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Tancendental Functions
Exponential Functions
Logarithmic functions
DERIVATIVE
• Recall your concept of a slope;
Tangent Line
What happens to the graph as the
change in x approaches 0?
Formula
Example
•Find an equation of the tangent line to
the parabola y = x2
-1 at point (2,3).
Sketch the parabola and show the
segment of the tangent line at (2,3).
Find the general formula for the slope
of the tangent line of this function.
What is the slope when x = 5?
2
3y x= −
( ) ( )2 2
0
3 3
lim
h
x h x
y
h→
+ − − −
′ =
2y x′ =
0
lim2
h
y x h
→
′ = +
3.1 Derivative of a Function
A function is differentiable if it has a
derivative everywhere in its domain.
It must be continuous and smooth.
Functions on closed intervals must
have one-sided derivatives defined
at the end points.
Derivative of a Function
To be differentiable, a function must be continuous
and smooth.
Derivatives will fail to exist at:
corner
( )f x x=
cusp
( )
2
3
f x x=
vertical tangent
( ) 3
f x x=
discontinuity
( )
1, 0
1, 0
x
f x
x
− <
=
≥
3.2 Differentiability
Most of the functions we study in calculus will be differentiable.
Differentiability
If f has a derivative at x = a, then f is continuous at x = a.
Since a function must be continuous to have a derivative,
if it has a derivative then it is continuous.
3.2 Differentiability
( )
1
2
f a′ =
( ) 3f b′ =
Intermediate Value Theorem for Derivatives
Between a and b, must take
on every value between and .
f ′
1
2
3
If a and b are any two points in an interval on which f is
differentiable, then takes on every value between
and .
f ′ ( )f a′
( )f b′
Differentiability
If the derivative of a function is its slope, then for a
constant function, the derivative must be zero.
( ) 0
d
c
dx
=
example: 3y =
0y′ =
The derivative of a constant is zero.
3.3 Rules for Differentiation
We saw that if , .
2
y x= 2y x′ =
This is part of a pattern.
( ) 1n nd
x nx
dx
−
=
examples:
( ) 4
f x x=
( ) 3
4f x x′ =
8
y x=
7
8y x′ =
power rule
Rules for Differentiation
( ) 1n nd
x nx
dx
−
=
Rules for Differentiation
Proof:
h
xhx
x
dx
d nn
h
n −+
=
→
)(
lim
0
h
xhhnxx
x
dx
d nnnn
h
n −+++
=
−
→
...
lim
1
0
h
hhnx
x
dx
d nn
h
n ++
=
−
→
...
lim
1
0
1
0
lim −
→
= n
h
n
nxx
dx
d
( )
d du
cu c
dx dx
=
examples:
1n nd
cx cnx
dx
−
=
constant multiple rule:
5 4 4
7 7 5 35
d
x x x
dx
= ⋅ =
Rules for Differentiation
(Each term is treated separately)
( )
d du
cu c
dx dx
=constant multiple rule:
sum and difference rules:
( )
d du dv
u v
dx dx dx
+ = + ( )
d du dv
u v
dx dx dx
− = −
4
12y x x= +
3
4 12y x′ = +
4 2
2 2y x x= − +
3
4 4
dy
x x
dx
= −
3.3 Rules for Differentiation
Find the horizontal tangents of:
4 2
2 2y x x= − + 3
4 4
dy
x x
dx
= −
Horizontal tangents occur when slope = zero.
3
4 4 0x x− =
3
0x x− =
( )2
1 0x x − =
( ) ( )1 1 0x x x+ − =
0, 1, 1x = −
Substituting the x values into the
original equation, we get:
2, 1, 1y y y= = =
(The function is even, so we
only get two horizontal
tangents.)
Rules for Differentiation
4 2
2 2y x x= − +
2y =
1y =
Rules for Differentiation
4 2
2 2y x x= − +
First derivative
(slope) is zero at:
0, 1, 1x = −
3
4 4
dy
x x
dx
= −
Rules for Differentiation
product rule:
( )
d dv du
uv u v
dx dx dx
= + Notice that this is not just the
product of two derivatives.
This is sometimes memorized as: ( )d uv u dv v du= +
( )( )2 3
3 2 5
d
x x x
dx
 + + 
( )5 3 3
2 5 6 15
d
x x x x
dx
+ + +
( )5 3
2 11 15
d
x x x
dx
+ +
4 2
10 33 15x x+ +
=( )2
3x + ( )2
6 5x + ( )3
2 5x x+ + ( )2x
4 2 2 4 2
6 5 18 15 4 10x x x x x+ + + + +
4 2
10 33 15x x+ +
Rules for Differentiation
product rule:
( )
d dv du
uv u v
dx dx dx
= +
Rules for Differentiation
Proof
h
xvxuhxvhxu
uv
dx
d
h
)()()()(
lim)(
0
−++
=
→
add and subtract u(x+h)v(x)
in the denominator
h
xvhxuxvhxuxvxuhxvhxu
uv
dx
d
h
)()()()()()()()(
lim)(
0
+−++−++
=
→
( ) ( )





