CALCULUS 1
##### Lesson 12: Techniques of Antidifferentiation 1.1. Topic 12.1: Antidifferentiation by Substitution and by Table of Integrals
Substitution method (u-substitution):
If you have an integral of the form \int f(g(x)) g'(x) dx , set u = g(x) so that du = g'(x) dx and the integral becomes \int f(u) du.
For definite integrals, change the limits: \inta^b f(x) dx = \int{u(a)}^{u(b)} f(x(u)) x'(u) du.
Table of Integrals: use standard antiderivatives to shortcut evaluation, e.g.
\int x^{n}\,dx = \frac{x^{n+1}}{n+1} + C, \quad n \neq -1
\int \frac{dx}{x} = \ln|x| + C
\int e^{ax}\,dx = \frac{1}{a} e^{ax} + C
\int \sin(bx)\,dx = -\frac{1}{b}\cos(bx) + C
\int \cos(bx)\,dx = \frac{1}{b}\sin(bx) + C
Significance: substitution reduces complex integrals to simpler forms; tables provide quick access to common antiderivatives.
Practical notes: recognize patterns that fit substitution; verify by differentiating the result.
Connections: links to the Fundamental Theorem of Calculus (FTC) since antiderivatives are the reverse of derivatives; underpins area calculations via definite integrals.
##### Lesson 13: Application of Antidifferentiation to Differential Equations 2.1. Topic 13.1: Separable Differential Equations
Form: dy/dt = g(t) h(y) (variables separated: put y terms on one side and t terms on the other).
Separation: dy/h(y) = g(t) dt
Integration: \int dy/h(y) = \int g(t) dt + C
Solve for y(t) using initial condition y(t0) = y0 if given; may require algebraic manipulation to isolate y.
Example template: if dy/dt = k y, then \int dy/y = \int k dt \rightarrow \ln|y| = kt + C \rightarrow y = C e^{kt}.
Practical use: models where a rate depends on both the current state and an independent variable (e.g., time).
Significance: shows how antidifferentiation techniques solve simple first-order ODEs.
##### Lesson 14: Application of Differential Equations in Life Sciences 3.1. Topic 14.1: Situational Problems Involving Growth and Decay Problems
Common model: exponential growth/decay dP/dt = r P, yielding P(t) = P_0 e^{r t}.
Acknowledge carrying capacity variants (e.g., logistic model) when appropriate: dP/dt = r P (1 - P/K).
Procedure: translate real-world situation into a differential equation, solve via separation or known forms, apply initial data, interpret results.
Relevance: helps in population biology, pharmacokinetics, cell growth, radioactive decay, and epidemiology.
##### Lesson 15: Riemann Sums and the Definite Integral 4.1. Topic 15.1: Approximation of Area using Riemann Sums
Partition [a,b] into n subintervals, choose sample points xi^* in each subinterval, \Delta xi = (b-a)/n (for equal partitions).
Riemann sum: Sn = \sum{i=1}^{n} f(xi^*) \Delta xi.. The definite integral is the limit: \inta^b f(x)\,dx = \lim{n\to\infty} S_n.
Important ideas: choice of sample points leads to left/right/midpoint sums; as n\to\infty, all converge to the same limit when f is integrable.
4.2. Topic 15.2: The Formal Definition of the Definite IntegralDefinition: \inta^b f(x)\,dx = \lim{\parallel P \parallel\to 0} \sum{i=1}^{n} f(xi^*) \Delta xi. where P is a partition of [a,b] with mesh \parallel P \parallel = \max \Delta xi.
Domains and integrability: f must be integrable on [a,b]; if f \geq 0, the integral represents area under the curve.
Significance: formal bridge between geometry (area) and analysis (limits); lays groundwork for FTC.
##### Lesson 16: The Fundamental Theorem of Calculus 5.1. Topic 16.1: Illustration of the Fundamental Theorem of Calculus
Part 1 (FTC1): If F is an antiderivative of f on [a,b], then \int_a^b f(x)\,dx = F(b) - F(a).
Consequence: differentiation and integration are inverse processes