Integration (Riemann sums, Fundamental Theorem of Calculus, u-substitution) Knowledge-Based Study

Math · Calculus · Math · Integrals

Math topic explanations on Integration (Riemann sums, Fundamental Theorem of Calculus, u-substitution).

Study notes

  1. The Area Problem and Partitions

    A fundamental goal of integral calculus is finding the exact area under a continuous curve f(x)f(x) over a closed interval [a,b][a, b], where f(x)≥0f(x) \ge 0. We approximate this region by dividing [a,b][a, b] into nn subintervals of equal width:

    Δx=b−an\Delta x = \frac{b - a}{n}

    The endpoints of these subintervals are given by xi=a+iΔxx_i = a + i\Delta x for i=0,1,2,…,ni = 0, 1, 2, \dots, n.

    Riemann Sum Definition

    By selecting a sample point xi∗x_i^* in each subinterval [xi−1,xi][x_{i-1}, x_i], we construct rectangles with base Δx\Delta x and height f(xi∗)f(x_i^*). The total approximate area is given by the Riemann sum:

    Sn=∑i=1nf(xi∗)ΔxS_n = \sum_{i=1}^{n} f(x_i^*) \Delta x

    Common choices for xi∗x_i^* include:

    • Left Riemann Sum: xi∗=xi−1x_i^* = x_{i-1}
    • Right Riemann Sum: xi∗=xix_i^* = x_i
    • Midpoint Rule: xi∗=xi−1+xi2x_i^* = \frac{x_{i-1} + x_i}{2}

    From Sums to Definite Integrals

    As the number of subdivisions nn approaches infinity (Δxo0\Delta x o 0), the approximation approaches the exact net signed area. If ff is continuous on [a,b][a, b], this limit exists and defines the definite integral:

    ∫abf(x) dx=lim⁡no∞∑i=1nf(xi∗)Δx\int_{a}^{b} f(x) \, dx = \lim_{n o \infty} \sum_{i=1}^{n} f(x_i^*) \Delta x

    Connecting Differentiation and Integration

    The Fundamental Theorem of Calculus (FTC) bridges the two central branches of calculus: differential calculus (slopes) and integral calculus (accumulated area).

    FTC Part 1: The Accumulation Function

    Let ff be a continuous function on [a,b][a, b]. The accumulation function defined by:

    g(x)=∫axf(t) dtg(x) = \int_{a}^{x} f(t) \, dt

    is continuous on [a,b][a, b], differentiable on (a,b)(a, b), and its derivative is:

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

    Chain Rule Extension: If the upper limit is a differentiable function u(x)u(x), then:

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

    FTC Part 2: The Evaluation Theorem

    If ff is continuous on [a,b][a, b] and FF is any antiderivative of ff 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) = \Big[ F(x) \Big]_{a}^{b}

    This allows us to evaluate definite integrals algebraically without computing limits of Riemann sums.

    The Chain Rule in Reverse

    Many integrands are composite functions multiplied by the derivative of the inner function. Integration by substitution reverses the differentiation chain rule:

    ddx[F(g(x))]=F′(g(x))⋅g′(x)=f(g(x))⋅g′(x)\frac{d}{dx} \Big[ F(g(x)) \Big] = F'(g(x)) \cdot g'(x) = f(g(x)) \cdot g'(x)

    Integrating both sides yields the substitution formula:

    ∫f(g(x))g′(x) dx=∫f(u) du=F(u)+C\int f(g(x)) g'(x) \, dx = \int f(u) \, du = F(u) + C

    Step-by-Step Procedure

    1. Identify the inner function: Choose u=g(x)u = g(x) such that its differential du=g′(x) dxdu = g'(x) \, dx appears in the integrand (up to a constant multiple).
    2. Compute the differential: Find du=g′(x) dxdu = g'(x) \, dx and solve for dxdx or directly rewrite g′(x) dxg'(x) \, dx as dudu.
    3. Rewrite entirely in terms of uu: Transform the entire integral into ∫f(u) du\int f(u) \, du. Ensure no terms with xx remain.
    4. Evaluate the integral: Find the antiderivative with respect to uu.
    5. Back-substitute: Replace uu with g(x)g(x) to express the final answer in terms of the original variable xx.

    Handling Limits of Integration

    When applying uu-substitution to a definite integral, there are two valid approaches:

    • Method 1 (Changing Limits): Transform the bounds x=ax = a and x=bx = b into u=g(a)u = g(a) and u=g(b)u = g(b):
      ∫abf(g(x))g′(x) dx=∫g(a)g(b)f(u) du\int_{a}^{b} f(g(x)) g'(x) \, dx = \int_{g(a)}^{g(b)} f(u) \, du
      This avoids back-substituting to xx at the end.
    • Method 2 (Back-Substitution): Evaluate the indefinite integral in terms of xx first, then apply the original bounds aa and bb.

    Worked Example 1: FTC Part 1 with Chain Rule

    Find ddx[∫1x3cos⁡(t) dt]\frac{d}{dx} \left[ \int_{1}^{x^3} \cos(t) \, dt \right].

    Using FTC Part 1 and the Chain Rule with u=x3u = x^3 and dudx=3x2\frac{du}{dx} = 3x^2:

    ddx[∫1x3cos⁡(t) dt]=cos⁡(x3)⋅ddx(x3)=3x2cos⁡(x3)\frac{d}{dx} \left[ \int_{1}^{x^3} \cos(t) \, dt \right] = \cos(x^3) \cdot \frac{d}{dx}(x^3) = 3x^2 \cos(x^3)

    Worked Example 2: Definite Integral via Substitution

    Evaluate ∫022xx2+1 dx\int_{0}^{2} 2x \sqrt{x^2 + 1} \, dx.

    Let u=x2+1u = x^2 + 1. Then du=2x dxdu = 2x \, dx.
    Update the limits of integration:

    • When x=0x = 0, u=02+1=1u = 0^2 + 1 = 1.
    • When x=2x = 2, u=22+1=5u = 2^2 + 1 = 5.

    Transform and evaluate:

    ∫15u du=∫15u1/2 du=[23u3/2]15=23(53/2−13/2)=23(55−1)\int_{1}^{5} \sqrt{u} \, du = \int_{1}^{5} u^{1/2} \, du = \left[ \frac{2}{3} u^{3/2} \right]_{1}^{5} = \frac{2}{3} \left( 5^{3/2} - 1^{3/2} \right) = \frac{2}{3}(5\sqrt{5} - 1)