Comprehensive Study Guide for Differential Calculus: Trigonometry, Limits, Continuity, and Derivatives

Foundations and Scope of Differential Calculus

Calculus is fundamentally structured around breaking a mathematical or physical quantity into smaller pieces to analyze its behavior and reconstruct comprehensive properties:

  • Calculus: The broad mathematical discipline of breaking up a continuous entity into infinitesimal pieces to perform analytical operations.
  • Differential Calculus: The branch of calculus centered on breaking up an entity into smaller pieces and working directly with those individual, infinitesimal pieces (rates of change, slopes, and local behaviors).
  • Integral Calculus: The branch of calculus centered on breaking up an entity into smaller pieces, analyzing those pieces, and integrating (accumulating or summing) them together to determine total quantities (areas, volumes, and accumulated change).

The primary foundational topics encompassed within Differential Calculus include:

  • Trigonometry and Functions
  • Limits and Continuity
  • Derivatives and Differentiation Techniques
  • Applications of Derivatives
  • Introduction to Definite and Indefinite Integrals
Historical Context and Modern Perspective of Trigonometry

Derived from the Greek language, the word trigonometry literally translates to "measurement of triangles." In its classical formulation, trigonometry dealt strictly with the geometric relationships among the sides and angles of triangles. This geometric framework was essential in ancient and early modern developments in astronomy, navigation, and land surveying.

During the seventeenth century, concurrent with the invention of calculus and the formulation of modern physical sciences, a fundamental shift in perspective occurred. Classic geometric triangle ratios were reconceptualized as analytic functions whose domains consist of the entire set of real numbers. This analytical transition expanded the applications of trigonometry far beyond static triangles to dynamic physical phenomena involving vibrations, periodic cycles, and rotations, including:

  • Sound waves
  • Light rays and electromagnetic waves
  • Planetary orbits
  • Vibrating strings
  • Pendulums
  • Trajectories and orbits of subatomic particles
Fundamental Mathematical Constants

In mathematics, fundamental constants have values strictly fixed by unambiguous definitions rather than arbitrary convention:

  • Archimedes' Constant (π\pi): Defined strictly as the ratio of any circle's circumference (CC) to its diameter (dd):   π=Cd\pi = \frac{C}{d}   Numerical approximation: π≈3.14159…\pi \approx 3.14159\dots(Note: Fractions such as 227\frac{22}{7} are rational approximations, and 180∘180^\circ represents its angular degree equivalence, but its true mathematical definition is the ratio Cd\frac{C}{d}.)
  • Euler's Number (ee): The base of the natural logarithm, representing continuous growth.
  • The Imaginary Unit (ii): Defined by i=−1i = \sqrt{-1}, where i2=−1i^2 = -1.
  • Pythagoras' Constant (2\sqrt{2}): The length of the hypotenuse of an isosceles right triangle with unit legs.

Angles, Rotational Geometry, and Angle Measurement

An angle is generated by rotating a ray (half-line) around its fixed endpoint:

  • Vertex: The fixed endpoint of the ray.
  • Initial Side: The starting position of the ray before rotation.
  • Terminal Side: The final position of the ray after rotation.
  • Standard Position: An angle positioned on a Cartesian coordinate plane such that its vertex coincides with the origin (0,0)(0, 0) and its initial side lies along the positive xx-axis.
  • Rotation Direction:
    • Counterclockwise rotation produces positive angles.
    • Clockwise rotation produces negative angles.
  • Nomenclature: Angles are standardly labeled using Greek letters such as α\alpha (alpha), β\beta (beta), and θ\theta (theta), or uppercase Latin letters such as AA, BB, and CC.
  • Coterminal Angles: Two angles that share the exact same initial and terminal sides. For any given angle θ\theta, there are infinitely many coterminal angles given by:   θ+n(360∘)orθ+2πn,n∈Z\theta + n(360^\circ) \quad \text{or} \quad \theta + 2\pi n, \quad n \in \mathbb{Z}
Degree Measure

A degree represents a rotational unit of measure denoted by the symbol ∘^\circ. A single degree (1∘1^\circ) is defined precisely as equivalent to a rotation of 1360\frac{1}{360} of a complete circular revolution about the vertex:

  • Complete revolution: 360∘360^\circ
  • Half revolution (straight angle): 180∘180^\circ
  • Quarter revolution (right angle): 90∘90^\circ

Coordinate plane quadrants are numbered counterclockwise as I, II, III, and IV:

  • Quadrant I: 0∘<θ<90∘0^\circ < \theta < 90^\circ
  • Quadrant II: 90∘<θ<180∘90^\circ < \theta < 180^\circ
  • Quadrant III: 180∘<θ<270∘180^\circ < \theta < 270^\circ
  • Quadrant IV: 270∘<θ<360∘270^\circ < \theta < 360^\circ

Angle classifications by magnitude:

  • Acute Angle: An angle strictly between 0∘0^\circ and 90∘90^\circ.
  • Obtuse Angle: An angle strictly between 90∘90^\circ and 180∘180^\circ.
  • Complementary Angles: Two positive angles α\alpha and β\beta whose sum is 90∘90^\circ (π2 rad\frac{\pi}{2}\,\text{rad}):   α+β=90∘\alpha + \beta = 90^\circ
  • Supplementary Angles: Two positive angles α\alpha and β\beta whose sum is 180∘180^\circ (π rad\pi\,\text{rad}):   α+β=180∘\alpha + \beta = 180^\circ
Radian Measure and Arc Length

Radian measure relies on the geometry of a central angle whose vertex is at the center of a circle. One radian (1 rad1\,\text{rad}) is defined as the measure of a central angle θ\theta that intercepts an arc ss equal in length to the radius rr of the circle.

Algebraic relationship: θ=sr\theta = \frac{s}{r} where θ\theta is measured in radians, ss is arc length, and rr is radius. Consequently: s=rθs = r\theta

When an angle measure is given without explicit units, radian measure is universally implied (e.g., θ=2\theta = 2 denotes θ=2 radians\theta = 2\,\text{radians}).

Because a complete revolution corresponds to an arc length equal to the full circumference s=2πrs = 2\pi r: θ=2πrr=2π rad=360∘\theta = \frac{2\pi r}{r} = 2\pi\,\text{rad} = 360^\circ Dividing both sides by 2 yields: π rad=180∘\pi\,\text{rad} = 180^\circ Because 2π≈6.282\pi \approx 6.28, there are slightly more than 6 radius lengths along the circumference of a complete circle.

Conversion Formulas and Worked Examples
  1. Degrees to Radians: Multiply by π rad180∘\frac{\pi\,\text{rad}}{180^\circ}
  2. Radians to Degrees: Multiply by 180∘π rad\frac{180^\circ}{\pi\,\text{rad}}
Conversion Examples
  • Convert 135∘135^\circ to radians:   135∘×π rad180∘=3π4 rad135^\circ \times \frac{\pi\,\text{rad}}{180^\circ} = \frac{3\pi}{4}\,\text{rad}
  • Convert −270∘-270^\circ to radians:   −270∘×π rad180∘=−3π2 rad-270^\circ \times \frac{\pi\,\text{rad}}{180^\circ} = -\frac{3\pi}{2}\,\text{rad}
  • Convert 30∘30^\circ to radians:   30∘×π180∘=π6 rad30^\circ \times \frac{\pi}{180^\circ} = \frac{\pi}{6}\,\text{rad}
  • Convert 45∘45^\circ to radians:   45∘×π180∘=π4 rad45^\circ \times \frac{\pi}{180^\circ} = \frac{\pi}{4}\,\text{rad}
  • Convert 50∘50^\circ to radians:   50∘×π180∘=5π18 rad50^\circ \times \frac{\pi}{180^\circ} = \frac{5\pi}{18}\,\text{rad}
  • Convert π2 rad\frac{\pi}{2}\,\text{rad} to degrees:   π2 rad×180∘π rad=90∘\frac{\pi}{2}\,\text{rad} \times \frac{180^\circ}{\pi\,\text{rad}} = 90^\circ
  • Convert 2 rad2\,\text{rad} to degrees:   2 rad×180∘π rad=360∘π≈114.59∘2\,\text{rad} \times \frac{180^\circ}{\pi\,\text{rad}} = \frac{360^\circ}{\pi} \approx 114.59^\circ
  • Convert π18 rad\frac{\pi}{18}\,\text{rad} to degrees:   π18×180∘π=10∘\frac{\pi}{18} \times \frac{180^\circ}{\pi} = 10^\circ
  • Convert 4 rad4\,\text{rad} to degrees:   4×180∘π=720∘π4 \times \frac{180^\circ}{\pi} = \frac{720^\circ}{\pi}
Arc Length and Subtended Angle Problems
  • Finding Angle (θ\theta): Given r=5 cmr = 5\,\text{cm} and arc length s=15 cms = 15\,\text{cm}:   θ=sr=15 cm5 cm=3 rad\theta = \frac{s}{r} = \frac{15\,\text{cm}}{5\,\text{cm}} = 3\,\text{rad}
  • Finding Angle with π\pi: Given r=π cmr = \pi\,\text{cm} and s=2 cms = 2\,\text{cm}:   θ=sr=2π rad\theta = \frac{s}{r} = \frac{2}{\pi}\,\text{rad}
  • Finding Arc Length (ss): Given r=4 inchesr = 4\,\text{inches} and θ=3.5 rad\theta = 3.5\,\text{rad}:   s=rθ=(4 inches)(3.5)=14 inchess = r\theta = (4\,\text{inches})(3.5) = 14\,\text{inches}
  • Finding Arc Length with Degree Input: Given r=4 inchesr = 4\,\text{inches} and central angle θ=240∘\theta = 240^\circ:   First convert θ\theta to radians:   θ=240∘×π180∘=4π3 rad\theta = 240^\circ \times \frac{\pi}{180^\circ} = \frac{4\pi}{3}\,\text{rad}   Then calculate ss:   s=rθ=(4)(4π3)=16π3 inchess = r\theta = (4)\left(\frac{4\pi}{3}\right) = \frac{16\pi}{3}\,\text{inches}

The Six Trigonometric Functions and Reference Angles

Right Triangle Definitions (0<θ<π20 < \theta < \frac{\pi}{2})

For an acute angle θ\theta within a right triangle, the three sides are designated relative to θ\theta as Hypotenuse (hyp\text{hyp}), Opposite (opp\text{opp}), and Adjacent (adj\text{adj}):

  • Sine: sin⁡(θ)=opphyp\sin(\theta) = \frac{\text{opp}}{\text{hyp}}
  • Cosine: cos⁡(θ)=adjhyp\cos(\theta) = \frac{\text{adj}}{\text{hyp}}
  • Tangent: tan⁡(θ)=oppadj\tan(\theta) = \frac{\text{opp}}{\text{adj}}
  • Cosecant: csc⁡(θ)=hypopp\csc(\theta) = \frac{\text{hyp}}{\text{opp}}
  • Secant: sec⁡(θ)=hypadj\sec(\theta) = \frac{\text{hyp}}{\text{adj}}
  • Cotangent: cot⁡(θ)=adjopp\cot(\theta) = \frac{\text{adj}}{\text{opp}}

All ratios are strictly positive for acute angles (0∘<θ<90∘0^\circ < \theta < 90^\circ).