 −++−++
=
→ h
xuhxuxvxvhxvhxu
uv
dx
d
h
)()()()()()(
lim)(
0
dx
du
v
dx
dv
uuv
dx
d
+=)(
quotient rule:
2
du dv
v u
d u dx dx
dx v v
−
 
= 
 
or 2
u v du u dv
d
v v
− 
= 
 
3
2
2 5
3
d x x
dx x
+
+
( )( ) ( )( )
( )
2 2 3
2
2
3 6 5 2 5 2
3
x x x x x
x
+ + − +
=
+
Rules for Differentiation
Higher Order Derivatives:
dy
y
dx
′ = is the first derivative of y with respect to x.
2
2
dy d dy d y
y
dx dx dx dx
′
′′ = = =
is the second derivative.
(y double prime)
dy
y
dx
′′
′′′ = is the third derivative.
( )4 d
y y
dx
′′′= is the fourth derivative.
We will learn
later what these
higher order
derivatives are
used for.
Rules for Differentiation
Rules for Differentiation
Suppose u and v are functions that are differentiable at
x = 3, and that u(3) = 5, u’(3) = -7, v(3) = 1, and v’(3)= 4.
Find the following at x = 3 :
)(.1 uv
dx
d
'')( vuuvuv
dx
d
+= 8)7)(1()3(5 =−+






