Title | Limit and continuity pdf lecture notes |
---|---|
Author | Dima Alnizami |
Course | Calculus I |
Institution | Lakehead University |
Pages | 163 |
File Size | 3.3 MB |
File Type | |
Total Downloads | 39 |
Total Views | 144 |
from class lecture, weeks 1 - 5 study this for exam midterm...
Lecture Notes for math111: Calculus I.
Dr. Vitaly A. Shneidman
New Jersey Institute of Technology
Fall, 2013
1
Introduction y = f (x)
Limits & Continuity Rates of change and tangents to curves
2
Average rate of change ∆y ∆x
=
f (x2) − f (x1) x2 − x1
(1)
Equation for the secant line: ∆y (x − x1) + f (x1) ∆x Tangent - secant in the limit x2 → x1 (Or, ∆x → 0). Slope of tangent Y =
f ′ (x1) ≡
∆y , ∆x → 0 ∆x
(2)
(notation f ′ is not yet in the book, but will appear later...). Equation of tangent line: Y = f ′ (x1) (x − x1) + f (x1) 3
Example (Galileo): t instead of x or x1, h instead of ∆x. 1 y(t) = at2 2 where a is a constant (”acceleration”). Secant (finite h) ∆y = y(t+h)−y (t) =
i 1 h 1 a (t + h)2 − t2 = a 2th + h2 2 2
∆y ∆y = a(t + h/2) = h ∆t Tangent (h → 0): y ′(t) = at (known as ”instantaneous velocity” or ”instantaneous 4
rate of change”). Returning to math notations ′ 2 = 2x x
(3)
Example: y(x) = x3 Use a3 −b3 = (a−b)(a2 +ab+b2) with a = x+h, b = x. Slope of secant (A.R.C.), finite h ≡ ∆x: h i 3 3 2 2 ∆y = y(x+h)−y (x) = (x+h) −x = h (x + h) + x(x + h) + x =
= h(3x2 + 3xh + h2)
∆y ∆y = 3x2 + 3xh + h2 = h ∆x Slope of tangent (I.R.C.) h → 0: x3
′
= 3x2
(4)
5
Example: y(x) =
√ x ∆y
∆y
√ √ x+h− x h ∆x = h √ √ √ √ 1 x+h− x x+h+ x = ·√ √ √ =√ x+h+ x x+h+ x h A.R.C. =
=
Now, no problem h → 0:
√ I.R.C. = 1/2 x
or √ ′
x
1 = √ 2 x
(5)
6
Continuity and Limits
-
-
-
-
Continuous (left) and discontinuous (right) functions
Intermediate value Theorem 11, p.99
7
Limit of a function Assume don’t know f (x0) but know f (x) for any x close to x0 . Example: H L
-
-
-
-
y (0) not defined. Can define y (0) = a, with any a. Why a = 1 is the ”best”? 8
Limit: lim f (x) = L
Example:
x→x0
x 2 − a2 = lim x + a = 2a lim x→a x − a x→a Functions with no limit as x → 0: step-function, 1/x, sin(1/x)
9
Limit Laws - Theorem 1, p.68. If f , g have limits L & M as x → c. Then, lim (f ± g) = L ± M , lim (f · g) = L · M , etc.
x→c
(6)
x→c lim (f n) = Ln , lim (f 1/n) = L1/n x→c x→c
(7)
”Dull functions” limx→c f (x) = f (c). Example q √ lim 4x2 − 3 = 13 x→−2
Example: any polynomial limx→c Pn(x) = Pn(c)
10
Limits of rational functions P (x)/Q(x) as x → c. If Q(c) 6= 0 - ”dull”, limit R(c)/Q(c). If Q(c) = 0 check P (c): if P (c) 6= 0 - no limit; If P (c) = 0 try to simplify. Example: x3 + x − 2 (x − 1)(x2 + x + 2) = lim =4 lim x→1 x→1 x2 − x x(x − 1) Other functions with limits of type ”0/0”. Example: lim
x→0
q
x 2 + a2 − a = lim x→0 x2 q
q
q 2 2 x + a − a x 2 + a2 + a ·q = x2 2 2
x +a +a
= limx→0 1/( x2 + a2 + a) = 1/2a
11
”Sandwich theorem” : Let f (x) ≤ g (x) and lim f (x) = lim g(x) = L .
