Comprehensive Calculus: Limits, Derivatives, Integrals, and Differential Equations Study Notes

The Exponential Function

  • The exponential function is defined as y=axy = a^x, where a>0a > 0 and xx is a variable. This function exists for integral, rational, and irrational exponents.
  • The Natural Exponential Function is defined as y=exy = e^x, where e=2.7183e = 2.7183 is the Euler number.
  • The Euler number is defined by the infinite series:     ex=∑k=0∞xkk!e^x = \sum_{k=0}^{\infty} \frac{x^k}{k!}

Properties and Graph of exe^x

  • The graph of y=exy = e^x for x>0x > 0 is asymptotic to the xx-axis and increases for all real values of xx.
  • Key mathematical properties include:
    1. e0=1e^0 = 1
    2. lim⁡x→−∞ex=0\lim_{x \to -\infty} e^x = 0
    3. lim⁡x→∞ex=∞\lim_{x \to \infty} e^x = \infty
    4. exey=ex+ye^x e^y = e^{x+y}
    5. exey=ex−y\frac{e^x}{e^y} = e^{x-y}
    6. (ex)r=exr(e^x)^r = e^{xr}

Calculus of Exponential Functions

  • Derivative of y=ef(x)y = e^{f(x)}: For a differentiable function ff, the derivative is given by:     y′(x)=f′(x)ef(x)y'(x) = f'(x) e^{f(x)}
  • Integral of y=ef(x)y = e^{f(x)}: If ff is a differentiable function of xx such that f′(x)f'(x) is a constant (not a function of xx), then:     ∫ef(x) dx=1f′(x)ef(x)+c\int e^{f(x)} \, dx = \frac{1}{f'(x)} e^{f(x)} + c
Examples: Derivatives
  1. y=ex2y = e^{x^2}
  2. y=e3x2y = e^{3x^2}
  3. y=e3x+1y = e^{3x+1}
  4. y=e5/xy = e^{5/x}
  5. y=exy = e^{\sqrt{x}}
  6. y=exsin⁡(x)y = e^{x \sin(x)}
Examples: Integrals
  1. ∫e2x+1 dx\int e^{2x+1} \, dx
  2. ∫ex/3 dx\int e^{x/3} \, dx
  3. ∫x2e−x3 dx\int x^2 e^{-x^3} \, dx
  4. ∫3ex/2 dx\int 3e^{x/2} \, dx
  5. ∫x2ex2 dx\int x^2 e^{x^2} \, dx
  6. ∫x3e−x4 dx\int x^3 e^{-x^4} \, dx

The Logarithmic Function

  • The logarithm of a number bb to the base aa (log⁡a(b)\log_a(b)) represents the power to which the base must be raised to equal bb:     log⁡a(b)=k  ⟹  b=ak\log_a(b) = k \implies b = a^k
  • Natural Logarithm: When the base is the Euler number ee, it is denoted as ln⁡(x)\ln(x).
  • Remark: Since ln⁡(x)\ln(x) is not defined for x<0x < 0, the notation ln⁡∣x∣\ln|x| is preferred in general contexts.

Properties and Graph of ln⁡(x)\ln(x)

  • The graph of y=ln⁡(x)y = \ln(x) for x>0x > 0 is asymptotic to the yy-axis.
  • Logarithmic characteristics based on domain:
    1. ln⁡(x)<0\ln(x) < 0 for all x∈Rx \in \mathbb{R} such that 0<x<10 < x < 1.
    2. ln⁡(x)=0\ln(x) = 0 for x=1x = 1.
    3. ln⁡(x)>0\ln(x) > 0 for all x≥1x \ge 1.
  • Mathematical properties:
    1. ln⁡(xy)=ln⁡(x)+ln⁡(y)\ln(xy) = \ln(x) + \ln(y)
    2. ln⁡(xy)=ln⁡(x)−ln⁡(y)\ln(\frac{x}{y}) = \ln(x) - \ln(y)
    3. ln⁡(xa)=aln⁡(x)\ln(x^a) = a \ln(x), where aa is a constant.
    4. ln⁡(b)=log⁡a(b)log⁡a(e)\ln(b) = \frac{\log_a(b)}{\log_a(e)}
    5. ln⁡(e)=1\ln(e) = 1
    6. lim⁡x→∞ln⁡(x)=∞\lim_{x \to \infty} \ln(x) = \infty
    7. lim⁡x→0+ln⁡(x)=−∞\lim_{x \to 0^+} \ln(x) = -\infty
    8. ln⁡(x)\ln(x) is a strictly increasing function.