v
u
dx
d
.2 2
''
v
uvvu
v
u
dx
d −
=





2
1
)4)(5()7)(1( −−
27−=






u
v
dx
d
.3 2
''
u
vuuv
u
v
dx
d −
=





2
5
)7)(1()4)(5( −−
25
27
=
Rules for Differentiation






hi
ho
dx
d
))((
)()()()(
hoho
hidhohodhi −
Consider a graph of displacement (distance traveled) vs. time.
time (hours)
distance
(miles)
Average velocity can be found by
taking:
change in position
change in time
s
t
∆
=
∆
t∆
s∆
A
B
( ) ( )
ave
f t t f ts
V
t t
+∆ −∆
= =
∆ ∆
The speedometer in your car does not measure average
velocity, but instantaneous velocity.
( )
( ) ( )
0
lim
t
f t t f tds
V t
dt t∆ →
+∆ −
= =
∆
(The velocity at one
moment in time.)
Velocity and other Rates of Change
Velocity and other Rates of Change
Velocity is the first derivative of position.
Acceleration is the second derivative
of position.
Example: Free Fall Equation
21
2
s g t=
Gravitational
Constants:
2
ft
32
sec
g =
2
m
9.8
sec
g =
2
cm
980
sec
g =
21
32
2
s t= ⋅
2
16s t= 32
ds
V t
dt
= =
Speed is the absolute value of velocity.
Velocity and other Rates of Change
Acceleration is the derivative of velocity.
dv
a
dt
=
2
2
d s
dt
= example:
32v t=
32a =
If distance is in: feet
Velocity would be in:
feet
sec
Acceleration would be in:
ft
sec
sec
2
ft
sec
=
Velocity and other Rates of Change
Rates of Change:
Average rate of change =
( ) ( )f x h f x
h
+ −
Instantaneous rate of change = ( )
( ) ( )
0
lim
h
f x h f x
f x
h→
+ −
′ =
These definitions are true for any function.
( x does not have to represent time. )
Velocity and other Rates of Change
For a circle: 2
A rπ=
2dA d
r
dr dr
π=
2
dA
r
dr
π=
Instantaneous rate of change of the area with
respect to the radius.
For tree ring growth, if the change in area is constant then dr
must get smaller as r gets larger.
2dA r drπ=
Velocity and other Rates of Change
from Economics:
Marginal cost is the first derivative of the cost function, and
represents an approximation of the cost of producing one
more unit.
Velocity and other Rates of Change
Example 13:
Suppose it costs: ( ) 3 2
6 15c x x x x= − +
to produce x stoves. ( ) 2
3 12 15c x x x′ = − +
If you are currently producing 10 stoves,
the 11th
stove will cost approximately:
( ) 2
10 3 10 12 10 15c′ = × − × +
300 120 15= − +
$195=
marginal cost
The actual cost is: ( ) ( )11 10C C−
( ) ( )3 2 3 2
11 6 11 15 11 10 6 10 15 10= − × + × − − × + ×
770 550= − $220= actual cost
Velocity and other Rates of Change
Derivatives of Trigonometric Functions
π
2
π
0
2
π
−
π−
Consider the function ( )siny θ=
We could make a graph of the slope:
θ slope
1−
0
1
0
1−
Now we connect the dots!
