A limit is the value to which a function grows close as the input approaches some value. One would say that the limit of f, as x approaches a, is L. Formally, for every real ε > 0, there exists a real δ > 0 such that for all real x, 0 < | x − a | < δ implies that | f(x) − L | < ε. In other words, f(x) gets closer and closer to L (f(x)∈ [L-ε, L+ε]) as x moves closer and closer to a (x ∈ [a-δ, a+δ], x≠a)) -Fig 1.a.-
A limit involves what is going on around a point, and does not care what happens at it.
Let f(x) be a function defined on an interval that contains x = a, except possibly at x = a, then we say that, $\lim_{x \to a} f(x) = L$ if
$\forall \epsilon>0, \exists \delta>0: 0<|x-a|<\delta, implies~ |f(x)-L|<\epsilon$
Or
$\forall \epsilon>0, \exists \delta>0: |f(x)-L|<\epsilon, whenever~ 0<|x-a|<\delta$
$\forall \epsilon>0, \exists \delta>0: 0<|x|<\delta, implies~ |x^{2}|<\epsilon$
Let’s choose $\delta = \sqrt \epsilon, then$ $\forall \epsilon>0, \exists \delta>0: 0<|x|<\sqrt \epsilon, implies~ |x^{2}|<\epsilon$
That’s true because $|x^{2}|=|x|^{2}<(\sqrt \epsilon)^{2} = \epsilon$
Exercise: $\lim_{x \to 2} 5x - 4 = 6$ -1.c.-
$\forall \epsilon>0, \exists \delta>0: 0<|x-2|<\epsilon,~implies~ |5x - 4 -6|<\epsilon$
$\forall \epsilon>0, \exists \delta>0: 0<|x-2|<\epsilon,~implies~ 5|x - 2|<\epsilon$
Let’s choose $\delta = \frac {\epsilon}{5}$, then
$\forall \epsilon>0, \exists \delta>0: 0<|x-2|<\frac {\epsilon}{5},~implies~ 5|x - 2|<\frac {5\epsilon}{5} = \epsilon$
Exercises:
$\forall \epsilon>0, \exists \delta>0: 0<|x|<\delta,~implies~ |xsin(\frac {1}{x})|<\epsilon$
Let’s choose $\delta = \epsilon, 0<|x|<\epsilon,~implies~ |xsin(\frac {1}{x})|≤|x|<\epsilon$
Definitions. A right hand limit is defined as the value L to which a function grows close as the input approaches some value from the right.Let f(x) be a function defined on an interval that contains x = a, except possibly at x = a, then we say that, $\lim_{x \to a^{+}} f(x) = L$ if
$\forall \epsilon>0, \exists \delta>0: |f(x)-L|<\epsilon, whenever~ 0 < x-a < \delta.$
Definitions. A left hand limit is defined as the value L to which a function grows close as the input approaches some value from the left.Let f(x) be a function defined on an interval that contains x = a, except possibly at x = a, then we say that, $\lim_{x \to a^{-}} f(x) = L$ if
$\forall \epsilon>0, \exists \delta>0: |f(x)-L|<\epsilon, whenever~ a - \delta < x < a.$
Example: $\lim_{x \to 0^{+}} \sqrt x = 0$
$\forall \epsilon>0, \exists \delta>0: |\sqrt x|<\epsilon, whenever~ 0 < x < \delta.$
Let’s choose $\delta = \epsilon^{2}$
$\forall \epsilon>0, \exists \delta>0: 0 < x < \epsilon^{2}, then~ |\sqrt x| < \sqrt{\epsilon^{2}} = \epsilon.$
Exercise: $f(x) = \begin{cases} x + 1, &x > 0\\\\ -2x + 2, &x < 0 \end{cases}$ -1.g.-
$\lim_{x \to 0^{+}} f(x) = \lim_{x \to 0^{+}} x + 1 = 1.$ $\lim_{x \to 0^{-}} f(x) = \lim_{x \to 0^{-}} -2x + 2 = 2.$ We don’t need a value for x = 0.
Let f(x) be a function defined on an interval that contains x = a, except possibly at x = a, then we say that, $\lim_{x \to a} f(x) = \infty$ if
$\forall M>0, \exists \delta>0: f(x) > M, whenever~ 0<|x-a|<\delta.$ We can make the value of f(x) arbitrary large by taking x to be sufficiently close, but not equal to a. -1.d.-
Let f(x) be a function defined on an interval that contains x = a, except possibly at x = a, then we say that, $\lim_{x \to a} f(x) = -\infty$ if
$\forall M<0, \exists \delta>0: f(x) < M, whenever~ 0<|x-a|<\delta.$ We can make the value of f(x) arbitrary small by taking x to be sufficiently close, but not equal to a.
$\forall M>0, \exists \delta>0: \frac {1}{x^{2}} > M, whenever~ 0<|x|<\delta.$
Let’s choose $\delta = \frac {1}{\sqrt M}$
$\forall M>0, \exists \delta = \frac {1}{\sqrt M}>0: \frac {1}{x^{2}} > M, whenever~ 0<|x|<\frac {1}{\sqrt M}.$
$|x|<\frac {1}{\sqrt M} ⇨ |x|^{2}<\frac {1}{M} ⇨ x^{2}<\frac {1}{M} ⇨ M <\frac{1}{x^{2}}$
Limits at infinity are used to describe the behavior of functions as the independent variable increases or decreases without bound.