x→c
x→c
IF f (x) ≤ u(x) ≤ g(x) THEN lim u(x) = L
x→c
12
Limit (sin x)/x as x → 0
6 AOC = x (in radians !)
S△OAC = 21 sin x Ssector OAC = 2x S△OAB = 21 tan x Thus,
sin x < x < tan x , 0 < x <
π 2
(8)
Divide by sin x and take the inverse, changing ””: 1 > sinx x > cos x. Since cos 0 = 1, from ”S.T.” sin x =1 x→0 x lim
(9) 13
Examples (discussed in class): tan x =1 x→0 x sin kx lim =k x→0 x 1 − cos x =0 lim x→0 x 1 − cos x 1 = lim x→0 2 x2 lim
(10) (11) (12) (13)
tan x − sin x 1 = x→0 x3 2 lim
14
One-sided limits (skip definition on p. 87) ¤
-
-
-
-
-
-
Functions with 1-sided limits. x x = 1 , lim = −1 , f (0) =? lim x→0− |x| x→0+ |x| lim
x→−1+
q
1 − x2 = 0 ,
lim
x→1−
q
1 − x2 = 0 15
Theorem 6, p.86: Limit of f (x) for x → c exists if and only if L.H. and R.H. limits at x → c− , c+ exist and have the same value (in which case, this also will be the value of the limit of f ) .
16
-
-
-
-
-
Tricky functions with 2- or 1-sided limits. lim x sin
x→0
√ 1 1 x sin = 0 = 0 , lim x x x→0+
17
Continuity at a point x = c (p. 93, or Continuity Test, p. 94): f (c) = lim f (x) x→c
for an interior point (and similarly for an endpoint with corresponding one-sided limit). Right-continuous at a point x = c : f (c) = lim f (x) x→c+
Left-continuous at a point x = c : f (c) = lim f (x) x→c−
18
d t
-
-
right-continuous integer ”floor” function
19
Continuous Function (CF) CF on an interval CF Theorem 8, p. 95 f ± g , etc.
Inverse of a CF is a CF: e.g. ex and ln x Composits of CF are CFs: e.g. Theorems 9, 10 on p. 97
q
f (x) , f (x) = 1 − x2
Continuous extension to a point: e.g. F (x) = sin x /x , x = 6 1; F (0) = 1 20
Limits involving ∞
x → ±∞ (skip p. 104) +
+
-
-
-
-
Limits of a rational function with the same power of denom. and numerator. Horizontal asymptote(s) - lim(s) of f (x) as x → ±∞ 21
Non-algebraic functions x3 x , x sin 1 , etc. , e x |x|3 + 1
-
-
Oblique and vertical asymptotes + + -
-
-
-
22
Derivatives f (x + h) − f (x) = h→0 h f (z) − f (x) = lim z→x z−x
f ′(x) = lim
If the limit exists, this is derivative a.k.a:
(14) (15) at a point x,
• slope of the graph at x • slope of the tangent to the graph at x 23
• rate of change of f with respect to x
Derivative as a function x is not ”frozen” anymore; can consider a new function g(x) = f ′(x) Other notations f ′(x) = y ′ =
df d dy f (x) = . . . = = dx dx dx
df g(a) = dx x=a
24
Examples:
or
d 1 x−z 1/z − 1/x 1 = lim = lim = − z→x z→x zx(z − x) z−x x2 dx x d 1 1 =− 2 x dx x
(16)
1/z 2 − 1/x2 x2 − z 2 d 1 1 = lim = lim = −2 z→x z→x z 2x2(z − x) dx x2 z−x x3 d x d 1 = 1+ dx x−1 dx x − 1
=0−
1 (x − 1)2 25
One-sided derivatives From right: f (x + h) − f (x) f (z) − f (x) = lim z−x h h→0+ z→x+
f ′(x) = lim From left:
f (x + h) − f (x) f (z) − f (x) = lim h z−x h→0− z→x−
f ′(x) = lim
Example: |x|′ = 1 for x > 0, = −1 for x < 0 and is not defined at x = 0 where only r.-h. or l.-h. derivatives exist. (This was a ”corner”;qother cases with no derivative may include ”cusp” as |x|, vertical tangent
as x1/3 and a discontinuity of the original function as |x|/x. Graphics in class.) 26
Theorem 3.1. If f (x) has a derivative at x = c it is continuous at x = c. Consider identity f (c + h) − f (c) ·h h and take the limit of both sides as h → 0. Note: Converse is false, e.g. |x|. f (c + h) = f (c) +
27
Differentiation rules
(af (x) + bg (x))′ = af ′ + bg ′
(17)
Proof. Consider af (z) + bg (z) − af (x) − bg (x) a[f (z) − f (x)] + b[g(z) − g (x)] ≡ z−x z−x and take the limit z → x.