Calculus of Logarithmic Functions

  • Derivative of ln⁡(f(x))\ln(f(x)): Given y=ln⁡(f(x))y = \ln(f(x)), then:     y′=f′(x)f(x)y' = \frac{f'(x)}{f(x)}
  • Integration resulting in Logarithms: The rule ∫xn dx=xn+1n+1+c\int x^n \, dx = \frac{x^{n+1}}{n+1} + c fails for n=−1n = -1. Since ddx(ln⁡(x))=1x\frac{d}{dx}(\ln(x)) = \frac{1}{x}, it follows that:     ∫1x dx=ln⁡∣x∣+c\int \frac{1}{x} \, dx = \ln|x| + c     Alternatively, ∫1x dx=ln⁡∣kx∣\int \frac{1}{x} \, dx = \ln|kx| where c=ln⁡∣k∣c = \ln|k|.
Examples: Logarithmic Operations
  1. Express as sum or difference:     (a) ln⁡(cot⁡(x))\ln(\cot(x))     (b) ln⁡(tan⁡2(x))\ln(\tan^2(x))     (c) ln⁡(x2−4)\ln(x^2 - 4)     (d) ln⁡(x+1x−1)\ln\left(\sqrt{\frac{x+1}{x-1}}\right)     (e) ln⁡(3x2sin⁡4(x))\ln(3x^2 \sin^4(x))

  2. Express as single logarithm:     (a) ln⁡(x)+ln⁡(y)−1\ln(x) + \ln(y) - 1     (b) ln⁡(e3x)+ln⁡(xe)\ln(\frac{e^3}{x}) + \ln(\frac{x}{e})

General Exponential Function axa^x

  • Derivative of axa^x: To find ddx(ax)\frac{d}{dx}(a^x), let y=axy = a^x.     Taking natural logs: ln⁡(y)=xln⁡(a)\ln(y) = x \ln(a).     Implicit differentiation: 1ydydx=ln⁡(a)\frac{1}{y} \frac{dy}{dx} = \ln(a).     The result is:     ddx(ax)=axln⁡(a)\frac{d}{dx}(a^x) = a^x \ln(a)
  • Integral of axa^x: Based on the derivative result:     ∫ax dx=axln⁡(a)+c\int a^x \, dx = \frac{a^x}{\ln(a)} + c

Definite Integrals with Negative Bounds

  • When evaluating ∫ab1x dx\int_a^b \frac{1}{x} \, dx for a<0a < 0 and b<0b < 0, the standard primitive ln⁡(x)\ln(x) is undefined.
  • However, for x<0x < 0, the function ln⁡(−x)\ln(-x) exists and its derivative is −1−x=1x\frac{-1}{-x} = \frac{1}{x}.
  • Thus, the generalized form is:     ∫ab1x dx=[ln⁡∣x∣]ab\int_a^b \frac{1}{x} \, dx = [\ln|x|]_a^b
  • Condition for Existence: This integral is undefined if the interval [a,b][a, b] contains x=0x = 0, as y=1xy = \frac{1}{x} is discontinuous at that point.

Integration by Parts

  • This technique is derived from the product rule of differentiation: ddx(uv)=vdudx+udvdx\frac{d}{dx}(uv) = v \frac{du}{dx} + u \frac{dv}{dx}.

