The volume is obtained by integrating cross-sectional circular disks:
- Revolved about the horizontal axis $y = k$: $V = \pi \int_a^b [R(x)]^2,dx$, where $R(x) = |f(x) - k|$.
- Revolved about the vertical axis $x = h$: $V = \pi \int_c^d [R(y)]^2,dy$, where $R(y) = |g(y) - h|$.
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 $A = \pi R_{\text{outer}}^2 - \pi r_{\text{inner}}^2 = \pi (R^2 - r^2)$:
- Revolved about the $x$-axis: $V = \pi \int_a^b \left([R(x)]^2 - [r(x)]^2\right),dx$
- Revolved about the $y$-axis: $V = \pi \int_c^d \left([R(y)]^2 - [r(y)]^2\right),dy$
Worked Exemplar: Area Between Curves & Solid of Revolution
Problem:
- Determine the exact area of the planar region bounded between the parabola $y = x^2$ and the line $y = 2x + 3$.
- Compute the volume of the solid generated by revolving the region bounded by $y = \sqrt{x}$, the horizontal line $y = 0$ ($x$-axis), and the vertical line $x = 4$ around the $x$-axis.
Step 1: Find Intersection Points for Area. Set the two equations equal to determine intersection points: The integration bounds are $x = -1$ and $x = 3$.
Step 2: Establish Boundary Orientation. Test $x = 0 \in (-1, 3)$: line value is $2(0) + 3 = 3$, parabola value is $0^2 = 0$. Because $3 > 0$, the line $y = 2x + 3$ is the upper boundary and the parabola $y = x^2$ is the lower boundary across the entire interval $[-1, 3]$.
Step 3: Integrate to Evaluate Enclosed Area. Apply the area formula: Find the antiderivative and evaluate at bounds: Evaluate at upper bound $x = 3$: Evaluate at lower bound $x = -1$: Subtract the evaluated bounds:
Step 4: Formulate Volume of Solid of Revolution. For the region bounded by $y = \sqrt{x}$, $y = 0$, and $x = 4$ revolved about the $x$-axis:
- The axis of revolution is the $x$-axis ($y = 0$).
- The region is flush against the $x$-axis from $x = 0$ to $x = 4$.
- The radius of each cross-sectional disk is $R(x) = \sqrt{x} - 0 = \sqrt{x}$.
- Cross-sectional area is $A(x) = \pi [R(x)]^2 = \pi (\sqrt{x})^2 = \pi x$.
Step 5: Integrate for Volume via the Disk Method. Set up and evaluate the definite integral: The exact volume of the paraboloid solid is $8\pi\text{ cubic units}$.
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 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?
What is the exact area of the planar region completely enclosed between the parabola y = 6x - x^2 and the line y = 2x?
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?