MSM 112: Mathematical Methods II – Limits, Continuity, and Differentiation
Fundamental Concepts and Informal Definitions of Limits
Within the study of calculus, the limit of a function serves as the foundational stone of differential calculus, representing the central idea that distinguishes the discipline from algebra and trigonometry. According to Definition 1, for a function f(x) defined on an open interval surrounding a point x0 (though not necessarily at x0 itself), if f(x) becomes arbitrarily close to a value L for all x sufficiently close to x0, we state that f approaches the limit L as x approaches x0. This is expressed mathematically as limx→x0f(x)=L.
Example 2 illustrates the behavior of the function f(x)=x−1x2−1 near x=1. While the function is undefined at x=1 due to division by zero, the formula can be simplified for all x=1 by factoring the numerator: f(x)=x−1(x+1)(x−1)=x+1. Consequently, the graph of f is a line y=x+1 with a hole at the point (1,2). Numerical data supports this limit; as x approaches 1 from below (0.9, 0.99, 0.999) and from above (1.1, 1.01, 1.001), the values of f(x) approach 1.9, 1.99, 1.999 and 2.1, 2.01, 2.001 respectively. Choosing x closer to 1, such as 0.999999 or 1.000001, yields f(x) values of 1.999999 and 2.000001. Thus, limx→1x−1x2−1=2. This demonstrates that the limit value does not depend on how the function is defined precisely at x0.
Limit Evaluation Techniques and Identity Functions
Evaluating a limit limx→x0f(x) can often be achieved through direct substitution by calculating f(x0). This is particularly applicable when f(x) is an algebraic combination of polynomials and trigonometric functions for which f(x0) is defined. For example, limx→2(5x−3)=10−3=7, and limx→−2x+53x+4=−2+5−6+4=−32. In more complex cases, such as limx→3x3−x2+x+12x2+2x−5, the result is (3)3−(3)2+3+12(3)2+2(3)−5=27−9+3+118+6−5=2219.
Specific functions such as Identity and Constant functions have reliable limits at every point. Definition 5 establishes that for an identity function f(x)=x, then for any x0, limx→x0x=x0. Similarly, for a constant function f(x)=k, limx→x0k=k regardless of the value of x0. Examples include limx→3x=3, and for constant values, limx→−74=4, limx→24=4, and limx→−1337=37.
The Limit Laws and Algebraic Manipulation
Theorem 6 details the formal Limit Laws provided that L, M, c, and k are real numbers and limx→cf(x)=L and limx→cg(x)=M. The Sum Rule states limx→c(f(x)+g(x))=L+M. The Difference Rule states limx→c(f(x)−g(x))=L−M. The Product Rule states limx→c(f(x)⋅g(x))=L⋅M. The Constant Multiple Rule states limx→c(k⋅f(x))=k⋅L. The Quotient Rule states limx→cg(x)f(x)=ML provided M=0. Finally, the Power Rule states that if r and s are integers with no common factor and s=0, then limx→x0(f(x))sr=Lsr, assuming Lsr is a real number (and if s is even, then L > 0).
When standard substitution results in a zero denominator, algebraic manipulation such as factoring or rationalization must be employed. Example 8 demonstrates this for limx→1x2−xx2+x−2. Substitution makes the denominator zero, but since the numerator is also zero at x=1, there is a common factor of (x−1). Simplifying gives x(x−1)(x+2)(x−1)=xx+2. Substituting x=1 into the result yields 11+2=3. Example 9 illustrates rationalization for limx→0x2x2+100−10. By multiplying the numerator and denominator by the conjugate x2+100+10, we obtain limx→0x2(x2+100+10)x2+100−100=limx→0x2+100+101=0+100+101=201.
Precise Definition and Limits at Infinity
While informal insight is useful, calculus relies on a precise definition of a limit (Definition 10). We say limx→x0f(x)=L if for every number \epsilon > 0, there exists a corresponding number \delta > 0 such that for all x, 0 < |x - x_0| < \delta \implies |f(x) - L| < \epsilon. This rigorous definition is generally reserved for higher-level courses.