The resulting curve is a cosine curve.
( )sin cos
d
x x
dx
=
Derivatives of Trigonometric Functions
Derivatives of Trigonometric Functions
h
xhx
x
dx
d
h
sin)sin(
limsin
0
−+
=
→
h
xxhhx
x
dx
d
h
sincossincossin
limsin
0
−+
=
→
h
xh
h
hx
x
dx
d
hh
cossin
lim
)1(cossin
limsin
00 →→
+
−
=
h
xhhx
x
dx
d
h
cossin)1(cossin
limsin
0
+−
=
→
Proof
Derivatives of Trigonometric Functions
h
xh
h
hx
x
dx
d
hh
cossin
lim
)1(cossin
limsin
00 →→
+
−
=
= 0 = 1
( )sin cos
d
x x
dx
=
Derivatives of Trigonometric Functions
h
xhx
x
dx
d
h
cos)cos(
limcos
0
−+
=
→
h
xxhhx
x
dx
d
h
cossinsincoscos
limcos
0
−−
=
→
h
xh
h
hx
x
dx
d
hh
sinsin
lim
)1(coscos
limcos
00 →→
−
−
=
h
xhhx
x
dx
d
h
sinsin)1(coscos
limcos
0
−−
=
→
Find the derivative of cos x
Derivatives of Trigonometric Functions
= 0 = 1
h
xh
h
hx
x
dx
d
hh
sinsin
lim
)1(coscos
limcos
00 →→
−
−
=
( )cos sin
d
x x
dx
= −
We can find the derivative of tangent x by using the
quotient rule.
tan
d
x
dx
sin
cos
d x
dx x
( )
2
cos cos sin sin
cos
x x x x
x
× − ×−
2 2
2
cos sin
cos
x x
x
+
2
1
cos x
2
sec x
( ) 2
tan sec
d
x x
dx
=
Derivatives of Trigonometric Functions
Derivatives of the remaining trig functions can
be determined the same way.
sin cos
d
x x
dx
=
cos sin
d
x x
dx
= −
2
tan sec
d
x x
dx
=
2
cot csc
d
x x
dx
= −
sec sec tan
d
x x x
dx
= ×
csc csc cot
d
x x x
dx
= − ×
Derivatives of Trigonometric Functions
Derivatives of Trigonometric Functions
Jerk A sudden change in acceleration
Definition Jerk
Jerk is the derivative of acceleration. If a body’s position
at time t is s(t), the body’s jerk at time t is
3
3
2
2
)(
dt
sd
dt
vd
dt
da
tj ===
Consider a simple composite function:
6 10y x= −
( )2 3 5y x= −
If 3 5u x= −
then 2y u=
6 10y x= − 2y u= 3 5u x= −
6
dy
dx
= 2
dy
du
= 3
du
dx
=
dy dy du
dx du dx
= ⋅
6 2 3= ⋅
Chain Rule
dy dy du
dx du dx
= ⋅Chain Rule:
example: ( ) sinf x x= ( ) 2
4g x x= − Find: ( ) at 2f g x′ =o
( ) cosf x x′ = ( ) 2g x x′ = ( )2 4 4 0g = − =
( ) ( )0 2f g′ ′⋅ ( ) ( )cos 0 2 2⋅ ⋅ 1 4⋅ 4=
Chain Rule
If is the composite of and ,
then:
f go ( )y f u= ( )u g x=
( ) ( ) atat xu g x
f g f g=
′ ′ ′= ⋅o )('))((' xgxgf •=
( )( ) ( )2
sin 4f g x x= −
( )2
sin 4y x= −
siny u=
2
4u x= −
cos
dy
u
du
= 2
du
x
dx
=
dy dy du
dx du dx
= ⋅
cos 2
dy
u x
dx
= ⋅
( )2
cos 4 2
dy
x x
dx
= − ⋅
( )2
cos 2 4 2 2
dy
dx
= − ⋅ ⋅
( )cos 0 4
dy
dx
= ⋅
4
dy
dx
=
Chain Rule
Here is a faster way to find the derivative:
( )2
sin 4y x= −
( ) ( )2 2
cos 4 4
d
y x x
dx
= − ⋅ −
( )2
cos 4 2y x x= − ⋅
Differentiate the outside function...
…then the inside function
At 2, 4x y= =
Chain Rule
( )2
cos 3
d
x
dx
( )
2
cos 3
d
x
dx
  