df (z) ′ (f (ax)) = a dz
(18) z=ax
Example: (sin(ωx))′ = ω cos(ωx) 28
[f (x) · g (x)]′ = f ′g + f g ′
(19)
Proof. Consider f (z )g(z ) − f (x)g(x) [f (z) − f (x)]g(z) + f (x)[g(z) − g(x)] ≡ z−x z−x and take the limit z → x. Example: (x · x)′ = 1 · x + x · 1 = 2x 29
1 !′ f
f′ = −f 2
(20)
Proof. Consider 1/f (z) − 1/f (x) f (x) − f (z) ≡ z−x f (z)f (x)(z − x) and take the limit z → x. Example: (1/x)′ = −1/x2
f g
!′
f ′ · g − g′ · f = g2
(21) 30
Derivatives of elementary functions (xn)′ = nxn−1 , any n
(22)
(sin x)′ = cos x , (cos x)′ = − sin x
(23)
x ′ = ex , x ′ = ex ln a ′ = ax · ln a (e ) (a )
(24)
(ln x)′ = 1/x
(25)
31
Trigonometric functions Earlier: (sin x)′ = cos x , (cos x)′ = − sin x and (tan x)′ = 1/ cos2 x
(26)
Other basic examples: 1/ cos x , 1/ sin x , cot x , . . . Simple harmonic motion: y(t) = A sin(ωt) ,
dy = Aω cos(ωt) dt
d2y = −Aω 2 sin(ωt) ≡ −ω 2y(t) 2 dt
(27) (28)
32
Chain rule (f (g (x)))′ =
df dg · ≡ (f (g))′ · (g(x))′ dg dx
(29)
”Proof”. Let u = g(z) , v = g(x) df dg f (u) − f (v) f (u) − f (v) u − v = lim · = · z→x z→x z−x u−v z−x dg dx
(f (g (x)))′ = lim
Simple example: (f (ax))′ = af ′(ax)
33
du dx du (sin u(x))′ = [cos u(x)] dx du (eu)′ = eu dx 1 du (ln u)′ = u dx (u(x)n)′ = nun−1
q
x2 + 1
′
(30) (31) (32) (33)
1 = q · (2x) 2 2 x +1 34
Example
2 e−x
′
2
= −2xe−x
I- M -
-
-
-
I- M
-
35
Example: ′ 2 sin(x ) = 2x cos(x2)
I M I M -
-
36
Example
−x e−e
′
−x −x −e · e =e
H-ã- L H- - ã- L
-
-
37
Implicit differentiation Let F (x, y) = 0 where F is a simple known function (e.g. F = x − y 2 describing a parabola). Then F x′ + Fy′
dy =0 dx
(34)
and dy = −Fx′ /Fy′ dx
38
Tangent at (x0 , y0) dy Y = y0 + (x − x0) dx x=x0
(35)
Normal:
Y = y0 −
dy dx x=x0
!−1
(x − x0)
(36)
39
Parabola: y 2 = x , 2y
dy dx
=1,
dy 1 = 2y dx
Tangent and normal: Y = y0 +
1 (x − x0) , Y = y0 − (2y0)(x − x0) 2y0
-
-
-
-
40
Ellipse: dy (x/a)2+(y/b)2 = 1 , 2x/a2+2y/b2 =0, dx
dy x b2 =− 2 ya dx
Tangent and normal: y0 a2 x 0 b2 (x − x0) (x − x0) , Y = y0 + Y = y0 − x 0 b2 y0 a2
+
-
-
41
Hyperbola: x2 − y 2 = 1 , 2x − 2y
dy dx
=0,
dy x = y dx
Tangent and normal: y x Y = y0 + 0 (x − x0) , Y = y0 − 0 (x − x0) x0 y0
-
-
-
-
-
-
42
Inverse Functions Consider y = f (x) and solve for x = F (y) (select only one branch, if several). Then, swap y and x. Then, y = F (x) , with (f (F (x))) = x is the inverse function (F ≡ f −1 in textbook). Examples: f = x2 , F = sin x , F = arcsin x, etc.