  • By integrating both sides and rearranging, the formula is:     ∫u dv=uv−∫v du\int u \, dv = uv - \int v \, du

  • 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)\ln(x): Using integration by parts with u=ln⁡(x)u = \ln(x), dv=dxdv = dx, du=dxxdu = \frac{dx}{x}, and v=xv = x:     ∫ln⁡(x) dx=xln⁡(x)−∫xdxx=xln⁡(x)−x+c\int \ln(x) \, dx = x \ln(x) - \int x \frac{dx}{x} = x \ln(x) - x + c

Trigonometric Functions: Derivatives and Integrals

Basic Trigonometric Identities
  • csc⁡(x)=1sin⁡(x)\csc(x) = \frac{1}{\sin(x)}
  • sec⁡(x)=1cos⁡(x)\sec(x) = \frac{1}{\cos(x)}
  • cot⁡(x)=1tan⁡(x)\cot(x) = \frac{1}{\tan(x)}
Derivatives
  1. ddx(sin⁡(x))=cos⁡(x)\frac{d}{dx}(\sin(x)) = \cos(x)
  2. ddx(cos⁡(x))=−sin⁡(x)\frac{d}{dx}(\cos(x)) = -\sin(x)
  3. ddx(tan⁡(x))=sec⁡2(x)\frac{d}{dx}(\tan(x)) = \sec^2(x)
  4. ddx(sec⁡(x))=sec⁡(x)tan⁡(x)\frac{d}{dx}(\sec(x)) = \sec(x) \tan(x)
  5. ddx(csc⁡(x))=−csc⁡(x)cot⁡(x)\frac{d}{dx}(\csc(x)) = -\csc(x) \cot(x)
  6. ddx(cot⁡(x))=−csc⁡2(x)\frac{d}{dx}(\cot(x)) = -\csc^2(x)
  • General Power Rule: If y=sin⁡n(x)y = \sin^n(x), then dydx=nsin⁡n−1(x)cos⁡(x)\frac{dy}{dx} = n \sin^{n-1}(x) \cos(x). If y=cos⁡n(x)y = \cos^n(x), then dydx=ncos⁡n−1(x)(−sin⁡(x))\frac{dy}{dx} = n \cos^{n-1}(x) (-\sin(x)).
Integrals
  1. ∫sin⁡(x) dx=−cos⁡(x)+c\int \sin(x) \, dx = -\cos(x) + c
  2. ∫cos⁡(x) dx=sin⁡(x)+c\int \cos(x) \, dx = \sin(x) + c
  3. ∫tan⁡(x) dx=−ln⁡∣cos⁡(x)∣+c=ln⁡∣sec⁡(x)∣+c\int \tan(x) \, dx = -\ln|\cos(x)| + c = \ln|\sec(x)| + c
  4. ∫sec⁡2(x) dx=tan⁡(x)+c\int \sec^2(x) \, dx = \tan(x) + c
  5. ∫csc⁡2(x) dx=−cot⁡(x)+c\int \csc^2(x) \, dx = -\cot(x) + c
  • Linear Arguments:     ∫cos⁡(ax+b) dx=1asin⁡(ax+b)+c\int \cos(ax+b) \, dx = \frac{1}{a} \sin(ax+b) + c∫sin⁡(ax+b) dx=−1acos⁡(ax+b)+c\int \sin(ax+b) \, dx = -\frac{1}{a} \cos(ax+b) + c

Integration of Trigonometric Powers

Even Powers of Sine and Cosine

Uses identities:

  • cos⁡2(x)=12(1+cos⁡(2x))\cos^2(x) = \frac{1}{2}(1 + \cos(2x))
  • sin⁡2(x)=12(1−cos⁡(2x))\sin^2(x) = \frac{1}{2}(1 - \cos(2x))
Odd Powers of Sine and Cosine

Uses the identity sin⁡2(x)+cos⁡2(x)=1\sin^2(x) + \cos^2(x) = 1. The power is split (e.g., sin⁡5(x)=sin⁡4(x)sin⁡(x)\sin^5(x) = \sin^4(x) \sin(x)) and solved via substitution.

Powers of Tangent

Uses the identity tan⁡2(x)=sec⁡2(x)−1\tan^2(x) = \sec^2(x) - 1.