Cofunction Relationships for Complementary Angles

Cofunctions of complementary angles are identical:

  • sin⁡(90∘−θ)=cos⁡(θ)\sin(90^\circ - \theta) = \cos(\theta)
  • cos⁡(90∘−θ)=sin⁡(θ)\cos(90^\circ - \theta) = \sin(\theta)
  • tan⁡(90∘−θ)=cot⁡(θ)\tan(90^\circ - \theta) = \cot(\theta)
  • cot⁡(90∘−θ)=tan⁡(θ)\cot(90^\circ - \theta) = \tan(\theta)
  • sec⁡(90∘−θ)=csc⁡(θ)\sec(90^\circ - \theta) = \csc(\theta)
  • csc⁡(90∘−θ)=sec⁡(θ)\csc(90^\circ - \theta) = \sec(\theta)

In radians, replacing 90∘90^\circ with π2\frac{\pi}{2}:

  • sin⁡(π2−u)=cos⁡(u)\sin\left(\frac{\pi}{2} - u\right) = \cos(u)
  • cos⁡(π2−u)=sin⁡(u)\cos\left(\frac{\pi}{2} - u\right) = \sin(u)
  • tan⁡(π2−u)=cot⁡(u)\tan\left(\frac{\pi}{2} - u\right) = \cot(u)
  • cot⁡(π2−u)=tan⁡(u)\cot\left(\frac{\pi}{2} - u\right) = \tan(u)
  • sec⁡(π2−u)=csc⁡(u)\sec\left(\frac{\pi}{2} - u\right) = \csc(u)
  • csc⁡(π2−u)=sec⁡(u)\csc\left(\frac{\pi}{2} - u\right) = \sec(u)
Special Right Triangles: θ=π6\theta = \frac{\pi}{6} (30∘30^\circ)

In a 30∘–60∘–90∘30^\circ\text{--}60^\circ\text{--}90^\circ right triangle, the side lengths satisfy: hyp=2×opp,adj=3×opp\text{hyp} = 2 \times \text{opp}, \quad \text{adj} = \sqrt{3} \times \text{opp} Setting opp=1\text{opp} = 1, adj=3\text{adj} = \sqrt{3}, and hyp=2\text{hyp} = 2:

  • sin⁡(π6)=12\sin\left(\frac{\pi}{6}\right) = \frac{1}{2}
  • cos⁡(π6)=32\cos\left(\frac{\pi}{6}\right) = \frac{\sqrt{3}}{2}
  • tan⁡(π6)=13\tan\left(\frac{\pi}{6}\right) = \frac{1}{\sqrt{3}}
  • csc⁡(π6)=2\csc\left(\frac{\pi}{6}\right) = 2
  • sec⁡(π6)=23\sec\left(\frac{\pi}{6}\right) = \frac{2}{\sqrt{3}}
  • cot⁡(π6)=3\cot\left(\frac{\pi}{6}\right) = \sqrt{3}

Notice that sin⁡(30∘)=12=cos⁡(60∘)\sin(30^\circ) = \frac{1}{2} = \cos(60^\circ) because 30∘30^\circ and 60∘60^\circ are complementary.

General Angle Definitions (Any Real Angle θ\theta)

Let θ\theta be an angle in standard position. Let (x,y)(x, y) be any point on the terminal side of θ\theta distinct from the origin, with distance r=x2+y2>0r = \sqrt{x^2 + y^2} > 0:

  • sin⁡(θ)=yr\sin(\theta) = \frac{y}{r}
  • cos⁡(θ)=xr\cos(\theta) = \frac{x}{r}
  • tan⁡(θ)=yx,x≠0\tan(\theta) = \frac{y}{x}, \quad x \ne 0
  • csc⁡(θ)=ry,y≠0\csc(\theta) = \frac{r}{y}, \quad y \ne 0
  • sec⁡(θ)=rx,x≠0\sec(\theta) = \frac{r}{x}, \quad x \ne 0
  • cot⁡(θ)=xy,y≠0\cot(\theta) = \frac{x}{y}, \quad y \ne 0
Quadrantal Signs and the CAST Rule

The sign of each trigonometric function depends on the algebraic signs of the coordinates xx and yy:

  • Quadrant I (All positive - 'A'): x>0,y>0  ⟹  x > 0, y > 0 \implies All six functions are positive.
  • Quadrant II (Sine positive - 'S'): x<0,y>0  ⟹  sin⁡(θ)x < 0, y > 0 \implies \sin(\theta) and csc⁡(θ)\csc(\theta) are positive; others are negative.
  • Quadrant III (Tangent positive - 'T'): x<0,y<0  ⟹  tan⁡(θ)x < 0, y < 0 \implies \tan(\theta) and cot⁡(θ)\cot(\theta) are positive; others are negative.
  • Quadrant IV (Cosine positive - 'C'): x>0,y<0  ⟹  cos⁡(θ)x > 0, y < 0 \implies \cos(\theta) and sec⁡(θ)\sec(\theta) are positive; others are negative.
Reference Angles

For any angle θ\theta in standard position, its reference angle θ′\theta' is the acute angle formed by the terminal side of θ\theta and the horizontal xx-axis (0<θ′<π20 < \theta' < \frac{\pi}{2}):

  • Quadrant I: θ′=θ\theta' = \theta
  • Quadrant II: θ′=180∘−θ=π−θ\theta' = 180^\circ - \theta = \pi - \theta
  • Quadrant III: θ′=θ−180∘=θ−π\theta' = \theta - 180^\circ = \theta - \pi
  • Quadrant IV: θ′=360∘−θ=2π−θ\theta' = 360^\circ - \theta = 2\pi - \theta

To evaluate any trigonometric function f(θ)f(\theta): f(θ)=±f(θ′)f(\theta) = \pm f(\theta') where the sign (+ or −+\text{ or } -) is determined by the quadrant of θ\theta using the CAST rule.

Reference Angle Examples
  1. Find reference angle for θ=300∘\theta = 300^\circ:    Lies in Quadrant IV: θ′=360∘−300∘=60∘\theta' = 360^\circ - 300^\circ = 60^\circ.    sin⁡(300∘)=−sin⁡(60∘)=−32\sin(300^\circ) = -\sin(60^\circ) = -\frac{\sqrt{3}}{2}
  2. Find reference angle for θ=2.3 rad\theta = 2.3\,\text{rad}:    Since π2≈1.5708<2.3<π≈3.1416\frac{\pi}{2} \approx 1.5708 < 2.3 < \pi \approx 3.1416, θ\theta is in Quadrant II:    θ′=π−2.3≈3.1416−2.3=0.8416\theta' = \pi - 2.3 \approx 3.1416 - 2.3 = 0.8416
  3. Find reference angle and ratios for θ=−135∘\theta = -135^\circ:    Coterminal with −135∘+360∘=225∘-135^\circ + 360^\circ = 225^\circ (Quadrant III).    θ′=225∘−180∘=45∘\theta' = 225^\circ - 180^\circ = 45^\circ
    • sin⁡(−135∘)=−sin⁡(45∘)=−12\sin(-135^\circ) = -\sin(45^\circ) = -\frac{1}{\sqrt{2}}
    • cos⁡(−135∘)=−cos⁡(45∘)=−12\cos(-135^\circ) = -\cos(45^\circ) = -\frac{1}{\sqrt{2}}
    • tan⁡(−135∘)=+tan⁡(45∘)=1\tan(-135^\circ) = +\tan(45^\circ) = 1
  4. Find ratios for θ=−210∘\theta = -210^\circ:    −210∘+360∘=150∘-210^\circ + 360^\circ = 150^\circ (Quadrant II).    θ′=180∘−150∘=30∘\theta' = 180^\circ - 150^\circ = 30^\circ
    • sin⁡(−210∘)=+sin⁡(30∘)=12\sin(-210^\circ) = +\sin(30^\circ) = \frac{1}{2}
    • cos⁡(−210∘)=−cos⁡(30∘)=−32\cos(-210^\circ) = -\cos(30^\circ) = -\frac{\sqrt{3}}{2}
    • tan⁡(−210∘)=−tan⁡(30∘)=−13\tan(-210^\circ) = -\tan(30^\circ) = -\frac{1}{\sqrt{3}}
Coordinate Evaluation Examples
  • Point on Terminal Side: Let (−3,4)(-3, 4) lie on the terminal side of θ\theta:   x=−3,y=4,r=(−3)2+42=9+16=5x = -3, \quad y = 4, \quad r = \sqrt{(-3)^2 + 4^2} = \sqrt{9 + 16} = 5
    • sin⁡(θ)=yr=45\sin(\theta) = \frac{y}{r} = \frac{4}{5}
    • cos⁡(θ)=xr=−35\cos(\theta) = \frac{x}{r} = -\frac{3}{5}
    • tan⁡(θ)=yx=−43\tan(\theta) = \frac{y}{x} = -\frac{4}{3}
    • csc⁡(θ)=ry=54\csc(\theta) = \frac{r}{y} = \frac{5}{4}
    • sec⁡(θ)=rx=−53\sec(\theta) = \frac{r}{x} = -\frac{5}{3}
    • cot⁡(θ)=xy=−34\cot(\theta) = \frac{x}{y} = -\frac{3}{4}
  • Quadrant and Value Deduction: Given tan⁡(θ)=−43\tan(\theta) = -\frac{4}{3} and 0≤θ≤π0 \le \theta \le \pi:   Since tangent is negative, θ\theta must lie in Quadrant II. Thus, x=−3x = -3, y=4y = 4, and r=5r = 5, yielding the identical ratios as above.
  • Quadrant III Ratios: Let sin⁡(θ)=−715\sin(\theta) = -\frac{7}{15} with π≤θ≤3π2\pi \le \theta \le \frac{3\pi}{2}:   Here y=−7y = -7, r=15r = 15. Because θ\theta is in Quadrant III, x<0x < 0:   x=−r2−y2=−152−(−7)2=−225−49=−176x = -\sqrt{r^2 - y^2} = -\sqrt{15^2 - (-7)^2} = -\sqrt{225 - 49} = -\sqrt{176}
    • cos⁡(θ)=xr=−17615\cos(\theta) = \frac{x}{r} = -\frac{\sqrt{176}}{15}
    • tan⁡(θ)=yx=−7−176=7176\tan(\theta) = \frac{y}{x} = \frac{-7}{-\sqrt{176}} = \frac{7}{\sqrt{176}}
    • csc⁡(θ)=ry=−157\csc(\theta) = \frac{r}{y} = -\frac{15}{7}
    • sec⁡(θ)=rx=−15176\sec(\theta) = \frac{r}{x} = -\frac{15}{\sqrt{176}}
    • cot⁡(θ)=xy=1767\cot(\theta) = \frac{x}{y} = \frac{\sqrt{176}}{7}

Fundamental Trigonometric Identities and Analytic Simplification

An identity is an equation that remains true for all values of the variable for which the expressions are defined (e.g., x+3x+41=4x+41x + 3x + 41 = 4x + 41 is an identity). In contrast, a standard conditional equation holds true only for specific values (e.g., x+3x=2x+6x + 3x = 2x + 6 is true only when x=3x = 3).

Comprehensive Catalog of Fundamental Identities
Reciprocal Identities

sin⁡(θ)=1csc⁡(θ),csc⁡(θ)=1sin⁡(θ)\sin(\theta) = \frac{1}{\csc(\theta)}, \quad \csc(\theta) = \frac{1}{\sin(\theta)}cos⁡(θ)=1sec⁡(θ),sec⁡(θ)=1cos⁡(θ)\cos(\theta) = \frac{1}{\sec(\theta)}, \quad \sec(\theta) = \frac{1}{\cos(\theta)}tan⁡(θ)=1cot⁡(θ),cot⁡(θ)=1tan⁡(θ)\tan(\theta) = \frac{1}{\cot(\theta)}, \quad \cot(\theta) = \frac{1}{\tan(\theta)}

Quotient Identities

tan⁡(θ)=sin⁡(θ)cos⁡(θ),cot⁡(θ)=cos⁡(θ)sin⁡(θ)\tan(\theta) = \frac{\sin(\theta)}{\cos(\theta)}, \quad \cot(\theta) = \frac{\cos(\theta)}{\sin(\theta)}

Pythagorean Identities

sin⁡2(θ)+cos⁡2(θ)=1\sin^2(\theta) + \cos^2(\theta) = 11+tan⁡2(θ)=sec⁡2(θ)1 + \tan^2(\theta) = \sec^2(\theta)1+cot⁡2(θ)=csc⁡2(θ)1 + \cot^2(\theta) = \csc^2(\theta)

Even/Odd Identities

sin⁡(−u)=−sin⁡(u),csc⁡(−u)=−csc⁡(u)\sin(-u) = -\sin(u), \quad \csc(-u) = -\csc(u)cos⁡(−u)=cos⁡(u),sec⁡(−u)=sec⁡(u)\cos(-u) = \cos(u), \quad \sec(-u) = \sec(u)tan⁡(−u)=−tan⁡(u),cot⁡(−u)=−cot⁡(u)\tan(-u) = -\tan(u), \quad \cot(-u) = -\cot(u)