( ) ( )2 cos 3 cos 3
d
x x
dx
⋅  
( ) ( ) ( )2cos 3 sin 3 3
d
x x x
dx
⋅− ⋅
( ) ( )2cos 3 sin 3 3x x− ⋅ ⋅
( ) ( )6cos 3 sin 3x x−
The chain rule can be used
more than once.
(That’s what makes the
“chain” in the “chain rule”!)
Chain Rule
Derivative formulas include the chain rule!
1n nd du
u nu
dx dx
−
= sin cos
d du
u u
dx dx
=
cos sin
d du
u u
dx dx
= − 2
tan sec
d du
u u
dx dx
=
etcetera…
Chain Rule
Chain Rule
Find
)3cos( 2
xxy += )16)(3sin( 2
++−= xxx
dx
dy
))sin(cos(xy =
)24(cos 33
xxy +=
)sin)(cos(cos xx
dx
dy
−=
)212))(24sin()(24(cos3 2332
++−+= xxxxx
dx
dy
))24sin()(24(cos)636( 3322
xxxxx
dx
dy
+−++=
dx
dy
The chain rule enables us to find the slope of
parametrically defined curves:
dy dy dx
dt dx dt
= ⋅
dy
dydt
dx dx
dt
=
The slope of a parametrized
curve is given by:
dy
dy dt
dxdx
dt
=
Chain Rule
2 2
1x y+ =
This is not a function,
but it would still be
nice to be able to find
the slope.
2 2
1
d d d
x y
dx dx dx
+ = Do the same thing to both sides.
2 2 0
dy
x y
dx
+ =
Note use of chain rule.
2 2
dy
y x
dx
= −
2
2
dy x
dx y
−
= dy x
dx y
= −
Implicit Differentiation
2
2 siny x y= +
2
2 sin
d d d
y x y
dx dx dx
= +
This can’t be solved for y.
2 2 cos
dy dy
x y
dx dx
= +
2 cos 2
dy dy
y x
dx dx
− =
( ) 22 cos
dy
xy
dx
=−
2
2 cos
dy x
dx y
=
−
This technique is called
implicit differentiation.
1 Differentiate both sides w.r.t. x.
2 Solve for .
dy
dx
Implicit Differentiation
Implicit Differentiation
Implicit Differentiation Process
1. Differentiate both sides of the equation with respect to x.
2. Collect the terms with dy/dx on one side of the equation.
3. Factor out dy/dx .
4. Solve for dy/dx .
Find the equations of the lines tangent and normal to the
curve at .
2 2
7x xy y− + = ( 1,2)−
2 2
7x xy y− + =
2 2 0
dydy
x yx y
dxdx
 − + =+  
Note product rule.
2 2 0
dy dy
x x y y
dx dx
− − + =
( ) 22
dy
y xy x
dx
= −−
2
2
dy y x
dx y x
−
=
−
( )
( )
2 2 1
2 2 1
m
− −
=
⋅ − −
2 2
4 1
+
=
+
4
5
=
Implicit Differentiation
Find the equations of the lines tangent and normal to the
curve at .
2 2
7x xy y− + = ( 1,2)−
4
5
m =
tangent:
( )
4
2 1
5
y x− = +
4 4
2
5 5
y x− = +
4 14
5 5
y x= +
normal:
( )
5
2 1
4
y x− = − +
5 5
2
4 4
y x− = − −
5 3
4 4
y x= − +
Implicit Differentiation
Find if .
2
2
d y
dx
3 2
2 3 7x y− =
3 2
2 3 7x y− =
2
6 6 0x y y′− =
2
6 6y y x′− = −
2
6
6
x
y
y
−
′ =
−
2
x
y
y
′ =
2
2
2y x x y
y
y
′⋅ −
′′ =
2
2
2x x
y y
y y
′′ ′= −
2 2
2
2x x
y
y
x
yy
′′ = − ⋅
4
3
2x x
y
y y
′′ = −
Substitute
back into the
equation.
y′
Implicit Differentiation
Implicit Differentiation
Rational Powers of Differentiable Functions
Power Rule for Rational Powers of x
If n is any rational number, then
1−
= nn
nxx
dx
d
Implicit Differentiation
Proof: Let p and q be integers with q > 0.
q
p
xy =
pq
xy =
Raise both sides to the q power
Differentiate with respect to x
11 −−
= pq
px
dx
dy
qy Solve for dy/dx
Implicit Differentiation
1
1
−
−
= q
p
qy
px
dx
dy Substitute for y
1/
1
)( −
−
= qqp
p
xq
px
dx
dy
Remove parenthesis
qpp
p
qx
px
dx
dy
/
1
−
−
= Subtract exponents
q
px
dx
dy qppp )/(1 −−−
=
1)/( −
= qp
x
q
p
dx
dy
Differentiate
Answer
4�3
−3�2
�
�3+�3
Differentiate
Answer
Look at the graph of
x
y e=
The slope at x = 0
appears to be 1.
If we assume this to be
true, then:
0 0
0
lim 1
h
h
e e
h
+
→
−
=
definition of derivative
Derivatives of Exponential and Logarithmic
Functions
Now we attempt to find a general formula for the
derivative of using the definition.
x
y e=
( ) 0
lim
x h x
x
h
d e e
e
dx h
+
→
−
=
0
lim
x h x
h
e e e
h→
⋅ −
=
0
1
lim
h
x
h
e
e
h→
 −
= ⋅ 
 