Product Form Inspections
  1. ∫sin⁡(x)cos⁡n(x) dx=−1n+1cos⁡n+1(x)+c\int \sin(x) \cos^n(x) \, dx = -\frac{1}{n+1} \cos^{n+1}(x) + c
  2. ∫cos⁡(x)sin⁡n(x) dx=1n+1sin⁡n+1(x)+c\int \cos(x) \sin^n(x) \, dx = \frac{1}{n+1} \sin^{n+1}(x) + c

Inverse Trigonometric Functions

  • Derivatives:

    1. ddx(sin⁡−1(x))=11−x2\frac{d}{dx}(\sin^{-1}(x)) = \frac{1}{\sqrt{1-x^2}}
    2. ddx(cos⁡−1(x))=−11−x2\frac{d}{dx}(\cos^{-1}(x)) = -\frac{1}{\sqrt{1-x^2}}
    3. ddx(tan⁡−1(x))=11+x2\frac{d}{dx}(\tan^{-1}(x)) = \frac{1}{1+x^2}
  • Integration via Trigonometric Substitution:     To evaluate ∫1a2−b2x2 dx\int \frac{1}{\sqrt{a^2 - b^2 x^2}} \, dx, use x=absin⁡(θ)x = \frac{a}{b} \sin(\theta). Result: 1bsin⁡−1(bxa)+c\frac{1}{b} \sin^{-1}(\frac{bx}{a}) + c.     To evaluate ∫1a2+b2x2 dx\int \frac{1}{a^2 + b^2 x^2} \, dx, use x=abtan⁡(θ)x = \frac{a}{b} \tan(\theta). Result: 1abtan⁡−1(bxa)+c\frac{1}{ab} \tan^{-1}(\frac{bx}{a}) + c.

Trigonometric Product Identities for Integration

For integrals of products with different linear arguments (αx\alpha x and βx\beta x):

  1. sin⁡(α)sin⁡(β)=12cos⁡(α−β)−12cos⁡(α+β)\sin(\alpha) \sin(\beta) = \frac{1}{2} \cos(\alpha - \beta) - \frac{1}{2} \cos(\alpha + \beta)
  2. cos⁡(α)cos⁡(β)=12cos⁡(α−β)+12cos⁡(α+β)\cos(\alpha) \cos(\beta) = \frac{1}{2} \cos(\alpha - \beta) + \frac{1}{2} \cos(\alpha + \beta)
  3. sin⁡(α)cos⁡(β)=12sin⁡(α−β)+12sin⁡(α+β)\sin(\alpha) \cos(\beta) = \frac{1}{2} \sin(\alpha - \beta) + \frac{1}{2} \sin(\alpha + \beta)
  4. cos⁡(α)sin⁡(β)=12sin⁡(α+β)−12sin⁡(α−β)\cos(\alpha) \sin(\beta) = \frac{1}{2} \sin(\alpha + \beta) - \frac{1}{2} \sin(\alpha - \beta)

Hyperbolic Functions

Defined in terms of exponential functions:

  1. sinh⁡(x)=ex−e−x2\sinh(x) = \frac{e^x - e^{-x}}{2}
  2. cosh⁡(x)=ex+e−x2\cosh(x) = \frac{e^x + e^{-x}}{2}
  3. tanh⁡(x)=sinh⁡(x)cosh⁡(x)=ex−e−xex+e−x\tanh(x) = \frac{\sinh(x)}{\cosh(x)} = \frac{e^x - e^{-x}}{e^x + 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: cos⁡2(x)+sin⁡2(x)=1  ⟹  cosh⁡2(x)−sinh⁡2(x)=1\cos^2(x) + \sin^2(x) = 1 \implies \cosh^2(x) - \sinh^2(x) = 1.
Derivatives of Hyperbolic Functions
  1. ddx(cosh⁡(x))=sinh⁡(x)\frac{d}{dx}(\cosh(x)) = \sinh(x)
  2. ddx(sinh⁡(x))=cosh⁡(x)\frac{d}{dx}(\sinh(x)) = \cosh(x)

Inverse Hyperbolic Functions

Expressed in logarithmic form:

  1. sinh⁡−1(x)=ln⁡(x+1+x2)\sinh^{-1}(x) = \ln(x + \sqrt{1 + x^2})
  2. cosh⁡−1(x)=ln⁡(x+x2−1)\cosh^{-1}(x) = \ln(x + \sqrt{x^2 - 1})
  3. tanh⁡−1(x)=12ln⁡(1+x1−x)\tanh^{-1}(x) = \frac{1}{2} \ln\left(\frac{1+x}{1-x}\right)