Limits at infinity describe the behavior of a function when values in the domain or range outgrow all finite values. The symbol for infinity (∞) is not a real number. For the function f(x)=x1, as x becomes increasingly large and positive, f(x) becomes decreasingly small, approaching 0. Thus, limx→∞x1=0 and limx→−∞x1=0. Definition 11 specifies that limx→∞f(x)=L if for every \epsilon > 0 there exists a number M such that x > M \implies |f(x) - L| < \epsilon. Similarly, limx→−∞f(x)=L if for every ϵ>0 there exists a number N such that x < N \implies |f(x) - L| < \epsilon. Theorem 12 confirms that the algebraic Limit Laws for finite limits also apply to limits as x→±∞.
To determine the limit of a rational function as x→±∞, one should divide the numerator and denominator by the highest power of x found in the denominator. In Example 14, where the degrees are equal (limx→∞3x2+25x2+8x−3), dividing by x2 results in 3+05+0−0=35. In Example 15, where the degree of the denominator is higher (limx→−∞2x3−111x+2), dividing by x3 produces 2−00+0=0.
Infinite Limits and Asymptotes
Infinite limits describe the behavior of functions whose values become arbitrarily large. For f(x)=x1, as x→0+, the values grow without bound, written as limx→0+x1=∞. This does not mean the limit exists in a traditional sense, but that the function becomes arbitrarily large and positive. Conversely, as x→0−, limx→0−x1=−∞. Example 16 analyzes y=x−11, which is a horizontal shift of y=x1 one unit to the right; here limx→1+x−11=∞ and limx→1−x−11=−∞.
Rational functions exhibit various behaviors near the zeros of their denominators. Sometimes zeros cancel, as in Example 19(i): limx→2x2−4(x−2)2=limx→2x+2x−2=0. However, if cancellation is incomplete, infinite limits may occur. For y=x2−4x−3, as x→2+, the limit is −∞, while as x→2−, the limit is ∞. Since the behavior is inconsistent, limx→2x2−4x−3 does not exist. Asymptotes are lines the graph approaches. Example 20 shows that for y=x+2x+3, which can be recast as y=1+x+21, the horizontal asymptote is y=1 and the vertical asymptote is x=−2. Example 22 explores oblique asymptotes; for f(x)=2x−4x2−3, long division yields 2x+1+2x−41. As x→±∞, the remainder vanishes, leaving the oblique asymptote y=2x+1.
Limits of Trigonometric, Exponential, and Logarithmic Functions
Definition 23 outlines basic trigonometric limits: limx→csin(x)=sin(c) and limx→ccos(x)=cos(c) for all real numbers c. Limitations exist for other functions (e.g., tan(x) is defined for all c=2π+kπ). Theorem 24 introduces special limits: limx→0xsin(x)=1 and limx→0x1−cos(x)=0. These can be extended via Theorem 28: limx→0nxsin(nx)=1. Evaluation often requires creating matching structures, such as in Example 29: limx→02x2+xsin(2x)=limx→0x(2x+1)sin(2x)=limx→0(2x2sin(2x)⋅2x+11)=2(1)(1)=2.
Exponential function limits rely on basic facts: limx→∞ex=∞ and limx→−∞ex=0. Specifically, Theorem 36 notes limx→∞(1+x1)x=e and limx→0xex−1=1. For logarithmic functions, finite limits agree with function values if c > 0. However, limx→∞loga(x)=∞ and limx→0+loga(x)=−∞ for a > 1. Theorem 41 adds special cases like limx→1x−1ln(x)=1 and limx→∞xln(x)=0. Example 79 demonstrates differentiation applications of these, noting dxd[ln(ax+b)]=ax+ba.