0
1
lim
h
x
h
e
e
h→
 −
= ⋅  
 
1x
e= ⋅
x
e=
This is the slope at x = 0, which
we have assumed to be 1.
Derivatives of Exponential and Logarithmic
Functions
75
– More Derivatives
4) Exponents
If y = bx
y’ = bx
ln(b)
Therefore
If y = ex
y’ = ex
( )x xd
e e
dx
=
→
77
– More Exciting Derivatives
2) Natural Logs
If y=ln(x),
y’ = 1/x
-chain rule may apply
If y=ln(x2
)
y’ = (1/x2
)2x = 2/x
x
e is its own derivative!
If we incorporate the chain rule: u ud du
e e
dx dx
=
We can now use this formula to find the derivative of
x
a
Derivatives of Exponential and
Logarithmic Functions
( )xd
a
dx
( )ln x
ad
e
dx
( )lnx ad
e
dx
( )ln
lnx a d
e x a
dx
⋅
Incorporating the chain rule:
( ) lnu ud du
a a a
dx dx
=
Derivatives of Exponential and
Logarithmic Functions
aaa
dx
d xx
ln=
So far today we have:
u ud du
e e
dx dx
= ( ) lnu ud du
a a a
dx dx
=
Now it is relatively easy to find the derivative of .ln x
3.9 Derivatives of Exponential and
Logarithmic Functions
lny x=
y
e x=
( ) ( )yd d
e x
dx dx
=
1y dy
e
dx
=
1
y
dy
dx e
=
1
ln
d
x
dx x
=
1
ln
d du
u
dx u dx
=
Derivatives of Exponential and
Logarithmic Functions
To find the derivative of a common log function, you
could just use the change of base rule for logs:
log
d
x
dx
ln
ln10
d x
dx
=
1
ln
ln10
d
x
dx
=
1 1
ln10 x
= ⋅
The formula for the derivative of a log of any base
other than e is:
1
log
ln
a
d du
u
dx u a dx
=
Derivatives of Exponential and
Logarithmic Functions
u ud du
e e
dx dx
= ( ) lnu ud du
a a a
dx dx
=
1
log
ln
a
d du
u
dx u a dx
=
1
ln
d du
u
dx u dx
=
Derivatives of Exponential and
Logarithmic Functions
84
– More Derivatives
4b) Exponents and chain rule
If y = bkx
y’ = bkx
ln(b)k
Or more generally:
If y = bg(x)
y’ = bg(x)
ln(b) X dg(x)/dx
85
2.1.2 – More Derivatives
4b) Exponents and chain rule
If y = 52x
y’ = 52x
ln(5)2
Or more complicated:
If y = 5sin(x)
y’ = 5sin(x)
ln(5) * cos(x)
Derivatives of Exponential and Logarithmic
Functions
x
ey 2
=
2
3x
y =
3
ln xy =
Find y’
x
ey 2
2'=
)2)(3ln(3'
2
xy x
=
x
x
x
y
3
)3(
1
' 2
3
==
Derivatives of Exponential and Logarithmic
Functions
Logarithmic differentiation
Used when the variable is in the base and the exponent
y = xx
ln y = ln xx
ln y = x ln x
x
x
x
dx
dy
y
ln
11
+