Even and Odd Functions

  • Even Functions: Satisfy f(−x)=f(x)f(-x) = f(x). Symmetric about the yy-axis. Examples: ∣x∣|x|, x2x^2, cos⁡(x)\cos(x).     ∫−aaf(x) dx=2∫0af(x) dx\int_{-a}^a f(x) \, dx = 2 \int_0^a f(x) \, dx
  • Odd Functions: Satisfy f(−x)=−f(x)f(-x) = -f(x). Symmetric about the origin (rotational symmetry). Examples: x3x^3, sin⁡(x)\sin(x), tan⁡(x)\tan(x).     ∫−aaf(x) dx=0\int_{-a}^a f(x) \, dx = 0

Ordinary Differential Equations (ODEs)

  • An equation containing differential coefficients like dydx\frac{dy}{dx}.
  • 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
  1. Separable Variables: Equations where terms can be grouped by variable (e.g., dydx=xy  ⟹  ∫1y dy=∫x dx\frac{dy}{dx} = xy \implies \int \frac{1}{y} \, dy = \int x \, dx).
  2. Exact Equations: Equations where one side is a direct derivative of a function. If not exact, an Integrating Factor (II) is used.
  3. Linear Equations: Formed as dydx+ay=b\frac{dy}{dx} + ay = b, where aa and bb are functions of xx or constants.
    • Integrating Factor: I(x)=e∫a dxI(x) = e^{\int a \, dx}.
    • General Solution: ddx(Iy)=bI  ⟹  Iy=∫bI dx\frac{d}{dx}(Iy) = bI \implies Iy = \int bI \, dx.
Second-Order Linear ODEs with Constant Coefficients

Form: ad2ydx2+bdydx+cy=0a \frac{d^2y}{dx^2} + b \frac{dy}{dx} + cy = 0. We assume valid solution y=eλxy = e^{\lambda x}, leading to the Auxiliary Quadratic Equation: aλ2+bλ+c=0a\lambda^2 + b\lambda + c = 0.

Solutions based on Discriminate (b2−4acb^2 - 4ac):

  1. Identical Real Roots (λ1\lambda_1): y=eλ1x(Ax+B)y = e^{\lambda_1 x}(Ax + B)
  2. Distinct Real Roots (λ1,λ2\lambda_1, \lambda_2): y=Aeλ1x+Beλ2xy = A e^{\lambda_1 x} + B e^{\lambda_2 x}
  3. Complex Roots (α±βi\alpha \pm \beta i): y=eαx(Acos⁡(βx)+Bsin⁡(βx))y = e^{\alpha x}(A \cos(\beta x) + B \sin(\beta x))
Non-Homogeneous Equations

Form: ay′′+by′+cy=f(x)ay'' + by' + cy = f(x). The general solution is yn=yc+ypy_n = y_c + y_p, where:

  • ycy_c (Complementary Solution) solves the homogeneous equation f(x)=0f(x) = 0.
  • ypy_p (Particular Integral) is a specific solution suited to the type of f(x)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\alpha and β\beta:     A=∫αβ12r2 dθA = \int_{\alpha}^{\beta} \frac{1}{2} r^2 \, d\theta

  • Length of a Curve (Arc Length):

    1. Cartesian: L=∫ab1+(dydx)2 dxL = \int_a^b \sqrt{1 + \left(\frac{dy}{dx}\right)^2} \, dx
    2. Parametric (x=f(t),y=g(t)x=f(t), y=g(t)): L=∫t1t2(dxdt)2+(dydt)2 dtL = \int_{t_1}^{t_2} \sqrt{\left(\frac{dx}{dt}\right)^2 + \left(\frac{dy}{dt}\right)^2} \, dt
    3. Polar: L=∫αβr2+(drdθ)2 dθL = \int_{\alpha}^{\beta} \sqrt{r^2 + \left(\frac{dr}{d\theta}\right)^2} \, d\theta