Comprehensive Calculus: Limits, Derivatives, Integrals, and Differential Equations Study Notes
The Exponential Function
The exponential function is defined as y=ax, where a>0 and x is a variable. This function exists for integral, rational, and irrational exponents.
The Natural Exponential Function is defined as y=ex, where e=2.7183 is the Euler number.
The Euler number is defined by the infinite series:
ex=∑k=0∞k!xk
Properties and Graph of ex
The graph of y=ex for x>0 is asymptotic to the x-axis and increases for all real values of x.
Key mathematical properties include:
e0=1
limx→−∞ex=0
limx→∞ex=∞
exey=ex+y
eyex=ex−y
(ex)r=exr
Calculus of Exponential Functions
Derivative of y=ef(x): For a differentiable function f, the derivative is given by:
y′(x)=f′(x)ef(x)
Integral of y=ef(x): If f is a differentiable function of x such that f′(x) is a constant (not a function of x), then:
∫ef(x)dx=f′(x)1ef(x)+c
Examples: Derivatives
y=ex2
y=e3x2
y=e3x+1
y=e5/x
y=ex
y=exsin(x)
Examples: Integrals
∫e2x+1dx
∫ex/3dx
∫x2e−x3dx
∫3ex/2dx
∫x2ex2dx
∫x3e−x4dx
The Logarithmic Function
The logarithm of a number b to the base a (loga(b)) represents the power to which the base must be raised to equal b:
loga(b)=k⟹b=ak
Natural Logarithm: When the base is the Euler number e, it is denoted as ln(x).
Remark: Since ln(x) is not defined for x<0, the notation ln∣x∣ is preferred in general contexts.
Properties and Graph of ln(x)
The graph of y=ln(x) for x>0 is asymptotic to the y-axis.
Logarithmic characteristics based on domain:
ln(x)<0 for all x∈R such that 0<x<1.
ln(x)=0 for x=1.
ln(x)>0 for all x≥1.
Mathematical properties:
ln(xy)=ln(x)+ln(y)
ln(yx)=ln(x)−ln(y)
ln(xa)=aln(x), where a is a constant.
ln(b)=loga(e)loga(b)
ln(e)=1
limx→∞ln(x)=∞
limx→0+ln(x)=−∞
ln(x) is a strictly increasing function.
Calculus of Logarithmic Functions
Derivative of ln(f(x)): Given y=ln(f(x)), then:
y′=f(x)f′(x)
Integration resulting in Logarithms: The rule ∫xndx=n+1xn+1+c fails for n=−1. Since dxd(ln(x))=x1, it follows that:
∫x1dx=ln∣x∣+c
Alternatively, ∫x1dx=ln∣kx∣ where c=ln∣k∣.
Examples: Logarithmic Operations
Express as sum or difference:
(a) ln(cot(x))
(b) ln(tan2(x))
(c) ln(x2−4)
(d) ln(x−1x+1)
(e) ln(3x2sin4(x))
Express as single logarithm:
(a) ln(x)+ln(y)−1
(b) ln(xe3)+ln(ex)
General Exponential Function ax
Derivative of ax: To find dxd(ax), let y=ax.
Taking natural logs: ln(y)=xln(a).
Implicit differentiation: y1dxdy=ln(a).
The result is:
dxd(ax)=axln(a)
Integral of ax: Based on the derivative result:
∫axdx=ln(a)ax+c
Definite Integrals with Negative Bounds
When evaluating ∫abx1dx for a<0 and b<0, the standard primitive ln(x) is undefined.
However, for x<0, the function ln(−x) exists and its derivative is −x−1=x1.
Thus, the generalized form is:
∫abx1dx=[ln∣x∣]ab
Condition for Existence: This integral is undefined if the interval [a,b] contains x=0, as y=x1 is discontinuous at that point.
Integration by Parts
This technique is derived from the product rule of differentiation: dxd(uv)=vdxdu+udxdv.
By integrating both sides and rearranging, the formula is:
∫udv=uv−∫vdu
Applications: This method applies to combinations including:
Polynomial and trigonometric
Polynomial and exponential
Polynomial and logarithm
Inverse trigonometric functions
Logarithmic functions
Exponential and trigonometric
Exponential and logarithm
Integral of ln(x): Using integration by parts with u=ln(x), dv=dx, du=xdx, and v=x:
∫ln(x)dx=xln(x)−∫xxdx=xln(x)−x+c
Trigonometric Functions: Derivatives and Integrals
Basic Trigonometric Identities
csc(x)=sin(x)1
sec(x)=cos(x)1
cot(x)=tan(x)1
Derivatives
dxd(sin(x))=cos(x)
dxd(cos(x))=−sin(x)
dxd(tan(x))=sec2(x)
dxd(sec(x))=sec(x)tan(x)
dxd(csc(x))=−csc(x)cot(x)
dxd(cot(x))=−csc2(x)
General Power Rule: If y=sinn(x), then dxdy=nsinn−1(x)cos(x). If y=cosn(x), then dxdy=ncosn−1(x)(−sin(x)).
