When a function is defined implicitly (e.g., x2+y2=25), differentiate both sides with Respect to xTreating y as a function of x.
dxd[yn]=nyn−1dxdyThis is the chain rule applied to y(x)n: dxd[yn]=nyn−1⋅y"(x).
Example: Find dxdy for x2+y2=25.
2x+2ydxdy=0dxdy=−yxThis makes geometric sense: on the upper semicircle (y>0), increasing x decreases yGiving A negative slope. On the lower semicircle (y<0), the slope is positive.
Example: Find dxdy for x3+y3=6xy.
Differentiate implicitly:
3x2+3y2dxdy=6y+6xdxdy3y2dxdy−6xdxdy=6y−3x2dxdy(3y2−6x)=6y−3x2dxdy=3y2−6x6y−3x2=y2−2x2y−x2Example: Find the tangent to x2+y2+2x−4y=11 at the point (1,2).
Verify: 1+4+2−8=−1=11. The point is not on the curve. Let us find the gradient Function first:
2x+2ydxdy+2−4dxdy=0(2y−4)dxdy=−2x−2dxdy=2y−4−2x−2=y−2−x−1Second derivatives implicitly. Differentiate dxdy again with respect to xUsing The chain rule wherever y appears.
If x=f(t) and y=g(t) Then:
dxdy=dx/dtdy/dt=f′(t)g′(t)This follows from the chain rule: dxdy=dx/dtdy/dt.
Second Derivative:
dx2d2y=dxd(dxdy)=dx/dtdtd(dxdy)Example: A curve has parametric equations x=2cost, y=sin2t. Find dxdy at t=4π.
dtdx=−2sint,dtdy=2cos2tdxdy=−2sint2cos2t=−sintcos2tAt t=4π:
dxdy=−sin(π/4)cos(π/2)=−1/20=0Example: Find dx2d2y for x=t2, y=t3.
dxdy=2t3t2=23tdx2d2y=dx/dtd/dt(3t/2)=2t3/2=4t3dxd[arcsinx]=1−x21,∣x∣<1dxd[arccosx]=1−x2−1,∣x∣<1dxd[arctanx]=1+x21Proof that dxd[arctanx]=1+x21. Let y=arctanx So x=tany. Differentiating implicitly: 1=sec2y⋅dxdyGiving dxdy=sec2y1=1+tan2y1=1+x21.
Example: Differentiate f(x)=arcsin(3x).
F′(x)=1−(3x)21⋅3=1−9x23For functions of the form y=[f(x)]g(x)Take natural logarithms first:
lny=g(x)lnf(x)Then differentiate implicitly.
Example: Differentiate y=xx.
lny=xlnxy1dxdy=lnx+x⋅x1=lnx+1dxdy=y(lnx+1)=xx(lnx+1)Example: Differentiate y=xsinx.
lny=sinx⋅lnxy1dxdy=cosx⋅lnx+sinx⋅x1dxdy=xsinx(cosxlnx+xsinx)Related rates problems involve finding the rate of change of one quantity given the rate of change Of a related quantity.
Example: A ladder 5 m long leans against a wall. The bottom slides away at 0.5 m/s. How fast is The top sliding down when the bottom is 3 m from the wall?
Let x be the distance from the wall and y be the height. Then x2+y2=25.
Differentiate: 2xdtdx+2ydtdy=0.
When x=3: y=25−9=4.
2(3)(0.5) + 2(4)\frac{dy}{dt} = 0 \implies 3 + 8\frac{dy}{dt} = 0 \implies \frac{dy}{dt} = -\frac{3}{8} \mathrm{ m/s
∫udv=uv−∫vduProof. By the product rule: dxd[uv]=u′v+uv′ So uv′=dxd[uv]−u′v. Integrating both sides: ∫uv′dx=uv−∫u′vdx.
LIATE rule for choosing u (in order of priority): Logarithmic, Inverse trig, Algebraic, Trigonometric, Exponential. Choose u as the function that appears earliest in this list.
Example: Evaluate ∫xe2xdx.
Let u = x$$dv = e^{2x} dx. Then du = dx$$v = \dfrac{e^{2x}}{2}.
∫xe2xdx=x⋅2e2x−∫2e2xdx=2xe2x−4e2x+C=4e2x(2x−1)+CExample: Evaluate ∫x2cosxdx.
Let u = x^2$$dv = \cos x \, dx. Then du = 2x \, dx$$v = \sin x.
=x2sinx−∫2xsinxdxApply integration by parts again for ∫xsinxdx:
Let u = x$$dv = \sin x \, dx. Then du = dx$$v = -\cos x.
∫xsinxdx=−xcosx+∫cosxdx=−xcosx+sinxSo:
∫x2cosxdx=x2sinx−2(−xcosx+sinx)+C=x2sinx+2xcosx−2sinx+CSome integrals require integration by parts twice, then solving algebraically.