Definition. Let f(x) be a function defined on (K, ∞) for some K. Then, we say that, $\lim_{x \to \infty} f(x) = L$, and f(x) is said to have a horizontal asymptote at y = L if
$\forall \epsilon>0, \exists M>0: |f(x)-L|<\epsilon, whenever~ x>M.$ We can make f(x) as close as we want to L by making x large enough. -1.e.-
Let f(x) be a function defined on (-∞, K) for some K. Then, we say that, $\lim_{x \to -\infty} f(x) = L$, and f(x) is said to have a horizontal asymptote at y = L if
$\forall \epsilon>0, \exists M<0: |f(x)-L|<\epsilon, whenever~ x < M$ We can make f(x) as close as we want to L by making x small enough.
Exercise: $\lim_{x \to \infty} \frac{1}{x} = 0$ -1.f.-
$\forall \epsilon>0, \exists M>0: |\frac{1}{x}|<\epsilon, whenever~ x>M$
Let’s choose $M = \frac{1}{\epsilon}, x>\frac{1}{\epsilon} ⇨ |x|>\frac{1}{\epsilon} ⇨ \epsilon>\frac{1}{|x|} = |\frac{1}{x}|$
Exercise: $\lim_{x \to \infty} \frac {cos(x)}{x} = \infty$. It intersects its horizontal asymptote (y = 0) an infinite number of times as it oscillates around it with ever-decreasing amplitude.
The squeeze or sandwich theorem. If a function f lies between two functions g and h, and the limits of each of them at a particular point are equal to L, then the limit of f at that particular point is also equal to L. Let f, g, and h be functions defined on an interval I that contains x = a, except possibly at x = a. Suppose that for every x in I not equal to a, we have g(x) ≤ f(x) ≤ h(x), and also suppose that $\lim_{x \to a} g(x) = \lim_{x \to a} h(x) = L.$ Then, $\lim_{x \to a} g(x) = L.$
Proof: $\forall \epsilon>0, \exists \delta_1>0: 0<|x-a|<\delta_1,~implies~ |g(x)-L|<\epsilon~ *_1$
$\forall \epsilon>0, \exists \delta_2>0: 0<|x-a|<\delta_2,~implies~ |h(x)-L|<\epsilon~ *_2$
Let’s choose as $\delta = min(\delta_1, \delta_2)$ $\forall \epsilon>0, \exists \delta>0: 0<|x-a|<\delta_1,~implies~$
$L -\epsilon < g(x) < L +\epsilon$ [*1] and $L -\epsilon < h(x) < L +\epsilon$ [*2]
$L -\epsilon < g(x) ≤ f(x) ≤ h(x) < L +\epsilon$ ⇨ $|f(x)-L|<\epsilon$
Exercises:
$-1 ≤ sin(\frac{1}{x}) ≤ 1 ⇨ -x^{2} ≤ x^{2}sin(\frac{1}{x}) ≤ x^{2}$
$\lim_{x \to 0} x^{2} = \lim_{x \to 0} -x^{2} = 0.$
Let’s prove it geometrically. The arc length of a circle in radians can be expressed as, Arc Length = $\theta·r = x~ because~ r=1.$ Notice that as x→0, the bow string is the same size than the bow itself, that is, $\lim_{x \to 0} (\frac{sin(x)}{x}) = 1.$ -1.b.-
Another way of proving it is as follows: -1.a.-
$Area(\triangle ADF) ≥ Area(Sector ADB) ≥ Area(\triangle ADB)$ $ ⇨ \frac{tan(x)}{2} ≥ \frac{x}{2} ≥ \frac{sin(x)}{2}$ because the Area of a circle with an angle measuring 360º is πr2 ⇨ Area of a sector is θ⁄360ºπr2 ⇨ Area(Sector ADB) = 1⁄2r2θ, where θ is the angle in radians = 1⁄2θ
$ ⇨ \frac{sin(x)}{cos(x)} ≥ x ≥ sin(x) ⇨ \frac{cos(x)}{sin(x)} ≤ \frac{1}{x} ≤\frac{1}{sin(x)} ⇨ cos(x) ≤ \frac{sin(x)}{x} ≤1$
$\lim_{x \to 0} cos(x) = \lim_{x \to 0} 1 = 1 ⇨ \lim_{x \to 0} (\frac{sin(x)}{x}) = 1.$
It can also be solved as follows,
$\lim_{x \to 0} (\frac{1-cos(x)}{x}) = \lim_{x \to 0} (\frac{(1-cos(x))(1+cos(x))}{x(1+cos(x))}) = \lim_{x \to 0} (\frac{1-cos^{2}(x)}{x(1+cos(x))}) = \lim_{x \to 0} (\frac{sin^{2}(x)}{x(1+cos(x))})$
$ = \lim_{x \to 0} (\frac{sin(x)}{x}\frac{sin(x)}{1+cos(x)}) = \lim_{x \to 0} (\frac{sin(x)}{x}) \lim_{x \to 0}(\frac{sin(x)}{1+cos(x)})$ [by the product law for limits] = 1·0 = 0.
Let f(x), g(x) be functions defined on an interval that contains x = a, except possibly at x = a. assume that L and M are real numbers such that $ \lim_{x \to a} f(x) = L$ and $ \lim_{x \to a} g(x) = M$. Let c be a constant. Then, each of the following statements holds:
Proof: Let $\epsilon>0$
$\exists \delta_1>0: 0<|x-a|<\delta_1, implies~ |f(x)-L|<\frac{epsilon}{2}$
$\exists \delta_2>0: 0<|x-a|<\delta_2, implies~ |g(x)-M|<\frac{epsilon}{2}$
Let’s choose $\delta = min (\delta_1, \delta_2).$
$\forall \epsilon>0, \exists \delta>0: 0<|x-a|<\delta, implies~ |f(x)+g(x)-L-M| ≤ |f(x)-L|+ |g(x)-M|$ [by the triangle inequality] $<\epsilon$