=
( )xy
dx
dy
ln1+=
( )xx
dx
dy x
ln1+=
Differentiate
Differentiate
Differentiate
Extrema on an Interval
Extrema of a Function
In calculus, much effort is devoted to determining the behavior of a
function f on an interval I.
Does f have a maximum value on I? Does it have a minimum value?
Where is the function increasing? Where is it decreasing?
In this chapter, you will learn how derivatives can be used to answer
these questions. You will also see why these questions are important in
real-life applications.
Extrema of a Function
A function need not have a minimum or a maximum on an interval. For
instance, in Figure 3.1(a) and (b), you can see that the function f(x) = x2
+ 1
has both a minimum and a maximum on the closed interval [–1, 2], but
does not have a maximum on the open interval (–1, 2).
Figure 3.1(a) Figure 3.1(b)
Extrema of a Function
Moreover, in Figure 3.1(c),
you can see that continuity
(or the lack of it) can affect the
existence of an extremum on
the interval.
This suggests the theorem below.
Figure 3.1(c)
Extrema of a Function
Relative Extrema and Critical Numbers
Relative Extrema and Critical Numbers
In Figure 3.2, the graph of f(x) = x3
– 3x2
has a relative maximum
at the point (0, 0) and a relative minimum at the point (2, –4).
Informally, for a continuous function,
you can think of a relative maximum
as occurring on a “hill” on the graph,
and a relative minimum as occurring
in a “valley” on the graph.
Figure 3.2
Such a hill and valley can occur in two ways.
When the hill (or valley) is smooth and rounded, the graph has a
horizontal tangent line at the high point (or low point).
When the hill (or valley) is sharp and peaked, the graph represents
a function that is not differentiable at the high point (or low point).
Relative Extrema and Critical Numbers
Relative Extrema and Critical Numbers
Example 1 – The Value of the Derivative at Relative Extrema
Find the value of the derivative at each relative extremum
shown in Figure 3.3.
Figure 3.3
Example 1(a) – Solution
At the point (3, 2), the value of the derivative is f'(3) = 0
[see Figure 3.3(a)].
The derivative of is
Figure 3.3(a)
Example 1(b) – Solution
At x = 0, the derivative of f(x) = |x| does not exist because the following
one-sided limits differ [see Figure 3.3(b)].
cont’d
Figure 3.3(b)
Example 1(c) – Solution
The derivative of f(x) = sin x is f'(x) = cos x.
At the point (π/2, 1), the value of the
derivative is f'(π/2) = cos(π/2) = 0.
At the point (3π/2, –1), the value of the
derivative is f'(3π/2) = cos(3π/2) = 0
[see Figure 3.3(c)].
cont’d
Figure 3.3(c)
Note in Example 1 that at each relative extremum, the derivative either is
zero or does not exist. The x-values at these special points are called
critical numbers.
Figure 3.4 illustrates the two types of critical numbers.
Figure 3.4
Relative Extrema and Critical Numbers
Relative Extrema and Critical Numbers
Notice in the definition above that the critical number c has
to be in the domain of f, but c does not have to been in the
domain of f'.
Finding Extrema on a Closed Interval
Theorem 3.2 states that the relative extrema of a function
can occur only at the critical number of the function.
Knowing this, you can use the following guidelines to find
extrema on a closed interval.
Example 2 – Finding Extrema on a Closed Interval
Find the extrema of f(x) = 3x4
– 4x3
on the interval [–1, 2].
Solution:
Begin by differentiating the function.
f(x) = 3x4
– 4x3
Write original function.
f'(x) = 12x3
– 12x2
Differentiate.
Example 2 – Solution
To find the critical numbers on the interval (– 1,2), you
must find all x-values for which f'(x) = 0 and all x-values
for which f'(x) does not exist.
f'(x) = 12x3
– 12x2
= 0 Set f'(x) equal to 0.
12x2
(x– 1) = 0 Factor.
x = 0, 1 Critical numbers
Because f' is defined for all x, you can conclude that
these are the only critical numbers of f.
cont’d
By evaluating f at these two critical numbers and at the
endpoints of [–1, 2], you can determine that the
maximum is f(2) = 16 and the minimum is f(1) = –1, as
shown in the table.
Example 2 – Solution cont’d
The graph of f is shown in Figure 3.5.
Figure 3.5
Example 2 – Solution cont’d
cont’d
In Figure 3.5, note that the critical number x = 0 does not
yield a relative minimum or a relative maximum.
This tells you that the converse of Theorem 3.2 is not true.
In other words, the critical numbers of a function need not
produce relative extrema.
Example 2 – Solution
• Determine the absolute extrema for the following function and
interval[-4,2].
•
First, a review problem:
Consider a sphere of radius 10 cm.
If the radius changes 0.1 cm (a very small amount)
how much does the volume change?
34
3
V rπ=
2
4dV r drπ=
( )
2
4 10cm 0.1cmdV π= ⋅
3
40 cmdV π=
The volume would change by approximately 40π cm3
Related Rates
Now, suppose that the radius is
changing at an instantaneous rate
of 0.1 cm/sec.
34
3
V rπ= 2
4
dV dr
r
dt dt
π=
( )
2 cm
4 10cm 0.1
sec
dV
dt
π
 
= ⋅ 
 
3
cm
40
sec
dV
dt
π=
The sphere is growing at a rate of 40π cm3
/sec .
Note: This is an exact answer, not an approximation like
we got with the differential problems.
Related Rates
Water is draining from a cylindrical tank
at 3 liters/second. How fast is the surface
dropping?
L
3
sec
dV
dt
= −
3
cm
3000
sec
= −
Find
dh
dt
2
V r hπ=
2dV dh
r
dt dt
π=
(r is a constant.)
3
2cm
3000
sec
dh
r
dt
π− =
3
2
cm
3000
secdh
dt rπ
= −
(We need a formula to
relate V and h. )
Related Rates
Steps for Related Rates Problems:
1. Draw a picture (sketch).
2. Write down known information.
3. Write down what you are looking for.
4. Write an equation to relate the variables.
5. Differentiate both sides with respect to t.
6. Evaluate.
Related Rates
Hot Air Balloon Problem:
Given:
4
π
θ =
rad
0.14
min
d
dt
θ
=
How fast is the balloon rising?
Find
dh
dt
tan
500
h
θ =
2 1
sec
500
d dh
dt dt
θ
θ =
( )
2
1
sec 0.14
4 500
dh
dt
π 
= 
 