Example: Evaluate ∫excosxdx.
Let u = e^x$$dv = \cos x\,dx. Then du = e^x\,dx$$v = \sin x.
I=exsinx−∫exsinxdxApply parts again for ∫exsinxdx: u = e^x$$dv = \sin x\,dx.
∫exsinxdx=−excosx+∫excosxdx=−excosx+ISubstituting back:
I=exsinx−(−excosx+I)=exsinx+excosx−I2I=ex(sinx+cosx)I=2ex(sinx+cosx)+C\int f(g(x))g'(x) \, dx = \int f(u) \, du \quad \mathrm{where u = g(x)Example: Evaluate ∫x2+1xdx.
Let u=x2+1 So du=2xdxGiving 21du=xdx.
∫x2+1xdx=21∫udu=21ln∣u∣+C=21ln(x2+1)+CWhen using substitution in a definite integral, you must change the limits.
Example: Evaluate ∫01x2+12xdx.
Let u=x2+1. When x = 0$$u = 1. When x = 1$$u = 2.
∫01x2+12xdx=∫12udu=[lnu]12=ln2−ln1=ln2Rational functions can be decomposed using partial fractions to make them easier to integrate.
Example: Evaluate ∫(x+1)(x−2)2x+1dx.
(x+1)(x−2)2x+1=x+1A+x−2B2x+1=A(x−2)+B(x+1)x=−1: −2+1=A(−3) So A=31.
x=2: 4+1=B(3) So B=35.
∫(x+1)(x−2)2x+1dx=31∫x+1dx+35∫x−2dx=31ln∣x+1∣+35ln∣x−2∣+C∫tanxdx=−ln∣cosx∣+C=ln∣secx∣+C∫cotxdx=ln∣sinx∣+C∫secxdx=ln∣secx+tanx∣+CExample: Evaluate ∫tan2xdx.
∫tan2xdx=∫(sec2x−1)dx=tanx−x+CExample: Evaluate ∫sin2x+4cos2xdx.
Divide numerator and denominator by cos2x:
=∫tan2x+4sec2xdxLet u = \tan x$$du = \sec^2 x \, dx:
=∫u2+4du=21arctan(2u)+C=21arctan(2tanx)+CThe volume generated by rotating y=f(x) about the x-axis from x=a to x=b:
V=π∫ab[f(x)]2dxThe volume generated by rotating about the y-axis:
V=π∫cd[f−1(y)]2dyExample: Find the volume generated by rotating y=x about the x-axis from x=0 to x=4.
V=π∫04xdx=π[2x2]04=8π
Separable Equations: Equations of the form dxdy=f(x)g(y) can be solved by Separating variables:
∫g(y)dy=∫f(x)dxExample: Solve dxdy=yx with y(0)=2.
Ydy=xdx∫ydy=∫xdx2y2=2x2+CY2=x2+2CUsing y(0)=2: 4=0+2C So C=2.
Y2=x2+4Since y(0)=2>0: y=x2+4.
Equations of the form:
dxdy+P(x)y=Q(x)Integrating Factor: μ(x)=e∫P(x)dx
Multiply through by the integrating factor:
dxd[μy]=μQY=μ1∫μQdxWhy this works. We want to write the left side as the derivative of a product. If we multiply by μ:
μdxdy+μPy=μQThis is dxd[μy] provided μ′=μPI.e., μ=e∫Pdx.
Example: Solve dxdy+3y=6e−3x.
Integrating factor: μ=e∫3dx=e3x.
E3xdxdy+3e3xy=6dxd[e3xy]=6E3xy=6x+CY=e−3x(6x+C)Homogeneous equations with constant coefficients:
Adx2d2y+bdxdy+cy=0Try y=emx: the auxiliary equation is am2+bm+c=0.
Case 1: Two distinct real roots m1,m2:
Y=Aem1x+Bem2xCase 2: Repeated root m:
Y=(Ax+B)emxCase 3: Complex roots m=α±βi:
Y=eαx(Acosβx+Bsinβx)Why the complex case produces sines and cosines. If m=α+βi Then e(α+βi)x=eαx(cosβx+isinβx). Since the original DE has real Coefficients, both e(α+βi)x and e(α−βi)x are solutions. Their linear Combinations give eαxcosβx and eαxsinβx.
Example: Solve dx2d2y−5dxdy+6y=0.
Auxiliary equation: m2−5m+6=0 So (m−2)(m−3)=0Giving m=2,3.
Y=Ae2x+Be3xExample: Solve dx2d2y+4y=0.
Auxiliary equation: m2+4=0 So m=±2i.
Y=Acos2x+Bsin2xExample: Solve dx2d2y+6dxdy+9y=0.
Auxiliary equation: m2+6m+9=0 So (m+3)2=0Giving m=−3 (repeated).
