P4.6 - Integration
- Syllabus
- 2019
- Topic
- P4.6
- Level
- A2
Rotating the region between a non-negative curve y=f(x) and the x-axis through a full turn produces circular cross-sections. A slice of thickness dx has area πy2, so its volume is accumulated by integration.
V=π∫aby2dx
For y=x+1 on 0≤x≤2, V=π∫02(x+1)2dx=π[3(x+1)3]02=326π. Square the whole expression for y before integrating, and obtain the limits from the region's x-coordinates.
If x=x(t) and y=y(t), replace dx by x′(t)dt: V=π∫t1t2y(t)2x′(t)dt. For x=t2, y=t+1, 0≤t≤2, V=π∫02(t+1)2(2t)dt=368π. Choose the parameter limits in the direction of increasing x; if x′(t)<0 throughout, reverse the limits so the volume is positive.
This specification requires π∫y2dx, including parametric use, but not the separate π∫x2dy rule. Do not integrate y instead of y2, omit π, or leave a physical volume negative because the parameter runs backwards.
Integration by substitution reverses the chain rule; integration by parts reverses the product rule. First identify which structure is present, then transform every factor, differential and—when the integral is definite—limit consistently.
| Structure | Reverse rule | Check |
|---|---|---|
| a function and (a multiple of) its derivative | set u=g(x) and use du=g′(x)dx | the transformed integrand contains only u |
| a product whose factors simplify differently | ∫udv=uv−∫vdu | differentiating u should simplify it |
| repeated product, such as polynomial ×ex | apply parts more than once | stop when the polynomial disappears |
For ∫xx2+4dx, let u=x2+4, so du=2xdx. Then ∫xx2+4dx=21∫u1/2du=31(x2+4)3/2+C. For a definite integral, either change both limits to u-values or return to x before applying the original limits—never mix the two.
For ∫x2exdx, take u=x2 and dv=exdx. Two applications give ∫x2exdx=x2ex−2∫xexdx=ex(x2−2x+2)+C. Also, writing lnx as 1⋅lnx gives the required result ∫lnxdx=xlnx−x+C.
Do not change only part of an integrand during substitution, forget the transformed dx or limits, or lose the minus sign in the parts formula. A cyclic integral such as one containing exsinx may return after two applications of parts; collect that integral algebraically rather than continuing forever.
When a proper rational expression has factorised linear denominators, decompose it into simpler fractions before integrating. Match a constant numerator to each linear factor and an additional term for every repeated power.
| Integrand pattern | Antiderivative pattern |
|---|---|
| ax+bA | aAln∣ax+b∣ |
| (ax+b)nA, n>1 | use the power rule with the inner derivative factor |
| f(x)f′(x) | ln∣f(x)∣; e.g. ∫x2+5xdx=21ln(x2+5)+C |
For (x+1)(x+2)5x+1=x+1A+x+2B, matching numerators gives A=−4 and B=9. Hence ∫(x+1)(x+2)5x+1dx=−4ln∣x+1∣+9ln∣x+2∣+C. Differentiate the result to check both coefficients.
A repeated linear factor does not produce another logarithm: ∫(x−1)23dx=−x−13+C. Likewise, ∫(2x−1)42dx=−3(2x−1)31+C.
Make an improper rational expression proper before decomposing. Preserve absolute-value bars in logarithms unless the stated interval fixes the sign, and include the derivative of every linear denominator. Do not treat all denominator powers as logarithmic.
A first-order equation is separable when all y-dependence can be placed with dy and all x-dependence with dx. Integrating produces a family of curves—the general solution. An initial or boundary condition then selects a particular member.
dxdy=f(x)g(y)⟹∫g(y)1dy=∫f(x)dx
For dy/dx=2xy with y=0, separation gives y1dy=2xdx, so ln∣y∣=x2+C⟹y=Aex2. This non-zero family, together with the equilibrium solution y=0 lost when dividing by y, is the general solution.
If y(0)=3, then 3=Ae0, so the particular solution is y=3ex2. Check it by differentiating: dy/dx=6xex2=2x(3ex2)=2xy, and it satisfies the initial condition.
A reliable sequence is: separate with dy and dx visible; integrate both sides and include one arbitrary constant; simplify only when it helps; use the condition; state the requested form; differentiate to verify. Partial fractions or integration by parts may be needed after separation.
Do not treat dy/dx as an ordinary fraction without preserving the differential relationship. Before dividing by a factor involving y, test whether setting that factor to zero gives a constant solution. A general solution must retain an arbitrary constant; a particular solution must use the supplied condition.
For a parametric curve x=x(t), y=y(t), convert the Cartesian area element ydx using dx=x′(t)dt. The parameter values at the region's endpoints supply the limits; the curve does not need to be rearranged into y=f(x).
A=∫abydx=∫t1t2y(t)x′(t)dt
For x=t2, y=t+1, 0≤t≤2, x′(t)=2t and the curve lies above the x-axis. Thus A=∫02(t+1)(2t)dt=[32t3+t2]02=328.
| Region | Integrand in parameter form |
|---|---|
| between curve and x-axis | y(t)x′(t) |
| between y=h and the curve | [h−y(t)]x′(t) |
| curve crosses the axis or doubles back | split where the sign or x-direction changes, then add geometric pieces |
The integral is signed: reversed parameter limits or x′(t)<0 can make it negative even though geometric area is positive. Establish the endpoint parameter values and direction before integrating. Do not integrate x(t)y(t), and do not spend time sketching a curve from its parametric equations—the specification does not require that skill here.