√ x, f = ex , F = ln x, f =
Note: range of f becomes the domain of F , but the domain of f becomes range of F for monotonic f only. Examples: ex (monotonic) and x2 or sin x (non-monotonic). 43
Note (f (F (x))) = x for all x in the domain of F , while F (f (x)) = x in the entire domain of f for monotonic f only. E.g.: eln x = x for 0 < x < ∞ , and ln (ex) = x for −∞ < x < ∞ sin(arcsin x) = x for − 1 ≤ x ≤ 1 , but arcsin(sin x) 6= x , for |x| > π/2
44
Primitive example: f = x − 1 , F = x + 1
-
-
-
+
-
-
45
Primitive example: f = x/2 + 1 , F = 2x − 2
+ -
f (F (x)) = 12 · (2x − 2) + 1 = x
-
-
-
46
Example: f = x2 , F =
√ x 1 (f )′ = 2x , (F )′ = 2√ x
Consider (x0 = 2 , y0 = 4) , (X0 = 4, Y0 = 2): (f )′ = 4 , (F )′ = 1 4
47
Example: f = x2 − 2 , F =
√ x+2 (f )′ = 2x , (F )′ = √ 1
2 x+2
+
Consider (x0 = 3 , y0 = 7) , (X0 = 7, Y0 = 3): (f )′ = 6 , (F )′ = 1 6
-
-
48
Example: f = ex , F = ln x
H L H L
-
-
49
Logarithm y = ln x ey = x ey · y ′ = 1 1 1 y′ = y = e x
50
Example: f = sin x , F = arcsin x
H L -
-
-
-
H L
-
-
51
arcsin y = arcsin x sin y = x (cos y) · y ′ = 1 y′ = =q
1 = cos y
1 1 − sin2 y
=q
1 1 − x2
52
Example: f = tan x , F = arctan x
H L -
-
H L
-
-
53
arctan y = arctan x tan y = x (1/ cos2 y) · y ′ = 1 y′ = = cos2 y =
1 = 1/ cos2 y
1 1 = tan2 y + 1 x2 + 1
54
General y = F (x) f (y) = x df · y′ = 1 dy 1 dF ′ = y ≡ df dx dy y=F (x)
55
Logarithmic functions and differentiation (ln u(x))′ =
1 · (u)′ u
Examples
(ln bx)′ =
(ln |x|)′ =
1 b = bx x
1 1 · (|x|)′ = , x 6= 0 x |x| 56
Recall: ax = ex ln a , loga x =
ln x , a > 0 , a 6= 1 ln a
(37)
x ′ = ex ln a ′ = ax · ln a (a )
(loga x)′ =
1 x ln a
n ′ = en ln x ′ = n n ln x (x ) e = nxn−1
x
57
x ′ = ex ln x ′ = ex ln x ln x + x = xx(ln x + 1) (x )
x
Remarkable limit: lim (1 + x)1/x = e
x→0
(38)
58
Logarithmic differentiation Let y=
P (x)Q(x) R(x)
ln y = ln P + ln Q − ln R (Q)′ (R)′ (P )′ ′ + − y /y = P
Q
R
P (x)Q(x) (P )′ (Q)′ (R)′ y′ = + · − P R(x) Q R "
#
59
Inverse trigonometric functions (arcsin x)′ = q
1
, |x| < 1
(39)
1 , −∞ < x < ∞ (arctan x)′ = 2 x +1
(40)
1 − x2
π −arctan x. Now, arccos x = π2 −arcsin x and cot−1 x = 2 Thus
(arccos x)′ = − q
′ −1 cot x = −
1
, |x| < 1
(41)
1 , −∞ < x < ∞ x2 + 1
(42)
1 − x2
60
sec−1(x) = arccos
1
1 , csc−1(x) = arcsin x
x ′ −1 1 ′ 1 −1 · 2 sec (x) = arccos = −q x 1 − (1/x)2 x
=
1
q
|x| x2 − 1
, |x| > 1
′ 1 ′ −1 csc (x) = arcsin =q
x
=−
1
q
|x|