Y=(Ax+B)e−3xAdx2d2y+bdxdy+cy=f(x)General Solution: y=yh+yp (complementary function + particular integral).
Method for finding yp: Guess the form of yp based on f(x).
| f(x) | Guess for yp |
|---|
| ekx | Cekx (if k is not a root) |
| kx+b | Ax+B |
| coskx or sinkx | Acoskx+Bsinkx |
Example: Solve dx2d2y−3dxdy+2y=4e3x.
Complementary function: m2−3m+2=0 So m=1,2.
Yh=Aex+Be2xFor the particular integral, try yp=Ce3x:
9Ce3x−9Ce3x+2Ce3x=4e3x2C=4⟹C=2Yp=2e3xGeneral solution: y=Aex+Be2x+2e3x.
The Maclaurin series expands a function as a power series about x=0:
F(x)=f(0)+f′(0)x+2!f′′(0)x2+3!f′′′(0)x3+⋯=n=0∑∞n!f(n)(0)xnEx=1+x+2!x2+3!x3+⋯sinx=x−3!x3+5!x5−⋯cosx=1−2!x2+4!x4−⋯ln(1+x)=x−2x2+3x3−4x4+⋯,∣x∣≤1,x=−1(1+x)n=1+nx+2!n(n−1)x2+3!n(n−1)(n−2)x3+⋯,∣x∣<1Example: Find the Maclaurin series for f(x)=e−x2 up to the term in x6.
Substitute −x2 into the series for eu:
E−x2=1+(−x2)+2!(−x2)2+3!(−x2)3+⋯=1−x2+2x4−6x6+⋯Limits: Maclaurin series can be used to evaluate limits that are indeterminate.
Example: Evaluate x→0limx2ex−1−x.
Ex−1−x=(1+x+2x2+⋯)−1−x=2x2+⋯x2ex−1−x=x22x2+⋯=21+⋯→21Integration of Series:
Example: Find ∫00.5e−x2dx to 4 decimal places.
E−x2≈1−x2+2x4−6x6∫00.5e−x2dx≈[x−3x3+10x5−42x7]00.5=0.5−30.125+100.03125−420.0078125=0.5−0.04167+0.003125−0.000186=0.46127
Calculus is the mathematics of change — differentiation finds the instantaneous rate of change (how fast something is happening right now), and integration finds the accumulation of change (how much has happened over time). The Fundamental Theorem of Calculus is the bridge between these two operations: they are inverses of each other, just as multiplication and division are inverses. Implicit differentiation is like working backwards from a recipe to find the ingredients: you know the result (the equation) and you work out how each variable contributes. The key insight is that calculus gives you exact answers about quantities that are constantly changing.
See the examples integrated throughout the sections above.
Forgetting the chain rule in implicit differentiation: When differentiating y3The result is 3y2dxdyNot 3y2.
Wrong choice of u in integration by parts: Follow the LIATE rule. Choosing algebraic functions as dv instead of u leads to more complicated integrals.
Missing the constant of integration: Always include +C for indefinite integrals.
Incorrect auxiliary equation: For dx2d2y+4y=0The auxiliary equation is m2+4=0Not m2+4m=0.
Domain restrictions in Maclaurin series: The series for ln(1+x) is valid for −1<x≤1Not all x.
Forgetting to change limits in definite substitution: When u=g(x)The new limits are u(a) and u(b)Not a and b.
Not checking that the particular integral guess works: If your guess for yp contains a term already in yhMultiply by x and try again.
Find dxdy for x3+xy2+y3=7.
Evaluate ∫x2e−xdx by parts.
Solve the differential equation dxdy=3y−22x+1 with y(0)=1.
Find the Maclaurin series for f(x)=cos(2x) up to the term in x6.
Solve dx2d2y+2dxdy+y=0.
A curve has parametric equations x = t^2$$y = t^3 - 3t. Find the coordinates of the stationary points.
Evaluate ∫011+x3dx by first finding the partial fraction decomposition.
Solve dxdy+x2y=x3 using an integrating factor.
Solve dx2d2y−4y=2e3x.
Find the volume of revolution when y=sinx is rotated about the x-axis from x=0 to x=π.
Evaluate ∫exsinxdx using cyclic integration by parts.
Use Maclaurin series to evaluate x→0limx21−cosx.
A[3_Calculus] --> B[Key Concepts]
A --> D[Practical Applications]
B --> E[Fundamental definitions]
D --> G[Real-world usage]
This topic covers the mathematical techniques and concepts related to further calculus, including key theorems, methods, and problem-solving approaches.
Key concepts include:
- differentiation from first principles
- product, quotient, and chain rules
- integration techniques (by parts, substitution)
- differential equations
- applications to kinematics
Regular practice with a variety of question types is essential to build fluency and confidence in applying these mathematical techniques.