Linearity of integration. For a constant k and integrable functions f1,f2,…:
∫kf(x)dx=k∫f(x)dx,∫(f1(x)±f2(x))dx=∫f1(x)dx±∫f2(x)dx.
Combined and extended: ∫(k1f1±k2f2±⋯±knfn)dx=k1∫f1dx±⋯±kn∫fndx — the integral of a linear combination is the linear combination of the integrals.
Simple applications. Integration recovers a function from its rate of change. If the derivative dxdy=f′(x) is known, integrating gives y=f(x)+c, and an initial condition fixes c. In kinematics, with the sign conventions of motion:
- acceleration a=dtdv, so v=∫adt;
- velocity v=dtds, so s=∫vdt.
Starting from a given acceleration (e.g. constant gravity or a braking retardation) and integrating twice — applying the initial velocity and initial position each time — yields velocity and then position as functions of time. The same rate→quantity idea models growth, decay, healing rates, marginal quantities, and similar problems (words like rate, growth, decay, marginal, change, varies signal a derivative).
Integrate first to get the general solution y=F(x)+c, then substitute the given data point to solve for c before answering any specific numerical question.