Angle Addition and Subtraction Identities

sin⁡(A+B)=sin⁡(A)cos⁡(B)+cos⁡(A)sin⁡(B)\sin(A + B) = \sin(A)\cos(B) + \cos(A)\sin(B)sin⁡(A−B)=sin⁡(A)cos⁡(B)−cos⁡(A)sin⁡(B)\sin(A - B) = \sin(A)\cos(B) - \cos(A)\sin(B)cos⁡(A+B)=cos⁡(A)cos⁡(B)−sin⁡(A)sin⁡(B)\cos(A + B) = \cos(A)\cos(B) - \sin(A)\sin(B)cos⁡(A−B)=cos⁡(A)cos⁡(B)+sin⁡(A)sin⁡(B)\cos(A - B) = \cos(A)\cos(B) + \sin(A)\sin(B)tan⁡(A+B)=tan⁡(A)+tan⁡(B)1−tan⁡(A)tan⁡(B)\tan(A + B) = \frac{\tan(A) + \tan(B)}{1 - \tan(A)\tan(B)}tan⁡(A−B)=tan⁡(A)−tan⁡(B)1+tan⁡(A)tan⁡(B)\tan(A - B) = \frac{\tan(A) - \tan(B)}{1 + \tan(A)\tan(B)}

Double-Angle Identities

sin⁡(2A)=2sin⁡(A)cos⁡(A)\sin(2A) = 2\sin(A)\cos(A)cos⁡(2A)=cos⁡2(A)−sin⁡2(A)=1−2sin⁡2(A)=2cos⁡2(A)−1\cos(2A) = \cos^2(A) - \sin^2(A) = 1 - 2\sin^2(A) = 2\cos^2(A) - 1tan⁡(2A)=2tan⁡(A)1−tan⁡2(A)\tan(2A) = \frac{2\tan(A)}{1 - \tan^2(A)}

Half-Angle Identities

sin⁡2(A2)=1−cos⁡(A)2\sin^2\left(\frac{A}{2}\right) = \frac{1 - \cos(A)}{2}cos⁡2(A2)=1+cos⁡(A)2\cos^2\left(\frac{A}{2}\right) = \frac{1 + \cos(A)}{2}tan⁡2(A2)=1−cos⁡(A)1+cos⁡(A)\tan^2\left(\frac{A}{2}\right) = \frac{1 - \cos(A)}{1 + \cos(A)}

Product-to-Sum Identities

sin⁡(A)cos⁡(B)=12[sin⁡(A+B)+sin⁡(A−B)]\sin(A)\cos(B) = \frac{1}{2}[\sin(A + B) + \sin(A - B)]sin⁡(A)sin⁡(B)=12[cos⁡(A−B)−cos⁡(A+B)]\sin(A)\sin(B) = \frac{1}{2}[\cos(A - B) - \cos(A + B)]cos⁡(A)cos⁡(B)=12[cos⁡(A−B)+cos⁡(A+B)]\cos(A)\cos(B) = \frac{1}{2}[\cos(A - B) + \cos(A + B)]

Sum-to-Product Identities

sin⁡(A)+sin⁡(B)=2sin⁡(A+B2)cos⁡(A−B2)\sin(A) + \sin(B) = 2\sin\left(\frac{A + B}{2}\right)\cos\left(\frac{A - B}{2}\right)sin⁡(A)−sin⁡(B)=2sin⁡(A−B2)cos⁡(A+B2)\sin(A) - \sin(B) = 2\sin\left(\frac{A - B}{2}\right)\cos\left(\frac{A + B}{2}\right)cos⁡(A)+cos⁡(B)=2cos⁡(A+B2)cos⁡(A−B2)\cos(A) + \cos(B) = 2\cos\left(\frac{A + B}{2}\right)\cos\left(\frac{A - B}{2}\right)cos⁡(A)−cos⁡(B)=−2sin⁡(A+B2)sin⁡(A−B2)\cos(A) - \cos(B) = -2\sin\left(\frac{A + B}{2}\right)\sin\left(\frac{A - B}{2}\right)

Analytical Examples and Identity Proofs
Exact Value of sin⁡(15∘)\sin(15^\circ)

sin⁡(15∘)=sin⁡(45∘−30∘)=sin⁡(45∘)cos⁡(30∘)−cos⁡(45∘)sin⁡(30∘)\sin(15^\circ) = \sin(45^\circ - 30^\circ) = \sin(45^\circ)\cos(30^\circ) - \cos(45^\circ)\sin(30^\circ)=(12)(32)−(12)(12)=3−122= \left(\frac{1}{\sqrt{2}}\right)\left(\frac{\sqrt{3}}{2}\right) - \left(\frac{1}{\sqrt{2}}\right)\left(\frac{1}{2}\right) = \frac{\sqrt{3} - 1}{2\sqrt{2}}

Compound Evaluation Problem

If sin⁡(A)=−13\sin(A) = -\frac{1}{3} and tan⁡(B)=512\tan(B) = \frac{5}{12}, where A,B∈[π2,3π2]A, B \in \left[\frac{\pi}{2}, \frac{3\pi}{2}\right], evaluate cos⁡(2A+B)\cos(2A + B).

  1. Determine Quadrants:
    • Interval is Quadrants II and III.
    • sin⁡(A)<0  ⟹  A\sin(A) < 0 \implies A is in Quadrant III: y=−1,r=3,x=−32−(−1)2=−22y = -1, r = 3, x = -\sqrt{3^2 - (-1)^2} = -2\sqrt{2}.      cos⁡(A)=−223\cos(A) = -\frac{2\sqrt{2}}{3}
    • tan⁡(B)>0  ⟹  B\tan(B) > 0 \implies B is in Quadrant III: x=−12,y=−5,r=(−12)2+(−5)2=13x = -12, y = -5, r = \sqrt{(-12)^2 + (-5)^2} = 13.      sin⁡(B)=−513,cos⁡(B)=−1213\sin(B) = -\frac{5}{13}, \quad \cos(B) = -\frac{12}{13}
  2. Evaluate Components:    cos⁡(2A)=2cos⁡2(A)−1=2(−223)2−1=2(89)−1=79\cos(2A) = 2\cos^2(A) - 1 = 2\left(-\frac{2\sqrt{2}}{3}\right)^2 - 1 = 2\left(\frac{8}{9}\right) - 1 = \frac{7}{9}sin⁡(2A)=2sin⁡(A)cos⁡(A)=2(−13)(−223)=429\sin(2A) = 2\sin(A)\cos(A) = 2\left(-\frac{1}{3}\right)\left(-\frac{2\sqrt{2}}{3}\right) = \frac{4\sqrt{2}}{9}
  3. Apply Addition Identity:    cos⁡(2A+B)=cos⁡(2A)cos⁡(B)−sin⁡(2A)sin⁡(B)\cos(2A + B) = \cos(2A)\cos(B) - \sin(2A)\sin(B)=(79)(−1213)−(429)(−513)=−84+202117=202−84117= \left(\frac{7}{9}\right)\left(-\frac{12}{13}\right) - \left(\frac{4\sqrt{2}}{9}\right)\left(-\frac{5}{13}\right) = \frac{-84 + 20\sqrt{2}}{117} = \frac{20\sqrt{2} - 84}{117}
Algebraic Simplification

Simplify sin⁡(2A)csc⁡(A)−cos⁡(2A)sec⁡(A)\sin(2A)\csc(A) - \cos(2A)\sec(A): =sin⁡(2A)sin⁡(A)−cos⁡(2A)cos⁡(A)=sin⁡(2A)cos⁡(A)−cos⁡(2A)sin⁡(A)sin⁡(A)cos⁡(A)= \frac{\sin(2A)}{\sin(A)} - \frac{\cos(2A)}{\cos(A)} = \frac{\sin(2A)\cos(A) - \cos(2A)\sin(A)}{\sin(A)\cos(A)} Applying the subtraction identity to the numerator: =sin⁡(2A−A)sin⁡(A)cos⁡(A)=sin⁡(A)sin⁡(A)cos⁡(A)=1cos⁡(A)=sec⁡(A)= \frac{\sin(2A - A)}{\sin(A)\cos(A)} = \frac{\sin(A)}{\sin(A)\cos(A)} = \frac{1}{\cos(A)} = \sec(A)

Verification of Identity: (sec⁡2(θ)−1)cos⁡2(θ)=sin⁡2(θ)(\sec^2(\theta) - 1)\cos^2(\theta) = \sin^2(\theta)

(sec⁡2(θ)−1)cos⁡2(θ)=tan⁡2(θ)cos⁡2(θ)=(sin⁡2(θ)cos⁡2(θ))cos⁡2(θ)=sin⁡2(θ)(\sec^2(\theta) - 1)\cos^2(\theta) = \tan^2(\theta)\cos^2(\theta) = \left(\frac{\sin^2(\theta)}{\cos^2(\theta)}\right)\cos^2(\theta) = \sin^2(\theta)

Identity Proof: sec⁡(x)−cos⁡(x)=tan⁡(x)sin⁡(x)\sec(x) - \cos(x) = \tan(x)\sin(x)

sec⁡(x)−cos⁡(x)=1cos⁡(x)−cos⁡(x)=1−cos⁡2(x)cos⁡(x)=sin⁡2(x)cos⁡(x)=(sin⁡(x)cos⁡(x))sin⁡(x)=tan⁡(x)sin⁡(x)\sec(x) - \cos(x) = \frac{1}{\cos(x)} - \cos(x) = \frac{1 - \cos^2(x)}{\cos(x)} = \frac{\sin^2(x)}{\cos(x)} = \left(\frac{\sin(x)}{\cos(x)}\right)\sin(x) = \tan(x)\sin(x)

Identity Proof: sin⁡(x+y)sin⁡(x−y)=sin⁡2(x)−sin⁡2(y)\sin(x + y)\sin(x - y) = \sin^2(x) - \sin^2(y)

sin⁡(x+y)sin⁡(x−y)=[sin⁡(x)cos⁡(y)+cos⁡(x)sin⁡(y)][sin⁡(x)cos⁡(y)−cos⁡(x)sin⁡(y)]\sin(x + y)\sin(x - y) = [\sin(x)\cos(y) + \cos(x)\sin(y)][\sin(x)\cos(y) - \cos(x)\sin(y)]=sin⁡2(x)cos⁡2(y)−cos⁡2(x)sin⁡2(y)= \sin^2(x)\cos^2(y) - \cos^2(x)\sin^2(y) Express completely in terms of sines using cos⁡2(θ)=1−sin⁡2(θ)\cos^2(\theta) = 1 - \sin^2(\theta): =sin⁡2(x)(1−sin⁡2(y))−(1−sin⁡2(x))sin⁡2(y)= \sin^2(x)(1 - \sin^2(y)) - (1 - \sin^2(x))\sin^2(y)=sin⁡2(x)−sin⁡2(x)sin⁡2(y)−sin⁡2(y)+sin⁡2(x)sin⁡2(y)=sin⁡2(x)−sin⁡2(y)= \sin^2(x) - \sin^2(x)\sin^2(y) - \sin^2(y) + \sin^2(x)\sin^2(y) = \sin^2(x) - \sin^2(y)

Exact Trigonometric Calculations Without a Calculator
  • Problem: If cos⁡(θ)=34\cos(\theta) = \frac{3}{4} and π≤θ≤2π\pi \le \theta \le 2\pi, find tan⁡(θ)\tan(\theta) and sin⁡(2θ)\sin(2\theta).   Since cos⁡(θ)>0\cos(\theta) > 0 and θ∈[π,2π]\theta \in [\pi, 2\pi], θ\theta lies strictly in Quadrant IV.   sin⁡(θ)=−1−cos⁡2(θ)=−1−916=−74\sin(\theta) = -\sqrt{1 - \cos^2(\theta)} = -\sqrt{1 - \frac{9}{16}} = -\frac{\sqrt{7}}{4}tan⁡(θ)=sin⁡(θ)cos⁡(θ)=−7434=−73\tan(\theta) = \frac{\sin(\theta)}{\cos(\theta)} = \frac{-\frac{\sqrt{7}}{4}}{\frac{3}{4}} = -\frac{\sqrt{7}}{3}sin⁡(2θ)=2sin⁡(θ)cos⁡(θ)=2(−74)(34)=−378\sin(2\theta) = 2\sin(\theta)\cos(\theta) = 2\left(-\frac{\sqrt{7}}{4}\right)\left(\frac{3}{4}\right) = -\frac{3\sqrt{7}}{8}

  • Problem: If tan⁡(x)=13\tan(x) = \frac{1}{3} and sec⁡(y)=1312\sec(y) = \frac{13}{12}, where xx and yy lie between π\pi and 2π2\pi, evaluate csc⁡(x−y)\csc(x - y) and cos⁡(2x)\cos(2x).