Integrals
∫sin(x)dx=−cos(x)+c
∫cos(x)dx=sin(x)+c
∫tan(x)dx=−ln∣cos(x)∣+c=ln∣sec(x)∣+c
∫sec2(x)dx=tan(x)+c
∫csc2(x)dx=−cot(x)+c
Linear Arguments:
∫cos(ax+b)dx=a1sin(ax+b)+c∫sin(ax+b)dx=−a1cos(ax+b)+c
Integration of Trigonometric Powers
Even Powers of Sine and Cosine
Uses identities:
cos2(x)=21(1+cos(2x))
sin2(x)=21(1−cos(2x))
Odd Powers of Sine and Cosine
Uses the identity sin2(x)+cos2(x)=1. The power is split (e.g., sin5(x)=sin4(x)sin(x)) and solved via substitution.
Powers of Tangent
Uses the identity tan2(x)=sec2(x)−1.
Product Form Inspections
∫sin(x)cosn(x)dx=−n+11cosn+1(x)+c
∫cos(x)sinn(x)dx=n+11sinn+1(x)+c
Inverse Trigonometric Functions
Derivatives:
dxd(sin−1(x))=1−x21
dxd(cos−1(x))=−1−x21
dxd(tan−1(x))=1+x21
Integration via Trigonometric Substitution:
To evaluate ∫a2−b2x21dx, use x=basin(θ). Result: b1sin−1(abx)+c.
To evaluate ∫a2+b2x21dx, use x=batan(θ). Result: ab1tan−1(abx)+c.
Trigonometric Product Identities for Integration
For integrals of products with different linear arguments (αx and βx):
sin(α)sin(β)=21cos(α−β)−21cos(α+β)
cos(α)cos(β)=21cos(α−β)+21cos(α+β)
sin(α)cos(β)=21sin(α−β)+21sin(α+β)
cos(α)sin(β)=21sin(α+β)−21sin(α−β)
Hyperbolic Functions
Defined in terms of exponential functions:
sinh(x)=2ex−e−x
cosh(x)=2ex+e−x
tanh(x)=cosh(x)sinh(x)=ex+e−xex−e−x
Osborn's Rule
A rule for converting trigonometric identities into hyperbolic identities: replace sine and cosine with hyperbolic counterparts. If a term contains a product of two sines (explicitly or implicitly via tangent/cotangent), the sign of that product must be negated.
Example: cos2(x)+sin2(x)=1⟹cosh2(x)−sinh2(x)=1.
Derivatives of Hyperbolic Functions
dxd(cosh(x))=sinh(x)
dxd(sinh(x))=cosh(x)
Inverse Hyperbolic Functions
Expressed in logarithmic form:
sinh−1(x)=ln(x+1+x2)
cosh−1(x)=ln(x+x2−1)
tanh−1(x)=21ln(1−x1+x)
Even and Odd Functions
Even Functions: Satisfy f(−x)=f(x). Symmetric about the y-axis. Examples: ∣x∣, x2, cos(x).
∫−aaf(x)dx=2∫0af(x)dx
Odd Functions: Satisfy f(−x)=−f(x). Symmetric about the origin (rotational symmetry). Examples: x3, sin(x), tan(x).
∫−aaf(x)dx=0
Ordinary Differential Equations (ODEs)
An equation containing differential coefficients like dxdy.
Order: Determined by the highest derivative present.
General Solution: Defines a family of curves.
Particular Solution: Obtained when initial conditions are used to find specific constants.
First-Order ODEs
Separable Variables: Equations where terms can be grouped by variable (e.g., dxdy=xy⟹∫y1dy=∫xdx).
Exact Equations: Equations where one side is a direct derivative of a function. If not exact, an Integrating Factor (I) is used.
Linear Equations: Formed as dxdy+ay=b, where a and b are functions of x or constants.
Integrating Factor: I(x)=e∫adx.
General Solution: dxd(Iy)=bI⟹Iy=∫bIdx.
Second-Order Linear ODEs with Constant Coefficients
Form: adx2d2y+bdxdy+cy=0.
We assume valid solution y=eλx, leading to the Auxiliary Quadratic Equation: aλ2+bλ+c=0.
Solutions based on Discriminate (b2−4ac):
Identical Real Roots (λ1): y=eλ1x(Ax+B)
Distinct Real Roots (λ1,λ2): y=Aeλ1x+Beλ2x
Complex Roots (α±βi): y=eαx(Acos(βx)+Bsin(βx))
Non-Homogeneous Equations
Form: ay′′+by′+cy=f(x). The general solution is yn=yc+yp, where:
yc (Complementary Solution) solves the homogeneous equation f(x)=0.
yp (Particular Integral) is a specific solution suited to the type of f(x) (Polynomial, Exponential, or Trigonometric).
Geometrical Applications of Calculus
Area of a Sector (Polar Coordinates):
For a sector bounded by radius vectors at angles α and β:
A=∫αβ21r2dθ