Continuity and the Continuity Test
A function f(x) is continuous if its graph can be sketched without lifting the pencil. Definition 43 specifies continuity at an interior point c if limx→cf(x)=f(c). For endpoints, one-sided limits must match function values. Definition 44 clarifies that a function is right-continuous at c if limx→c+f(x)=f(c) and left-continuous if limx→c−f(x)=f(c). Theorem 46 provides the Continuity Test: a function is continuous at c in its domain if and only if f(c) exists, limx→cf(x) exists (requiring the left-hand limit to equal the right-hand limit), and the limit equals the function value.
Example 47 discusses the unit step function g(x) which is 1 for x≥0 and 0 for x < 0. At x=0, g(0)=1, but limx→0−g(x)=0 and limx→0+g(x)=1. Since the one-sided limits are unequal, limx→0g(x) does not exist, and the function is discontinuous at x=0. Example 48 features h(x)=x−1(x+2)(x−1) for x=1 and h(1)=2. Here, limx→1h(x)=3. Although the limit and function value exist, they are not equal, making the function discontinuous at x=1.
Differentiation from First Principles and Basic Rules
Differentiation is the process of finding the differential coefficient of a function. The derivative f′(x) is defined as limh→0hf(x+h)−f(x), provided the limit exists. This formula is often called the First Principle. Differentiability requires a "smoothness" condition on the graph; if secant lines through points P and Q do not approach a limiting slope as Q→P, the derivative fails to exist at that point. Common notations include f′(x), y′, dxdy, and Dxf(x).
Basic differentiation rules include the Power Rule (dxd[xn]=nxn−1), Constant Multiple Rule (dxd[cf(x)]=cf′(x)), Constant Rule (dxd[c]=0), and the Sum and Difference Rules (dxd[f(x)±g(x)]=f′(x)±g′(x)). The Product Rule is dxd[f(x)g(x)]=f(x)g′(x)+g(x)f′(x). The Quotient Rule is dxd[g(x)f(x)]=[g(x)]2g(x)f′(x)−f(x)g′(x). Theorem 60 provides trigonometric derivatives: dxdsin(x)=cos(x) and dxdcos(x)=−sin(x). Related functions follow: dxdtan(x)=sec2(x), dxdcot(x)=−csc2(x), dxdsec(x)=sec(x)tan(x), and dxdcsc(x)=−csc(x)cot(x).
Chain Rule, Implicit Differentiation, and Higher-Order Derivatives
The Chain Rule allows for the differentiation of composite functions (f∘g)(x)=f(g(x)). According to Definition 64, (f∘g)′(x)=f′(g(x))⋅g′(x), or in Leibniz notation, dxdy=dudy⋅dxdu. Example 66 shows that to differentiate y=sin(x2+x), you set u=x2+x, find dudy=cos(u) and dxdu=2x+1, resulting in dxdy=(2x+1)cos(x2+x).
Implicit functions, where y cannot be easily isolated as f(x), require implicit differentiation. This involves differentiating both sides of an equation with respect to x, assuming y is a differentiable function of x, and then solving for dxdy. The rule is stated as dxd[f(y)]=dyd[f(y)]⋅dxdy. Example 74 demonstrates this with 2y2−5x4−2−7y3=0, yielding 4ydxdy−20x3−21y2dxdy=0, then solved as dxdy=4y−21y220x3. Logarithmic differentiation is a specific technique where natural logarithms are taken on both sides to simplify products, quotients, or variable exponents (like y=xx) before differentiating implicitly.
Successive Differentiation involves taking derivatives of derivatives. If y=f(x), the second derivative is f′′(x) or dx2d2y. Higher orders like the third (dx3d3y) or n-th (dxndny) can be calculated. Standard formulas for inverse trigonometric derivatives also exist. When y=sin−1(x), dxdy=1−x21. For the general case y=sin−1f(x), dxdy=1−[f(x)]2f′(x). Similar general formulas are defined for cos−1, tan−1, and others, often involving a constant a representing scale, such as dxd[tan−1(ax)]=a2+x2a.