    1. Quadrant of xx: tan⁡(x)=13>0\tan(x) = \frac{1}{3} > 0 and x∈(π,2π)  ⟹  xx \in (\pi, 2\pi) \implies x is in Quadrant III.      xcoord=−3,ycoord=−1,r=(−3)2+(−1)2=10x_{\text{coord}} = -3, \quad y_{\text{coord}} = -1, \quad r = \sqrt{(-3)^2 + (-1)^2} = \sqrt{10}sin⁡(x)=−110,cos⁡(x)=−310\sin(x) = -\frac{1}{\sqrt{10}}, \quad \cos(x) = -\frac{3}{\sqrt{10}}
    2. Quadrant of yy: sec⁡(y)=1312>0  ⟹  cos⁡(y)=1213>0\sec(y) = \frac{13}{12} > 0 \implies \cos(y) = \frac{12}{13} > 0. For y∈(π,2π)y \in (\pi, 2\pi), yy is in Quadrant IV.      sin⁡(y)=−1−(1213)2=−513\sin(y) = -\sqrt{1 - \left(\frac{12}{13}\right)^2} = -\frac{5}{13}
    3. Evaluate sin⁡(x−y)\sin(x - y):      sin⁡(x−y)=sin⁡(x)cos⁡(y)−cos⁡(x)sin⁡(y)\sin(x - y) = \sin(x)\cos(y) - \cos(x)\sin(y)=(−110)(1213)−(−310)(−513)=−121310−151310=−271310= \left(-\frac{1}{\sqrt{10}}\right)\left(\frac{12}{13}\right) - \left(-\frac{3}{\sqrt{10}}\right)\left(-\frac{5}{13}\right) = -\frac{12}{13\sqrt{10}} - \frac{15}{13\sqrt{10}} = -\frac{27}{13\sqrt{10}}csc⁡(x−y)=1sin⁡(x−y)=−131027\csc(x - y) = \frac{1}{\sin(x - y)} = -\frac{13\sqrt{10}}{27}
    4. Evaluate cos⁡(2x)\cos(2x):      cos⁡(2x)=2cos⁡2(x)−1=2(−310)2−1=2(910)−1=1810−1=45\cos(2x) = 2\cos^2(x) - 1 = 2\left(-\frac{3}{\sqrt{10}}\right)^2 - 1 = 2\left(\frac{9}{10}\right) - 1 = \frac{18}{10} - 1 = \frac{4}{5}
  • Problem: Evaluate tan⁡(sin⁡−1(13))\tan\left(\sin^{-1}\left(\frac{1}{3}\right)\right).   Let θ=sin⁡−1(13)\theta = \sin^{-1}\left(\frac{1}{3}\right), so sin⁡(θ)=13\sin(\theta) = \frac{1}{3} with θ∈(0,π2)\theta \in \left(0, \frac{\pi}{2}\right).   Using a reference right triangle with opp=1\text{opp} = 1 and hyp=3\text{hyp} = 3:   adj=32−12=8=22\text{adj} = \sqrt{3^2 - 1^2} = \sqrt{8} = 2\sqrt{2}tan⁡(θ)=oppadj=122\tan(\theta) = \frac{\text{opp}}{\text{adj}} = \frac{1}{2\sqrt{2}}

Solving Trigonometric Equations

Systematic Solution Strategy
  1. Use trigonometric identities to write the equation in terms of a single trigonometric function.
  2. Isolate that function using algebraic operations (factoring, collecting terms, quadratic formula). Suppose sin⁡(x)=a\sin(x) = a.
  3. Ignore the algebraic sign of aa and solve sin⁡(x)=∣a∣\sin(x) = |a| to establish the acute reference angle x′∈[0,π2]x' \in \left[0, \frac{\pi}{2}\right].
  4. Use the original sign of aa and the CAST rule to identify all quadrants where the equation is satisfied.
  5. Compute all quadrant solutions within the specified interval.
Linear Equations
  • Solve: 2sin⁡(x)−1=02\sin(x) - 1 = 0 for x∈[0,2π]x \in [0, 2\pi]:   2sin⁡(x)=1  ⟹  sin⁡(x)=122\sin(x) = 1 \implies \sin(x) = \frac{1}{2}   Reference angle: x′=π6x' = \frac{\pi}{6}. Since sin⁡(x)\sin(x) is positive, solutions lie in Quadrants I and II:   x=π6,x=π−π6=5π6x = \frac{\pi}{6}, \quad x = \pi - \frac{\pi}{6} = \frac{5\pi}{6}

  • Solve: 2sin⁡(x)+1=02\sin(x) + 1 = 0 for x∈[0,2π]x \in [0, 2\pi]:   2sin⁡(x)=−1  ⟹  sin⁡(x)=−122\sin(x) = -1 \implies \sin(x) = -\frac{1}{2}   Reference angle: x′=π6x' = \frac{\pi}{6}. Since sin⁡(x)\sin(x) is negative, solutions lie in Quadrants III and IV:   x=π+π6=7π6,x=2π−π6=11π6x = \pi + \frac{\pi}{6} = \frac{7\pi}{6}, \quad x = 2\pi - \frac{\pi}{6} = \frac{11\pi}{6}

Quadratic-Type Trigonometric Equations

Trigonometric equations often appear in quadratic form au2+bu+c=0au^2 + bu + c = 0, where uu is a trigonometric function.

  • Solve: 2cos⁡2(x)=1−sin⁡(x)2\cos^2(x) = 1 - \sin(x) on [0,2π][0, 2\pi]:   Rewrite cos⁡2(x)\cos^2(x) as 1−sin⁡2(x)1 - \sin^2(x):   2(1−sin⁡2(x))=1−sin⁡(x)2(1 - \sin^2(x)) = 1 - \sin(x)2−2sin⁡2(x)=1−sin⁡(x)2 - 2\sin^2(x) = 1 - \sin(x)2sin⁡2(x)−sin⁡(x)−1=02\sin^2(x) - \sin(x) - 1 = 0   Factor the quadratic:   (2sin⁡(x)+1)(sin⁡(x)−1)=0(2\sin(x) + 1)(\sin(x) - 1) = 0   Set each factor to zero:

    1. 2sin⁡(x)+1=0  ⟹  sin⁡(x)=−12  ⟹  x=7π6,11π62\sin(x) + 1 = 0 \implies \sin(x) = -\frac{1}{2} \implies x = \frac{7\pi}{6}, \frac{11\pi}{6}
    2. sin⁡(x)−1=0  ⟹  sin⁡(x)=1  ⟹  x=π2\sin(x) - 1 = 0 \implies \sin(x) = 1 \implies x = \frac{\pi}{2}   Full solution set: x=π2,7π6,11π6x = \frac{\pi}{2}, \frac{7\pi}{6}, \frac{11\pi}{6}
  • Solve: sin⁡2(θ)+2cos⁡2(θ)=1\sin^2(\theta) + 2\cos^2(\theta) = 1 for 0≤θ≤2π0 \le \theta \le 2\pi:   Decompose the terms:   sin⁡2(θ)+cos⁡2(θ)+cos⁡2(θ)=1\sin^2(\theta) + \cos^2(\theta) + \cos^2(\theta) = 11+cos⁡2(θ)=1  ⟹  cos⁡2(θ)=0  ⟹  cos⁡(θ)=01 + \cos^2(\theta) = 1 \implies \cos^2(\theta) = 0 \implies \cos(\theta) = 0   Within [0,2π][0, 2\pi]:   θ=π2,3π2\theta = \frac{\pi}{2}, \frac{3\pi}{2}

  • Solve: 5cos⁡(x)−2sin⁡2(x)=15\cos(x) - 2\sin^2(x) = 1 on [0,2π][0, 2\pi]:   Substitute sin⁡2(x)=1−cos⁡2(x)\sin^2(x) = 1 - \cos^2(x):   5cos⁡(x)−2(1−cos⁡2(x))=15\cos(x) - 2(1 - \cos^2(x)) = 15cos⁡(x)−2+2cos⁡2(x)=15\cos(x) - 2 + 2\cos^2(x) = 12cos⁡2(x)+5cos⁡(x)−3=02\cos^2(x) + 5\cos(x) - 3 = 0   Factor the quadratic expression:   (2cos⁡(x)−1)(cos⁡(x)+3)=0(2\cos(x) - 1)(\cos(x) + 3) = 0   Setting each factor to zero:

    1. cos⁡(x)+3=0  ⟹  cos⁡(x)=−3\cos(x) + 3 = 0 \implies \cos(x) = -3 (No solution, since −1≤cos⁡(x)≤1-1 \le \cos(x) \le 1).
    2. 2cos⁡(x)−1=0  ⟹  cos⁡(x)=122\cos(x) - 1 = 0 \implies \cos(x) = \frac{1}{2}.      Within [0,2π][0, 2\pi], cosine is positive in Quadrants I and IV:      x=π3,x=2π−π3=5π3x = \frac{\pi}{3}, \quad x = 2\pi - \frac{\pi}{3} = \frac{5\pi}{3}
Multiple-Angle Equations
  • Solve: 2cos⁡(3t)−1=02\cos(3t) - 1 = 0 where t∈[0,2π]t \in [0, 2\pi]:   2cos⁡(3t)=1  ⟹  cos⁡(3t)=122\cos(3t) = 1 \implies \cos(3t) = \frac{1}{2}   If t∈[0,2π]t \in [0, 2\pi], the argument 3t3t spans three full revolutions: 3t∈[0,6π]3t \in [0, 6\pi].   The reference angle is π3\frac{\pi}{3}. In Quadrants I and IV:
    • Cycle 1 ([0,2π][0, 2\pi]): 3t=π3,5π33t = \frac{\pi}{3}, \frac{5\pi}{3}
    • Cycle 2 ([2π,4π][2\pi, 4\pi]): 3t=2π+π3=7π3,3t=4π−π3=11π33t = 2\pi + \frac{\pi}{3} = \frac{7\pi}{3}, \quad 3t = 4\pi - \frac{\pi}{3} = \frac{11\pi}{3}
    • Cycle 3 ([4π,6π][4\pi, 6\pi]): 3t=4π+π3=13π3,3t=6π−π3=17π33t = 4\pi + \frac{\pi}{3} = \frac{13\pi}{3}, \quad 3t = 6\pi - \frac{\pi}{3} = \frac{17\pi}{3}   Dividing each value by 3:   t=π9,5π9,7π9,11π9,13π9,17π9t = \frac{\pi}{9}, \frac{5\pi}{9}, \frac{7\pi}{9}, \frac{11\pi}{9}, \frac{13\pi}{9}, \frac{17\pi}{9}
Equations Involving Inverse Trigonometric Functions
  • Solve: sec⁡2(x)−2tan⁡(x)=4\sec^2(x) - 2\tan(x) = 4 on [0,2π][0, 2\pi]:   Apply the Pythagorean identity sec⁡2(x)=1+tan⁡2(x)\sec^2(x) = 1 + \tan^2(x):   1+tan⁡2(x)−2tan⁡(x)−4=01 + \tan^2(x) - 2\tan(x) - 4 = 0tan⁡2(x)−2tan⁡(x)−3=0\tan^2(x) - 2\tan(x) - 3 = 0   Factor:   (tan⁡(x)−3)(tan⁡(x)+1)=0(\tan(x) - 3)(\tan(x) + 1) = 0
    1. tan⁡(x)=−1\tan(x) = -1:      Reference angle is π4\frac{\pi}{4}. Tangent is negative in Quadrants II and IV:      x=3π4,7π4x = \frac{3\pi}{4}, \frac{7\pi}{4}
    2. tan⁡(x)=3\tan(x) = 3:      Since 3 is not a special triangle ratio, use the inverse tangent function: x′=arctan⁡(3)x' = \arctan(3). Tangent is positive in Quadrants I and III:      x=arctan⁡(3),x=π+arctan⁡(3)x = \arctan(3), \quad x = \pi + \arctan(3)

Graphs of Trigonometric and Damped Functions

Properties of Parent Sine and Cosine Curves
CharacteristicParent Sine: y=sin⁡(x)y = \sin(x)Parent Cosine: y=cos⁡(x)y = \cos(x)
DomainR\mathbb{R} ((−∞,∞)(-\infty, \infty))R\mathbb{R} ((−∞,∞)(-\infty, \infty))
Range[−1,1][-1, 1][−1,1][-1, 1]
Period2π2\pi2π2\pi
Mapping PropertyNot one-to-one; Onto [−1,1][-1, 1]Not one-to-one; Onto [−1,1][-1, 1]
SymmetryOrigin symmetry (Odd function: sin⁡(−x)=−sin⁡(x)\sin(-x) = -\sin(x))yy-axis symmetry (Even function: cos⁡(−x)=cos⁡(x)\cos(-x) = \cos(x))
ContinuityContinuous on all of R\mathbb{R}Continuous on all of R\mathbb{R}