x2 − 1
−1 2 1 − (1/x)2 x 1
·
, |x| > 1 61
Related rates Suggested notations: V - volume, A - area, L - length/distance, r , R - radii, y Y, h, H - vertical position, x, X -horizontal position, v, V velocity, t - time Sphere: V=
4 3 πR , A = 4πR2 3
(43)
1 Abase · h 3
(44)
Cone: V=
62
Circle:
A = πr 2
dA/dt = 2πr · dr/dt: -
-
-
-
63
Sphere:
V = 43 πr 3 dV = 4πr 2 · dr = A · dr dt dt dt -
-
-
-
64
Cone:
1 πr 2(h) · h = V =3
2 V h 1 = 3 π R(H) H · h = H03 · h3 dV = V0 · 3h2 dh = A(h) · dh dt dt dt H3
65
”Coffee maker” :
1 + dV2 = 0 V1 + V2 = const , dV dt dt
dV1 dh 2 dt = πr (h) · dt dV2 2 dY dt = πR · dt
dY dh 1 = − 2 r 2(h) · R dt dt 66
An a(t) × b(t) rectangle: A = ab , P = 2(a + b) , D =
q
a 2 + b2
dA db da =a +b dt dt dt dP da db =2 + dt dt dt
da db dD 1 d 2 1 2 a +b = a +b = 2D dt dt D dt dt
67
Distance between two moving points:
H
L
L= H
L
q
(x − X)2 + (y − Y )2
1 d dL = (x − X)2 + (y − Y )2 = dt 2L dt
1 dx dX dy dY = ) (x − X)( − ) + (y − Y )( − dt dt dt dt L
68
Police car: X ≡ 0, dY /dt = −V , y ≡ 0, dx/dt = v dL 1 d 2 2 = x +Y = dt 2L dt
1 dx dY = x +Y dt L dt
v=
=
1 (xv − Y V ) L
1 (L · dL/dt + Y V ) x
69
Angle with horizontal (X, Y = 0, L = x/ cos θ):
q
x2 + y 2 =
1 dθ dy dx 1 tan θ = y/x , x − y = dt cos2 θ dt x2 dt
dθ dy dx 1 = 2 x −y dt L dt dt
Balloon: x = const , dy/dt = V . Aircraft: y = const , dx/dt = −v .
70
+ H - L
-
Tangent line and error (for a parabola): Y (x) = y (a) + y ′(a)(x − a) y(x) − Y (x) = x2 − a2 − 2a(x − a) = (x − a)2 71
+
72
-
H L + H - L -
-
H
H L - - H - LL
-
-
73
Differential: dx - independent variable dy = y ′(x) dx
74
D
75
f (x + dx) ≃ f (x) + df = f (x) + f ′(x) · dx Examples (small x instead of dx; approximation only near x = 0): (1 + x)2 ≃ 1 + 2x
(45)
p
1 + x ≃ 1 + x/2
(47)
ex ≃ 1 + x
(49)
1/(1 + x) ≃ 1 − x
(1 + x)k ≃ 1 + kx ln(1 + x) ≃ x
(46) (48) (50)
76
-
77
H
L H
L
Absolute maximum: f (c) = M , f (x) ≤ M for every x in the domain of f . Theorem. On a closed domain [a, b] any continuous f (x) will have an absolute maximum.
78
Local maximum: f (c) = M , f (x) ≤ M for every x on some open interval containing c. Theorem. For any differentiable f (x) a local maximum will have a zero derivative: f (c) = M , (f (x))′x=c = 0
(51)
(but, the reverse can be false: e.g. x3)
79
Critical and end points:
• endpoint(s) • zero derivative • no derivative (e.g |x| or
q
|x|)
80
E.g.: critical point - no extrema: