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UP Academic League of Chemical Engineering Students (UP ALCHEMES) Academic Affairs Committee - Reviews and Tutorials Series, AY 2014-2015 Math 53 First Exam (REVIEWER) I. o
Introduction to derivatives: derivative as a slope of tangent lines
f
Suppose
lim
f ( x 1 +∆ x )−f ( x 1)
∴
eq’n of tangent line at
y−f ( x1 ) =m(x−x 1)
x → ∆x
is
5.
Derivatives of Trigonometric Functions.
.
f ( x 1 +∆ x )−f ( x 1) ∆x
f −1
∆x
x →∆x
derivative of
f
The dom dom
f
±∞
is
x=x 1
, then,
.
defined by
f ( x 1+ ∆ x )−f ( x1 )
f −1 = lim
[ ]
P
eq’n of the tangent line The function
is called the
with respect to
f −1
Quotient Rule. VII. ' ' f ( x) g ( x ) f ( x )−f (x) g ( x) Dx = g (x) g (x)2
If the limit DNE, ie.,
lim
o
c.
,
is true.
∆x
x → ∆x
I.
P
is continuous at pt.
D x [ f ( x )∙ g(x ) ] =f ' ( x )+ g ' ( x)
VI.
x
6.
x
consists of all
b.
Dx [ cos x ] =−sin x
c.
Dx [ tan x ] =sec 2 x
d.
D x [ cot x ]=−csc 2 x
e.
Dx [ sec x ] =sec x tan x
f.
D x [ csc x ] =−csc x cot x
y=f ( g ( x ) )
If
for which the limit exists. III.
1. 2.
Dx [ c ] =0
cϵR
Power Rule.
+¿ n ϵ Z¿
dy dx
XII. Solve for
3.
cϵR
, V.
4.
f ,g
f
XIV.
x
x1
D x [ f ( x )± g( x )] =f ( x ) g ' ( x )+ g ( x)f ' (x ) Product Rule.
IV.
)(
(
XVII. Differentiability of a function XVIII.
Theorem: If then
f'
XIX.If
f
))
dy dy dy 2 − cot y+ x −csc y =2 x dx dx dx
dy 2 y− y 2 cos x+ cot y = dx 2 y sin x + x csc 2 y −2 x
XVI.
D x [ cf (x ) ] =c f ' (x)
are differentiable at
(
2
a.
b.
Solution: XV.
y cos x+sin x 2 y
is differentiable at
.
y 2 sin x−x cot y=2 xy
XIII.
D x [ n x n−1 ]
IV.
, then,
X. Implicit differentiation XI. Example:
x
II. Normal Line to the T.L. III. II. Techniques of differentiation
u=g ( x )
and
dy dy du = = dx du dx
IX.
in the
( dxd , D )
D x [ sin x ] =cos x
Chain Rule. VIII.
.
a.
f
is differentiable at
is continuous at is defined at
differentiable at
x
, then:
x1
x1
.
, but not
x1
,
1.
f'
2.
f
3.
f'
is continuous (essential) at
'
has a vertical T.L at has no T.L at
x=x 1
x1
x1
XX. XXI. XXII. V. Rectilinear motion and derivatives as (Instantaneous) rates of change '
v ( t )=s (t)
1. XXIII.
XXV.
iii.
i.
VI.
- particle is moving to the
v <0
- instantaneous speed
a ( t )=v ' ( t ) =s ' ' (t)
2. XXIV. i. ii.
VII.
a<0
a<0
- particle is speeding up
v
and
a
have the same
x
close to
f
is differentiable at
x0
x0
.
,
f ( x ) ≈ f ( x 0 ) +f ' ( x 0 ) (x−x 0)
away and starts to rise at a rate of 10
v >0
a>0
XXX. Related rates XXXI. Example: XXXII. A boy observes a hot air balloon on the ground through a telescope. The balloon stands 100m
Remarks: A particle is If
- particle is slowing down
XXVI. Linear approximation and differentials XXVII.
XXIX.
left iii.
a>0
From (ii), if
For
- particle is moving to the
v =0
XXVIII. Suppose
right ii.
v <0
sign, then the particle is speeding up. Otherwise, the particle is slowing down.
Remarks:
v >0
If
m s
. At
what rate is the angle of elevation of the - particle is speeding up - particle is slowing down
telescope changing when the angle is
XXXIII.
dh m =10 dt s
dθ π =? at θ= dt 6 tan θ=
h dθ 1 dh sec 2 θ = 100 dt 100 dt
dθ 1 dh = cos 2 θ dt 100 dt dθ θ 1 3 3 rad at θ= = ∙ ∙10= dt 6 100 4 40 s