To graph one full cycle of a basic curve over [0,2π][0, 2\pi], use the five key points:

  • For y=sin⁡(x)y = \sin(x):
    • Intercept: (0,0)(0, 0)
    • Maximum: (π2,1)\left(\frac{\pi}{2}, 1\right)
    • Intercept: (π,0)(\pi, 0)
    • Minimum: (3π2,−1)\left(\frac{3\pi}{2}, -1\right)
    • Intercept: (2π,0)(2\pi, 0)
  • For y=cos⁡(x)y = \cos(x):
    • Maximum: (0,1)(0, 1)
    • Intercept: (π2,0)\left(\frac{\pi}{2}, 0\right)
    • Minimum: (π,−1)(\pi, -1)
    • Intercept: (3π2,0)\left(\frac{3\pi}{2}, 0\right)
    • Maximum: (2π,1)(2\pi, 1)
Transformations: Amplitude, Period, and Translations

For general sine and cosine curves: y=d+asin⁡(bx−c)andy=d+acos⁡(bx−c)y = d + a\sin(bx - c) \quad \text{and} \quad y = d + a\cos(bx - c)

  • Amplitude: ∣a∣|a|. When ∣a∣>1|a| > 1, the graph undergoes vertical stretching; when ∣a∣<1|a| < 1, it undergoes vertical shrinking. The range for d=0d = 0 is [−∣a∣,∣a∣][-|a|, |a|].
  • Reflection: If a<0a < 0, the curve reflects across the horizontal midline y=dy = d.
  • Period: If b>0b > 0, the period is 2πb\frac{2\pi}{b}. When 0<b<10 < b < 1, the curve undergoes horizontal stretching (period >2π> 2\pi). When b>1b > 1, it undergoes horizontal compression (period <2π< 2\pi). If b<0b < 0, use even/odd identities to rewrite before graphing.
  • Phase Shift (Horizontal Translation): The expression bx−cbx - c completes one full period from bx−c=0bx - c = 0 to bx−c=2πbx - c = 2\pi, so:   x=cbtox=cb+2πbx = \frac{c}{b} \quad \text{to} \quad x = \frac{c}{b} + \frac{2\pi}{b}   The shift amount is cb\frac{c}{b}.
  • Vertical Shift: dd. Shifts the baseline midline of oscillation to y=dy = d.
Transformation Examples
  • Scale Adjustment: Graph g(x)=2sin⁡(x)g(x) = 2\sin(x) on [−π,4π][-\pi, 4\pi]:   The amplitude is 2, period is 2π2\pi. Key points on [0,2π][0, 2\pi] have twice the height of parent sine:   (0,0),(π2,2),(π,0),(3π2,−2),(2π,0)(0, 0), \left(\frac{\pi}{2}, 2\right), (\pi, 0), \left(\frac{3\pi}{2}, -2\right), (2\pi, 0)
  • Comparative Amplitudes: Compare y=12cos⁡(x)y = \frac{1}{2}\cos(x) and y=3cos⁡(x)y = 3\cos(x):
    • y=12cos⁡(x)y = \frac{1}{2}\cos(x) has amplitude 12\frac{1}{2}, maximum value 12\frac{1}{2}, minimum value −12-\frac{1}{2}. Key points: (0,12),(π2,0),(π,−12),(3π2,0),(2π,12)\left(0, \frac{1}{2}\right), \left(\frac{\pi}{2}, 0\right), \left(\pi, -\frac{1}{2}\right), \left(\frac{3\pi}{2}, 0\right), \left(2\pi, \frac{1}{2}\right).
    • y=3cos⁡(x)y = 3\cos(x) has amplitude 3, maximum value 3, minimum value −3-3. Key points: (0,3),(π2,0),(π,−3),(3π2,0),(2π,3)(0, 3), \left(\frac{\pi}{2}, 0\right), (\pi, -3), \left(\frac{3\pi}{2}, 0\right), (2\pi, 3).
    • The graph of y=−3cos⁡(x)y = -3\cos(x) is the exact vertical reflection of y=3cos⁡(x)y = 3\cos(x) across the xx-axis.
  • Horizontal Translation Analysis: For a curve with period 2π2\pi shifted by phase shift π3\frac{\pi}{3}, the interval [π3,7π3]\left[\frac{\pi}{3}, \frac{7\pi}{3}\right] forms one complete cycle. Dividing into four quarters yields the key points:   (π3,0),(5π6,max),(4π3,0),(11π6,min),(7π3,0)\left(\frac{\pi}{3}, 0\right), \left(\frac{5\pi}{6}, \text{max}\right), \left(\frac{4\pi}{3}, 0\right), \left(\frac{11\pi}{6}, \text{min}\right), \left(\frac{7\pi}{3}, 0\right)
Graphs of Tangent and Cotangent Functions
  • Tangent: y=tan⁡(x)=sin⁡(x)cos⁡(x)y = \tan(x) = \frac{\sin(x)}{\cos(x)}

    • Odd function (tan⁡(−x)=−tan⁡(x)\tan(-x) = -\tan(x)), origin symmetric.
    • Undefined when cos⁡(x)=0  ⟹  \cos(x) = 0 \implies Vertical asymptotes at x=π2+nπ,n∈Zx = \frac{\pi}{2} + n\pi, n \in \mathbb{Z}.
    • Domain: all real numbers x≠π2+nπx \ne \frac{\pi}{2} + n\pi.
    • Range: (−∞,∞)(-\infty, \infty).
    • Period: π\pi.
    • As x→(π2)−x \to \left(\frac{\pi}{2}\right)^-, tan⁡(x)→∞\tan(x) \to \infty; as x→(−π2)+x \to \left(-\frac{\pi}{2}\right)^+, tan⁡(x)→−∞\tan(x) \to -\infty.
    • Example: For f(x)=tan⁡(x2)f(x) = \tan\left(\frac{x}{2}\right), consecutive vertical asymptotes occur where x2=−π2\frac{x}{2} = -\frac{\pi}{2} and x2=π2  ⟹  x=−π\frac{x}{2} = \frac{\pi}{2} \implies x = -\pi and x=πx = \pi. The period is 2π2\pi.
  • Cotangent: y=cot⁡(x)=cos⁡(x)sin⁡(x)y = \cot(x) = \frac{\cos(x)}{\sin(x)}

    • Odd function, origin symmetric.
    • Undefined when sin⁡(x)=0  ⟹  \sin(x) = 0 \implies Vertical asymptotes at x=nπ,n∈Zx = n\pi, n \in \mathbb{Z}.
    • Domain: all real numbers x≠nπx \ne n\pi.
  • Range: (−∞,∞)(-\infty, \infty).

  • Period: π\pi.

  • xx-intercepts: (π2+nπ,0)\left(\frac{\pi}{2} + n\pi, 0\right).

  • Example: For y=2cot⁡(x3)y = 2\cot\left(\frac{x}{3}\right), consecutive vertical asymptotes occur where x3=0\frac{x}{3} = 0 and x3=π  ⟹  x=0\frac{x}{3} = \pi \implies x = 0 and x=3πx = 3\pi. Period is 3π3\pi.

Graphs of Secant and Cosecant Functions

Secant and cosecant curves are constructed directly from reciprocal curves:

  • Secant: y=sec⁡(x)=1cos⁡(x)y = \sec(x) = \frac{1}{\cos(x)}
    • Vertical asymptotes wherever cos⁡(x)=0  ⟹  x=π2+nπ\cos(x) = 0 \implies x = \frac{\pi}{2} + n\pi.
    • Domain: all real numbers x≠π2+nπx \ne \frac{\pi}{2} + n\pi.
    • Range: (−∞,−1]∪[1,∞)(-\infty, -1] \cup [1, \infty).
    • Period: 2π2\pi.
    • Even function, symmetric about the yy-axis.
  • Cosecant: y=csc⁡(x)=1sin⁡(x)y = \csc(x) = \frac{1}{\sin(x)}
    • Vertical asymptotes wherever sin⁡(x)=0  ⟹  x=nπ\sin(x) = 0 \implies x = n\pi.
    • Domain: all real numbers x≠nπx \ne n\pi.
  • Range: (−∞,−1]∪[1,∞)(-\infty, -1] \cup [1, \infty).
  • Period: 2π2\pi.
  • Odd function, symmetric about the origin.
  • To graph y=acsc⁡(bx−c)y = a\csc(bx - c), first graph the auxiliary curve y=asin⁡(bx−c)y = a\sin(bx - c). The vertical asymptotes of the cosecant function occur exactly at the xx-intercepts (midline crossings) of the sine wave, while the peaks of the sine wave correspond to the local minima of the cosecant curve, and troughs correspond to local maxima.
Damped Trigonometric Graphs

A damped trigonometric function is the product of an oscillating trigonometric term and another damping factor: f(x)=g(x)sin⁡(bx)f(x) = g(x)\sin(bx).

  • Analysis of f(x)=xsin⁡(x)f(x) = x\sin(x):
    • The factor xx is the damping factor.
    • Because ∣sin⁡(x)∣≤1|\sin(x)| \le 1, we have ∣xsin⁡(x)∣≤∣x∣  ⟹  −∣x∣≤xsin⁡(x)≤∣x∣|x\sin(x)| \le |x| \implies -|x| \le x\sin(x) \le |x|.
    • The graph is bounded between the lines y=−xy = -x and y=xy = x.
    • The curve touches y=±xy = \pm x wherever sin⁡(x)=±1\sin(x) = \pm 1, which occurs at x=π2+nπx = \frac{\pi}{2} + n\pi.
    • The curve has xx-intercepts wherever sin⁡(x)=0\sin(x) = 0, which occurs at x=nπx = n\pi.
  • Analysis of f(x)=e−xsin⁡(3x)f(x) = e^{-x}\sin(3x):
    • Domain: (−∞,∞)(-\infty, \infty).
    • Because e−x>0e^{-x} > 0 and ∣sin⁡(3x)∣≤1|\sin(3x)| \le 1, the inequality holds:     −e−x≤e−xsin⁡(3x)≤e−x-e^{-x} \le e^{-x}\sin(3x) \le e^{-x}
    • The graph oscillates between the bounding curves y=−e−xy = -e^{-x} and y=e−xy = e^{-x}.
    • The curve touches the envelope curves y=±e−xy = \pm e^{-x} when sin⁡(3x)=±1\sin(3x) = \pm 1:     3x=π2+nπ  ⟹  x=π6+nπ33x = \frac{\pi}{2} + n\pi \implies x = \frac{\pi}{6} + \frac{n\pi}{3}
    • The xx-intercepts occur when sin⁡(3x)=0\sin(3x) = 0:     3x=nπ  ⟹  x=nπ33x = n\pi \implies x = \frac{n\pi}{3}

Functions, Compositions, and Transformations

Function Classifications and Behavior
  • Function 1: f(x)=x2−10x+1f(x) = x^2 - 10x + 1

    • One-to-One: No. As an upward-opening parabola with vertex at x=−−102(1)=5x = -\frac{-10}{2(1)} = 5, it fails the horizontal line test (e.g., f(0)=1f(0) = 1 and f(10)=1f(10) = 1).
    • Even/Odd: Neither. f(−x)=(−x)2−10(−x)+1=x2+10x+1≠f(x)f(-x) = (-x)^2 - 10(-x) + 1 = x^2 + 10x + 1 \ne f(x) and ≠−f(x)\ne -f(x).
    • Periodicity: Not periodic.
    • Intervals of Monotonicity:
    • Interval of decrease: (−∞,5)(-\infty, 5)
    • Interval of increase: (5,∞)(5, \infty)
  • Function 2: f(x)=−sin⁡(2x)f(x) = -\sin(2x) on the restricted domain x∈(−π,π)x \in (-\pi, \pi)

    • One-to-One: No. It oscillates and takes the same values multiple times.
    • Even/Odd: Odd. f(−x)=−sin⁡(2(−x))=−sin⁡(−2x)=sin⁡(2x)=−f(x)f(-x) = -\sin(2(-x)) = -\sin(-2x) = \sin(2x) = -f(x).
    • Periodicity: Not periodic on a bounded domain (periodic with period π\pi only when defined on R\mathbb{R}).
    • Intervals of Monotonicity: Analyzed via f′(x)=−2cos⁡(2x)f'(x) = -2\cos(2x). Critical points occur where cos⁡(2x)=0  ⟹  x=−3π4,−π4,π4,3π4\cos(2x) = 0 \implies x = -\frac{3\pi}{4}, -\frac{\pi}{4}, \frac{\pi}{4}, \frac{3\pi}{4}.
    • Intervals of increase (f′(x)>0f'(x) > 0): (−3π4,−π4)\left(-\frac{3\pi}{4}, -\frac{\pi}{4}\right) and (π4,3π4)\left(\frac{\pi}{4}, \frac{3\pi}{4}\right)
    • Intervals of decrease (f′(x)<0f'(x) < 0): (−π,−3π4)\left(-\pi, -\frac{3\pi}{4}\right), (−π4,π4)\left(-\frac{\pi}{4}, \frac{\pi}{4}\right), and (3π4,π)\left(\frac{3\pi}{4}, \pi\right)
  • Function 3: f(x)=ln⁡(2x−2)−5f(x) = \ln(2x - 2) - 5

    • Domain: 2x−2>0  ⟹  x>12x - 2 > 0 \implies x > 1, or (1,∞)(1, \infty).
    • One-to-One: Yes. Its derivative f′(x)=22x−2=1x−1>0f'(x) = \frac{2}{2x - 2} = \frac{1}{x - 1} > 0 for all x>1x > 1, meaning ff is strictly monotonic.
    • Even/Odd: Neither. The domain is not symmetric about the origin.
    • Periodicity: Not periodic.
    • Interval of Increase: (1,∞)(1, \infty)
Inverse Functions, Domains, and Ranges

To find an inverse formula f−1(x)f^{-1}(x), solve the relation y=f(x)y = f(x) for xx in terms of yy, then swap variables. The fundamental properties dictate: domain(f−1)=range(f)andrange(f−1)=domain(f)\text{domain}(f^{-1}) = \text{range}(f) \quad \text{and} \quad \text{range}(f^{-1}) = \text{domain}(f)

  • Rational Function: f(x)=3x+2−x+9f(x) = \frac{3x + 2}{-x + 9}

    • Set y=3x+2−x+9y = \frac{3x + 2}{-x + 9}
    • Solve for xx:     y(−x+9)=3x+2y(-x + 9) = 3x + 2−xy+9y=3x+2-xy + 9y = 3x + 29y−2=3x+xy=x(3+y)9y - 2 = 3x + xy = x(3 + y)x=9y−23+yx = \frac{9y - 2}{3 + y}
    • Swap variables:     f−1(x)=9x−23+xf^{-1}(x) = \frac{9x - 2}{3 + x}
    • Domain and Range:     domain(f)=range(f−1)=(−∞,9)∪(9,∞)\text{domain}(f) = \text{range}(f^{-1}) = (-\infty, 9) \cup (9, \infty)domain(f−1)=range(f)=(−∞,−3)∪(−3,∞)\text{domain}(f^{-1}) = \text{range}(f) = (-\infty, -3) \cup (-3, \infty)
  • Radical Function: f(x)=20x−5f(x) = \sqrt{20x - 5}

    • The expression inside the radical must be non-negative: 20x−5≥0  ⟹  x≥1420x - 5 \ge 0 \implies x \ge \frac{1}{4}.
    • The principal square root yields non-negative values: y≥0y \ge 0.
    • Set y=20x−5  ⟹  y2=20x−5  ⟹  x=120(y2+5)y = \sqrt{20x - 5} \implies y^2 = 20x - 5 \implies x = \frac{1}{20}(y^2 + 5).
    • Swap variables:     f−1(x)=120(x2+5)f^{-1}(x) = \frac{1}{20}(x^2 + 5)
    • Domain and Range:     domain(f)=range(f−1)=[14,∞)\text{domain}(f) = \text{range}(f^{-1}) = \left[\frac{1}{4}, \infty\right)domain(f−1)=range(f)=[0,∞)\text{domain}(f^{-1}) = \text{range}(f) = [0, \infty)
Function Graphing via Transformations
  • Transforming Square Root: y=2x+4−2y = \sqrt{2x + 4} - 2

    • Rewrite into standard form: y=2(x+2)−2y = \sqrt{2(x + 2)} - 2.
    • Parent function: y=xy = \sqrt{x}.
    • Transformation sequence:
    1. Horizontal compression by a factor of 12\frac{1}{2}.
    2. Horizontal translation left by 2 units.
    3. Vertical translation down by 2 units.
    • Endpoint shifts from (0,0)(0, 0) to (−2,−2)(-2, -2). The yy-intercept occurs at (0,0)(0, 0) because y=4−2=0y = \sqrt{4} - 2 = 0.
  • Transforming Exponential: y=ex−2+1y = e^{x - 2} + 1

    • Parent function: y=exy = e^x.
    • Transformation sequence:
    1. Horizontal translation right by 2 units.
    2. Vertical translation up by 1 unit.
    • The horizontal asymptote shifts from y=0y = 0 to y=1y = 1.
    • The characteristic anchor point (0,1)(0, 1) maps to (2,2)(2, 2).
Function Combinations and Compositions

Let f(x)=1xf(x) = \frac{1}{x} and g(x)=sin⁡(3x)−x+1g(x) = \sin(3x) - \sqrt{x + 1}.

  • Sum: (f+g)(x)=1x+sin⁡(3x)−x+1(f + g)(x) = \frac{1}{x} + \sin(3x) - \sqrt{x + 1}
  • Product: (fg)(x)=sin⁡(3x)−x+1x(fg)(x) = \frac{\sin(3x) - \sqrt{x + 1}}{x}
  • Composition (g∘f)(x)(g \circ f)(x): Substitute f(x)f(x) into gg:   (g∘f)(x)=g(f(x))=sin⁡(3(1x))−1x+1=sin⁡(3x)−1x+1(g \circ f)(x) = g(f(x)) = \sin\left(3\left(\frac{1}{x}\right)\right) - \sqrt{\frac{1}{x} + 1} = \sin\left(\frac{3}{x}\right) - \sqrt{\frac{1}{x} + 1}
  • Composition (f∘g)(x)(f \circ g)(x): Substitute g(x)g(x) into ff:   (f∘g)(x)=f(g(x))=1sin⁡(3x)−x+1(f \circ g)(x) = f(g(x)) = \frac{1}{\sin(3x) - \sqrt{x + 1}}
Logarithmic and Exponential Equations and Inequalities
  • Logarithmic Equation: log⁡(x+1)+log⁡(x−2)=1\log(x + 1) + \log(x - 2) = 1

    • Domain constraints: x+1>0  ⟹  x>−1x + 1 > 0 \implies x > -1, and x−2>0  ⟹  x>2x - 2 > 0 \implies x > 2. Joint restriction: x>2x > 2.
    • Use log product rule:     log⁡((x+1)(x−2))=1\log((x + 1)(x - 2)) = 1(x+1)(x−2)=101=10(x + 1)(x - 2) = 10^1 = 10x2−x−2=10  ⟹  x2−x−12=0x^2 - x - 2 = 10 \implies x^2 - x - 12 = 0(x−4)(x+3)=0(x - 4)(x + 3) = 0
    • Potential solutions: x=4x = 4 or x=−3x = -3.
    • Since x>2x > 2, discard x=−3x = -3. The only valid solution is x=4x = 4.
  • Exponential Inequality: ex+5>1e^{x + 5} > 1

    • Take the natural logarithm of both sides (a strictly increasing operation):     ln⁡(ex+5)>ln⁡(1)\ln(e^{x + 5}) > \ln(1)x+5>0  ⟹  x>−5x + 5 > 0 \implies x > -5

Limits and Asymptotic Behavior

Analytical Limits (Without L'Hôpital's Rule)
  • Limit with Nonzero Denominator:   lim⁡h→0h2+15−h+15h+3−2\lim_{h \to 0} \frac{\sqrt{h^2 + 15} - \sqrt{h + 15}}{\sqrt{h + 3} - 2}   Direct substitution yields:   0+15−0+150+3−2=03−2=0\frac{\sqrt{0 + 15} - \sqrt{0 + 15}}{\sqrt{0 + 3} - 2} = \frac{0}{\sqrt{3} - 2} = 0

  • Limit by Dual Conjugate Rationalization:   lim⁡h→1h2+15−h+15h+3−2\lim_{h \to 1} \frac{\sqrt{h^2 + 15} - \sqrt{h + 15}}{\sqrt{h + 3} - 2}   Direct substitution gives the indeterminate form 00\frac{0}{0}. Multiply numerator and denominator simultaneously by their conjugates:   (h2+15−h+15)(h2+15+h+15)(h+3+2)(h+3−2)(h+3+2)(h2+15+h+15)\frac{(\sqrt{h^2 + 15} - \sqrt{h + 15})(\sqrt{h^2 + 15} + \sqrt{h + 15})(\sqrt{h + 3} + 2)}{(\sqrt{h + 3} - 2)(\sqrt{h + 3} + 2)(\sqrt{h^2 + 15} + \sqrt{h + 15})}=[(h2+15)−(h+15)](h+3+2)[(h+3)−4](h2+15+h+15)= \frac{[(h^2 + 15) - (h + 15)](\sqrt{h + 3} + 2)}{[(h + 3) - 4](\sqrt{h^2 + 15} + \sqrt{h + 15})}=(h2−h)(h+3+2)(h−1)(h2+15+h+15)=h(h−1)(h+3+2)(h−1)(h2+15+h+15)= \frac{(h^2 - h)(\sqrt{h + 3} + 2)}{(h - 1)(\sqrt{h^2 + 15} + \sqrt{h + 15})} = \frac{h(h - 1)(\sqrt{h + 3} + 2)}{(h - 1)(\sqrt{h^2 + 15} + \sqrt{h + 15})}   Cancel the (h−1)(h - 1) factor and evaluate at h=1h = 1:   1(1+3+2)16+16=1(2+2)4+4=48=12\frac{1(\sqrt{1 + 3} + 2)}{\sqrt{16} + \sqrt{16}} = \frac{1(2 + 2)}{4 + 4} = \frac{4}{8} = \frac{1}{2}

  • Limit by Quadratic Factoring:   lim⁡x→2x2−3x+22x2−3x−2\lim_{x \to 2} \frac{x^2 - 3x + 2}{2x^2 - 3x - 2}   Factor both polynomials:   (x−2)(x−1)(x−2)(2x+1)\frac{(x - 2)(x - 1)}{(x - 2)(2x + 1)}   Cancel the (x−2)(x - 2) factor for x≠2x \ne 2:   lim⁡x→2x−12x+1=2−12(2)+1=15\lim_{x \to 2} \frac{x - 1}{2x + 1} = \frac{2 - 1}{2(2) + 1} = \frac{1}{5}

  • Difference of Squares Limit:   lim⁡h→0(h+4)2−16h=lim⁡h→0h2+8h+16−16h=lim⁡h→0h(h+8)h=lim⁡h→0(h+8)=8\lim_{h \to 0} \frac{(h + 4)^2 - 16}{h} = \lim_{h \to 0} \frac{h^2 + 8h + 16 - 16}{h} = \lim_{h \to 0} \frac{h(h + 8)}{h} = \lim_{h \to 0} (h + 8) = 8

  • Direct Polynomial Substitution:   lim⁡x→1x4−3x2+10x2+2x+1=14−3(12)+1012+2(1)+1=84=2\lim_{x \to 1} \frac{x^4 - 3x^2 + 10}{x^2 + 2x + 1} = \frac{1^4 - 3(1^2) + 10}{1^2 + 2(1) + 1} = \frac{8}{4} = 2

  • Piecewise Limit Involving Absolute Value:   lim⁡x→1∣x−1∣x2−1=lim⁡x→1∣x−1∣(x−1)(x+1)\lim_{x \to 1} \frac{|x - 1|}{x^2 - 1} = \lim_{x \to 1} \frac{|x - 1|}{(x - 1)(x + 1)}

    • Left-Hand Limit (x→1−x \to 1^-): Here x−1<0  ⟹  ∣x−1∣=−(x−1)x - 1 < 0 \implies |x - 1| = -(x - 1).     lim⁡x→1−−(x−1)(x−1)(x+1)=lim⁡x→1−−1x+1=−12\lim_{x \to 1^-} \frac{-(x - 1)}{(x - 1)(x + 1)} = \lim_{x \to 1^-} \frac{-1}{x + 1} = -\frac{1}{2}
    • Right-Hand Limit (x→1+x \to 1^+): Here x−1>0  ⟹  ∣x−1∣=x−1x - 1 > 0 \implies |x - 1| = x - 1.     lim⁡x→1+x−1(x−1)(x+1)=lim⁡x→1+1x+1=12\lim_{x \to 1^+} \frac{x - 1}{(x - 1)(x + 1)} = \lim_{x \to 1^+} \frac{1}{x + 1} = \frac{1}{2}
    • Conclusion: Since LHL=−12≠RHL=12\text{LHL} = -\frac{1}{2} \ne \text{RHL} = \frac{1}{2}, the two-sided limit Does Not Exist (DNE).
  • Limit by Squeeze Theorem (Exponential and Cosine):   lim⁡x→0(x8+x2)ecos⁡(x+1x6)\lim_{x \to 0} (x^8 + x^2)e^{\cos\left(\frac{x + 1}{x^6}\right)}   Because the cosine function is bounded, −1≤cos⁡(x+1x6)≤1-1 \le \cos\left(\frac{x + 1}{x^6}\right) \le 1, we have:   e−1≤ecos⁡(x+1x6)≤e1e^{-1} \le e^{\cos\left(\frac{x + 1}{x^6}\right)} \le e^1   Since x8+x2≥0x^8 + x^2 \ge 0 for all real xx:   (x8+x2)e−1≤(x8+x2)ecos⁡(x+1x6)≤(x8+x2)e(x^8 + x^2)e^{-1} \le (x^8 + x^2)e^{\cos\left(\frac{x + 1}{x^6}\right)} \le (x^8 + x^2)e   Evaluate bounding limits as x→0x \to 0:   lim⁡x→0(x8+x2)e−1=0andlim⁡x→0(x8+x2)e=0\lim_{x \to 0} (x^8 + x^2)e^{-1} = 0 \quad \text{and} \quad \lim_{x \to 0} (x^8 + x^2)e = 0   By the Squeeze Theorem, the limit is 00.

  • Limit by Squeeze Theorem (Logarithmic Argument):   lim⁡x→0+sin⁡(ln⁡(x))ln⁡(x)\lim_{x \to 0^+} \frac{\sin(\ln(x))}{\ln(x)}   Let u=ln⁡(x)u = \ln(x). As x→0+x \to 0^+, u→−∞u \to -\infty. We analyze:   lim⁡u→−∞sin⁡(u)u\lim_{u \to -\infty} \frac{\sin(u)}{u}   Since −1≤sin⁡(u)≤1-1 \le \sin(u) \le 1, dividing by u<0u < 0 reverses the inequalities:   1u≤sin⁡(u)u≤−1u\frac{1}{u} \le \frac{\sin(u)}{u} \le -\frac{1}{u}   As u→−∞u \to -\infty, 1u→0\frac{1}{u} \to 0 and −1u→0-\frac{1}{u} \to 0.   By the Squeeze Theorem, the limit is 00.

  • Limit at Negative Infinity Involving Radicals:   lim⁡x→−∞4x2−x+1−2x3x+2\lim_{x \to -\infty} \frac{\sqrt{4x^2 - x + 1} - 2x}{3x + 2}   For x<0x < 0, x2=∣x∣=−x\sqrt{x^2} = |x| = -x. Factor x2x^2 from the radicand:   4x2−x+1=x2(4−1x+1x2)=−x4−1x+1x2\sqrt{4x^2 - x + 1} = \sqrt{x^2\left(4 - \frac{1}{x} + \frac{1}{x^2}\right)} = -x\sqrt{4 - \frac{1}{x} + \frac{1}{x^2}}   The expression becomes:   −x4−1x+1x2−2xx(3+2x)=x(−4−1x+1x2−2)x(3+2x)\frac{-x\sqrt{4 - \frac{1}{x} + \frac{1}{x^2}} - 2x}{x\left(3 + \frac{2}{x}\right)} = \frac{x\left(-\sqrt{4 - \frac{1}{x} + \frac{1}{x^2}} - 2\right)}{x\left(3 + \frac{2}{x}\right)}   Divide numerator and denominator by xx and evaluate as x→−∞x \to -\infty:   −4−0+0−23+0=−2−23=−43\frac{-\sqrt{4 - 0 + 0} - 2}{3 + 0} = \frac{-2 - 2}{3} = -\frac{4}{3}

  • Limit of Rational Function at Infinity:   lim⁡x→∞5x2−3x+19x2+2=lim⁡x→∞5−3x+1x29+2x2=5−0+09+0=59\lim_{x \to \infty} \frac{5x^2 - 3x + 1}{9x^2 + 2} = \lim_{x \to \infty} \frac{5 - \frac{3}{x} + \frac{1}{x^2}}{9 + \frac{2}{x^2}} = \frac{5 - 0 + 0}{9 + 0} = \frac{5}{9}

  • Limit Involving Conjugate Multiplication at Infinity:   lim⁡x→∞(16x2+7x−4x)\lim_{x \to \infty} (\sqrt{16x^2 + 7x} - 4x)   Multiply by the conjugate expression:   (16x2+7x−4x)(16x2+7x+4x)16x2+7x+4x=(16x2+7x)−16x216x2+7x+4x=7x16x2+7x+4x\frac{(\sqrt{16x^2 + 7x} - 4x)(\sqrt{16x^2 + 7x} + 4x)}{\sqrt{16x^2 + 7x} + 4x} = \frac{(16x^2 + 7x) - 16x^2}{\sqrt{16x^2 + 7x} + 4x} = \frac{7x}{\sqrt{16x^2 + 7x} + 4x}   Divide numerator and denominator by xx (noting that for x>0x > 0, x=x2x = \sqrt{x^2}):   716+7x+4\frac{7}{\sqrt{16 + \frac{7}{x}} + 4}   Taking the limit as x→∞x \to \infty:   716+0+4=74+4=78\frac{7}{\sqrt{16 + 0} + 4} = \frac{7}{4 + 4} = \frac{7}{8}

  • Trigonometric Limit with Tangent:   lim⁡x→0xtan⁡(9x)=lim⁡x→0xcos⁡(9x)sin⁡(9x)=lim⁡x→0[19⋅9xsin⁡(9x)⋅cos⁡(9x)]\lim_{x \to 0} \frac{x}{\tan(9x)} = \lim_{x \to 0} \frac{x\cos(9x)}{\sin(9x)} = \lim_{x \to 0} \left[\frac{1}{9} \cdot \frac{9x}{\sin(9x)} \cdot \cos(9x)\right]   Using the standard limit lim⁡u→0sin⁡(u)u=1\lim_{u \to 0} \frac{\sin(u)}{u} = 1:   =19⋅(1)⋅cos⁡(0)=19= \frac{1}{9} \cdot (1) \cdot \cos(0) = \frac{1}{9}

Horizontal and Vertical Asymptotes
  • Rational Function: y=x2−4x+4x2+5x−14y = \frac{x^2 - 4x + 4}{x^2 + 5x - 14}   Factor numerator and denominator:   y=(x−2)2(x+7)(x−2)=x−2x+7,x≠2y = \frac{(x - 2)^2}{(x + 7)(x - 2)} = \frac{x - 2}{x + 7}, \quad x \ne 2

    • Horizontal Asymptote (HA):     lim⁡x→±∞x−2x+7=1  ⟹  y=1\lim_{x \to \pm\infty} \frac{x - 2}{x + 7} = 1 \implies y = 1
    • Vertical Asymptote (VA): Occurs where the simplified denominator is zero: x+7=0  ⟹  x=−7x + 7 = 0 \implies x = -7.     (Note: x=2x = 2 is a removable discontinuity or hole, not a vertical asymptote.)
  • Exponential Rational Function: y=2e2x+e−2x2e2x−3e−2xy = \frac{2e^{2x} + e^{-2x}}{2e^{2x} - 3e^{-2x}}

    • Horizontal Asymptote as x→∞x \to \infty: Divide numerator and denominator by e2xe^{2x}:     lim⁡x→∞2+e−4x2−3e−4x=2+02−0=1  ⟹  y=1\lim_{x \to \infty} \frac{2 + e^{-4x}}{2 - 3e^{-4x}} = \frac{2 + 0}{2 - 0} = 1 \implies y = 1
    • Horizontal Asymptote as x→−∞x \to -\infty: Divide numerator and denominator by e−2xe^{-2x}:     lim⁡x→−∞2e4x+12e4x−3=0+10−3=−13  ⟹  y=−13\lim_{x \to -\infty} \frac{2e^{4x} + 1}{2e^{4x} - 3} = \frac{0 + 1}{0 - 3} = -\frac{1}{3} \implies y = -\frac{1}{3}
    • Vertical Asymptote: Set the denominator to zero:     2e2x−3e−2x=02e^{2x} - 3e^{-2x} = 02e2x=3e−2x  ⟹  e4x=32=1.52e^{2x} = 3e^{-2x} \implies e^{4x} = \frac{3}{2} = 1.54x=ln⁡(1.5)  ⟹  x=14ln⁡(1.5)4x = \ln(1.5) \implies x = \frac{1}{4}\ln(1.5)

Continuity and the Intermediate Value Theorem

Determining Continuity Parameters

A function f(x)f(x) is continuous at a point x=ax = a if and only if: lim⁡x→a−f(x)=lim⁡x→a+f(x)=f(a)\lim_{x \to a^-} f(x) = \lim_{x \to a^+} f(x) = f(a)

Problem: Find all values of cc that make f(x)f(x) continuous on R\mathbb{R}: f(x)={c2+x2−1x−1,if x<12cx+x+9,if x≥1f(x) = \begin{cases} c^2 + \frac{x^2 - 1}{x - 1}, & \text{if } x < 1 \\ 2cx + x + 9, & \text{if } x \ge 1 \end{cases}

  • For x<1x < 1, simplify the rational term for x≠1x \ne 1:   x2−1x−1=(x−1)(x+1)x−1=x+1\frac{x^2 - 1}{x - 1} = \frac{(x - 1)(x + 1)}{x - 1} = x + 1   Compute the left-hand limit:   lim⁡x→1−f(x)=lim⁡x→1−[c2+(x+1)]=c2+1+1=c2+2\lim_{x \to 1^-} f(x) = \lim_{x \to 1^-} [c^2 + (x + 1)] = c^2 + 1 + 1 = c^2 + 2
  • For x≥1x \ge 1, evaluate the right-hand limit and function value directly:   f(1)=lim⁡x→1+(2cx+x+9)=2c(1)+1+9=2c+10f(1) = \lim_{x \to 1^+} (2cx + x + 9) = 2c(1) + 1 + 9 = 2c + 10
  • Equate the one-sided limits to ensure continuity at x=1x = 1:   c2+2=2c+10c^2 + 2 = 2c + 10c2−2c−8=0c^2 - 2c - 8 = 0   Factor the quadratic equation:   (c−4)(c+2)=0(c - 4)(c + 2) = 0   Solving for cc yields:   c=4orc=−2c = 4 \quad \text{or} \quad c = -2
Root Existence via the Intermediate Value Theorem (IVT)

The Intermediate Value Theorem states that if a function g(x)g(x) is continuous on a closed interval [a,b][a, b], and NN is any value strictly between g(a)g(a) and g(b)g(b), then there exists at least one number k∈(a,b)k \in (a, b) such that g(k)=Ng(k) = N.

Problem: Show that the equation cos⁡(x)+x3−3=e−x\cos(x) + x^3 - 3 = e^{-x} has a real root.

  1. Set up an auxiliary function by moving all terms to one side:    g(x)=cos⁡(x)+x3−3−e−xg(x) = \cos(x) + x^3 - 3 - e^{-x}
  2. Establish continuity: The functions cos⁡(x)\cos(x), x3−3x^3 - 3, and e−xe^{-x} are continuous on all of R\mathbb{R}, so their linear combination g(x)g(x) is continuous on any interval [a,b][a, b].
  3. Test endpoints:
    • At x=0x = 0:      g(0)=cos⁡(0)+03−3−e0=1+0−3−1=−3<0g(0) = \cos(0) + 0^3 - 3 - e^{0} = 1 + 0 - 3 - 1 = -3 < 0
    • At x=2x = 2:      g(2)=cos⁡(2)+23−3−e−2=cos⁡(2)+8−3−1e2=5+cos⁡(2)−1e2g(2) = \cos(2) + 2^3 - 3 - e^{-2} = \cos(2) + 8 - 3 - \frac{1}{e^2} = 5 + \cos(2) - \frac{1}{e^2}      Since −1≤cos⁡(2)≤1-1 \le \cos(2) \le 1 and 0<1e2<10 < \frac{1}{e^2} < 1, we have:      g(2)≥5−1−1=3>0g(2) \ge 5 - 1 - 1 = 3 > 0
  4. Apply the theorem: Since g(0)<0g(0) < 0 and g(2)>0g(2) > 0, and g(x)g(x) is continuous on [0,2][0, 2], by the Intermediate Value Theorem there exists at least one real value c∈(0,2)c \in (0, 2) such that g(c)=0g(c) = 0. Therefore, cos⁡(x)+x3−3=e−x\cos(x) + x^3 - 3 = e^{-x} has a real root.

Differential Calculus: First Principles and Differentiation Rules

The Limit Definition of the Derivative

The derivative of a function f(x)f(x) is defined as the limit of the difference quotient: f′(x)=lim⁡h→0f(x+h)−f(x)hf'(x) = \lim_{h \to 0} \frac{f(x + h) - f(x)}{h}

Definition Applied to a Polynomial

Find the derivative of f(x)=x2+5xf(x) = x^2 + 5x using the limit definition: f′(x)=lim⁡h→0[(x+h)2+5(x+h)]−[x2+5x]hf'(x) = \lim_{h \to 0} \frac{[(x + h)^2 + 5(x + h)] - [x^2 + 5x]}{h}=lim⁡h→0x2+2xh+h2+5x+5h−x2−5xh= \lim_{h \to 0} \frac{x^2 + 2xh + h^2 + 5x + 5h - x^2 - 5x}{h}=lim⁡h→02xh+h2+5hh=lim⁡h→0(2x+h+5)=2x+5= \lim_{h \to 0} \frac{2xh + h^2 + 5h}{h} = \lim_{h \to 0} (2x + h + 5) = 2x + 5

Definition Applied to a Radical Quotient

Find the derivative of f(x)=75x+4f(x) = \frac{7}{\sqrt{5x + 4}} using the limit definition: f′(x)=lim⁡h→01h[75(x+h)+4−75x+4]f'(x) = \lim_{h \to 0} \frac{1}{h} \left[\frac{7}{\sqrt{5(x + h) + 4}} - \frac{7}{\sqrt{5x + 4}}\right] Combine fractions over a common denominator: =lim⁡h→07h[5x+4−5x+5h+45x+5h+45x+4]= \lim_{h \to 0} \frac{7}{h} \left[\frac{\sqrt{5x + 4} - \sqrt{5x + 5h + 4}}{\sqrt{5x + 5h + 4}\sqrt{5x + 4}}\right] Rationalize the numerator by multiplying by its conjugate: =lim⁡h→07h(5x+4)−(5x+5h+4)5x+5h+45x+4(5x+4+5x+5h+4)= \lim_{h \to 0} \frac{7}{h} \frac{(5x + 4) - (5x + 5h + 4)}{\sqrt{5x + 5h + 4}\sqrt{5x + 4}(\sqrt{5x + 4} + \sqrt{5x + 5h + 4})}=lim⁡h→07h−5h5x+5h+45x+4(5x+4+5x+5h+4)= \lim_{h \to 0} \frac{7}{h} \frac{-5h}{\sqrt{5x + 5h + 4}\sqrt{5x + 4}(\sqrt{5x + 4} + \sqrt{5x + 5h + 4})} Cancel hh and evaluate the limit as h→0h \to 0: =−355x+45x+4(5x+4+5x+4)=−35(5x+4)(25x+4)=−352(5x+4)3/2= \frac{-35}{\sqrt{5x + 4}\sqrt{5x + 4}(\sqrt{5x + 4} + \sqrt{5x + 4})} = \frac{-35}{(5x + 4)(2\sqrt{5x + 4})} = -\frac{35}{2(5x + 4)^{3/2}}

Definition Applied to a Trigonometric Function

Find the derivative of f(x)=sin⁡(7x)f(x) = \sin(7x) using the limit definition: f′(x)=lim⁡h→0sin⁡(7(x+h))−sin⁡(7x)h=lim⁡h→0sin⁡(7x+7h)−sin⁡(7x)hf'(x) = \lim_{h \to 0} \frac{\sin(7(x + h)) - \sin(7x)}{h} = \lim_{h \to 0} \frac{\sin(7x + 7h) - \sin(7x)}{h} Apply the angle sum identity sin⁡(7x+7h)=sin⁡(7x)cos⁡(7h)+cos⁡(7x)sin⁡(7h)\sin(7x + 7h) = \sin(7x)\cos(7h) + \cos(7x)\sin(7h): =lim⁡h→0sin⁡(7x)cos⁡(7h)+cos⁡(7x)sin⁡(7h)−sin⁡(7x)h= \lim_{h \to 0} \frac{\sin(7x)\cos(7h) + \cos(7x)\sin(7h) - \sin(7x)}{h} Group terms: =lim⁡h→0[sin⁡(7x)(cos⁡(7h)−1h)+cos⁡(7x)(sin⁡(7h)h)]= \lim_{h \to 0} \left[\sin(7x)\left(\frac{\cos(7h) - 1}{h}\right) + \cos(7x)\left(\frac{\sin(7h)}{h}\right)\right] Multiply and divide by 7 to use fundamental trigonometric limits: =sin⁡(7x)(7lim⁡h→0cos⁡(7h)−17h)+cos⁡(7x)(7lim⁡h→0sin⁡(7h)7h)= \sin(7x)\left(7 \lim_{h \to 0} \frac{\cos(7h) - 1}{7h}\right) + \cos(7x)\left(7 \lim_{h \to 0} \frac{\sin(7h)}{7h}\right) Using lim⁡θ→0cos⁡(θ)−1θ=0\lim_{\theta \to 0} \frac{\cos(\theta) - 1}{\theta} = 0 and lim⁡θ→0sin⁡(θ)θ=1\lim_{\theta \to 0} \frac{\sin(\theta)}{\theta} = 1: =sin⁡(7x)(7⋅0)+cos⁡(7x)(7⋅1)=7cos⁡(7x)= \sin(7x)(7 \cdot 0) + \cos(7x)(7 \cdot 1) = 7\cos(7x)

Advanced Analytical Differentiation
  • Logarithmic and Power Composite Function:   y=log⁡2(tan⁡(x))+(x2+3)1/3y = \log_2(\tan(x)) + (x^2 + 3)^{1/3}   Differentiate term by term using the chain rule:   ddx[log⁡2(tan⁡(x))]=1tan⁡(x)ln⁡(2)⋅ddx[tan⁡(x)]=sec⁡2(x)tan⁡(x)ln⁡(2)\frac{d}{dx}[\log_2(\tan(x))] = \frac{1}{\tan(x)\ln(2)} \cdot \frac{d}{dx}[\tan(x)] = \frac{\sec^2(x)}{\tan(x)\ln(2)}ddx[(x2+3)1/3]=13(x2+3)−2/3⋅ddx[x2+3]=2x3(x2+3)2/3\frac{d}{dx}[(x^2 + 3)^{1/3}] = \frac{1}{3}(x^2 + 3)^{-2/3} \cdot \frac{d}{dx}[x^2 + 3] = \frac{2x}{3(x^2 + 3)^{2/3}}   Combining terms:   y′=sec⁡2(x)tan⁡(x)ln⁡(2)+2x3(x2+3)2/3y' = \frac{\sec^2(x)}{\tan(x)\ln(2)} + \frac{2x}{3(x^2 + 3)^{2/3}}

  • Quotient Involving General Exponential, Trigonometric, and Cotangent Functions:   y=2x6+cos⁡(x)+3cot⁡(x2)1+xy = \frac{2^{x^6} + \cos(x) + 3\cot(x^2)}{1 + x}   Let u=2x6+cos⁡(x)+3cot⁡(x2)u = 2^{x^6} + \cos(x) + 3\cot(x^2) and v=1+xv = 1 + x.   Compute u′u' by applying the chain rule to each component:   ddx[2x6]=2x6ln⁡(2)⋅ddx[x6]=2x6ln⁡(2)(6x5)\frac{d}{dx}[2^{x^6}] = 2^{x^6}\ln(2) \cdot \frac{d}{dx}[x^6] = 2^{x^6}\ln(2)(6x^5)ddx[cos⁡(x)]=−sin⁡(x)\frac{d}{dx}[\cos(x)] = -\sin(x)ddx[3cot⁡(x2)]=3(−csc⁡2(x2))(2x)=−6xcsc⁡2(x2)\frac{d}{dx}[3\cot(x^2)] = 3(-\csc^2(x^2))(2x) = -6x\csc^2(x^2)u′=2x6ln⁡(2)(6x5)−sin⁡(x)−6xcsc⁡2(x2)u' = 2^{x^6}\ln(2)(6x^5) - \sin(x) - 6x\csc^2(x^2)   The derivative of the denominator is v′=1v' = 1.   Applying the Quotient Rule y′=u′v−uv′v2y' = \frac{u'v - uv'}{v^2}:   y′=(2x6ln⁡(2)(6x5)−sin⁡(x)−6xcsc⁡2(x2))(1+x)−(2x6+cos⁡(x)+3cot⁡(x2))(1+x)2y' = \frac{(2^{x^6}\ln(2)(6x^5) - \sin(x) - 6x\csc^2(x^2))(1 + x) - (2^{x^6} + \cos(x) + 3\cot(x^2))}{(1 + x)^2}

  • Product Rule with Inverse Sine Composite:   y=e5xsin⁡(x3−2x)−4sin⁡−1(2x+1)y = e^{5x}\sin(x^3 - 2x) - 4\sin^{-1}(2x + 1)   Differentiate the product term using ddx[uv]=u′v+uv′\frac{d}{dx}[uv] = u'v + uv':   ddx[e5xsin⁡(x3−2x)]=5e5xsin⁡(x3−2x)+e5xcos⁡(x3−2x)(3x2−2)\frac{d}{dx}[e^{5x}\sin(x^3 - 2x)] = 5e^{5x}\sin(x^3 - 2x) + e^{5x}\cos(x^3 - 2x)(3x^2 - 2)   Differentiate the inverse trigonometric term using ddu[sin⁡−1(u)]=11−u2\frac{d}{du}[\sin^{-1}(u)] = \frac{1}{\sqrt{1 - u^2}}, where u=2x+1u = 2x + 1:   ddx[−4sin⁡−1(2x+1)]=−4(11−(2x+1)2)(2)=−81−(2x+1)2\frac{d}{dx}[-4\sin^{-1}(2x + 1)] = -4\left(\frac{1}{\sqrt{1 - (2x + 1)^2}}\right)(2) = -\frac{8}{\sqrt{1 - (2x + 1)^2}}   Combining all terms:   y′=5e5xsin⁡(x3−2x)+(3x2−2)e5xcos⁡(x3−2x)−81−(2x+1)2y' = 5e^{5x}\sin(x^3 - 2x) + (3x^2 - 2)e^{5x}\cos(x^3 - 2x) - \frac{8}{\sqrt{1 - (2x + 1)^2}}

  • Chain and Product Rules with Inverse Cotangent:   y=esec⁡(x)+ln⁡(x)cot⁡−1(x5)y = e^{\sec(x)} + \ln(x)\cot^{-1}(x^5)   Differentiate the exponential term via the chain rule:   ddx[esec⁡(x)]=esec⁡(x)⋅ddx[sec⁡(x)]=esec⁡(x)sec⁡(x)tan⁡(x)\frac{d}{dx}[e^{\sec(x)}] = e^{\sec(x)} \cdot \frac{d}{dx}[\sec(x)] = e^{\sec(x)}\sec(x)\tan(x)   Differentiate the product term using ddu[cot⁡−1(u)]=−11+u2\frac{d}{du}[\cot^{-1}(u)] = -\frac{1}{1 + u^2}, where u=x5u = x^5 and u′=5x4u' = 5x^4:   ddx[ln⁡(x)cot⁡−1(x5)]=(1x)cot⁡−1(x5)+ln⁡(x)(−5x41+(x5)2)=cot⁡−1(x5)x−5x4ln⁡(x)1+x10\frac{d}{dx}[\ln(x)\cot^{-1}(x^5)] = \left(\frac{1}{x}\right)\cot^{-1}(x^5) + \ln(x)\left(-\frac{5x^4}{1 + (x^5)^2}\right) = \frac{\cot^{-1}(x^5)}{x} - \frac{5x^4\ln(x)}{1 + x^{10}}   Combining all terms:   y′=esec⁡(x)sec⁡(x)tan⁡(x)+cot⁡−1(x5)x−5x4ln⁡(x)1+x10y' = e^{\sec(x)}\sec(x)\tan(x) + \frac{\cot^{-1}(x^5)}{x} - \frac{5x^4\ln(x)}{1 + x^{10}}