h
θ
500ft
Related Rates
Hot Air Balloon Problem:
Given:
4
π
θ =
rad
0.14
min
d
dt
θ
=
How fast is the balloon rising?
Find
dh
dt
tan
500
h
θ =
2 1
sec
500
d dh
dt dt
θ
θ = ( )
2
1
sec 0.14
4 500
dh
dt
π 
= 
 
h
θ
500ft
( ) ( )
2
2 0.14 500
dh
dt
⋅ =
1
1
2
4
π
sec 2
4
π
=
ft
140
min
dh
dt
=
Related Rates
4x =
3y =
B
A
5z =
Truck Problem:
Truck A travels east at 40 mi/hr.
Truck B travels north at 30 mi/hr.
How fast is the distance between the
trucks changing 6 minutes later?
r t d⋅ =
1
40 4
10
⋅ =
1
30 3
10
⋅ =
2 2 2
3 4 z+ =
2
9 16 z+ = 2
25 z= 5 z=
Related Rates
4x =
3y =
30
dy
dt
=
40
dx
dt
=
B
A
5z =
Truck Problem:
How fast is the distance between the
trucks changing 6 minutes later?
r t d⋅ =
1
40 4
10
⋅ =
1
30 3
10
⋅ =
2 2 2
3 4 z+ =
2
9 16 z+ =
2 2 2
x y z+ =
2 2 2
dx dy dz
x y z
dt dt dt
+ =
4 40 3 30 5
dz
dt
⋅ + ⋅ =
Truck A travels east at 40 mi/hr.
Truck B travels north at 30 mi/hr.
Related Rates
250 5
dz
dt
= 50
dz
dt
=
miles
50
hour
4Related Rates
Truck Problem:
How fast is the distance between the
trucks changing 6 minutes later?
Truck A travels east at 40 mi/hr.
Truck B travels north at 30 mi/hr.
A stone dropped in a pond sends
out a circular ripple whose radius
increases at a constant rate of 4
ft/sec. After 12 seconds, how
rapidly is the area enclosed by the
ripple increasing?
Library Work # 2
•1. Sketch the graph of f. Find the absolute
and local maximum and minimum values of f.
Use the interval [-1,4]
•2. f(x)= X4
+ 4x3
-2x2
-12x
Maxima Minima Problems
•3. A farmer has 800 m fencing material to enclose a
rectangular pen adjacent to a long existing wall. He
will use the wall for one side of the pen and the
available fencing material for the remaining three
sides. What is the maximum area that can be
enclosed this way?
4. Differentiate each of the following:
 
 .
10x4
 − 18xy2
 + 10y3
 = 48
5. Find the derivative of each function.
5. y = e–3xsin4x
6. Solve the Related Rates problem.
•An airplane is flying west at 500 ft/sec at an altitude
of 4000 ft and a searchlight on the ground lies
directly under the path of the plane. If the light is
kept on the plane , how fast is the searchlight
revolving when the airline distance of the plane
from the searchlight is 2000 feet due east?
End….

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Differential calculus

  • 2.
  • 3.
  • 5.
  • 7. DERIVATIVE • Recall your concept of a slope;
  • 9. What happens to the graph as the change in x approaches 0?
  • 10.
  • 12. Example •Find an equation of the tangent line to the parabola y = x2 -1 at point (2,3). Sketch the parabola and show the segment of the tangent line at (2,3). Find the general formula for the slope of the tangent line of this function. What is the slope when x = 5?
  • 13. 2 3y x= − ( ) ( )2 2 0 3 3 lim h x h x y h→ + − − − ′ = 2y x′ = 0 lim2 h y x h → ′ = + 3.1 Derivative of a Function
  • 14. A function is differentiable if it has a derivative everywhere in its domain. It must be continuous and smooth. Functions on closed intervals must have one-sided derivatives defined at the end points. Derivative of a Function
  • 15. To be differentiable, a function must be continuous and smooth. Derivatives will fail to exist at: corner ( )f x x= cusp ( ) 2 3 f x x= vertical tangent ( ) 3 f x x= discontinuity ( ) 1, 0 1, 0 x f x x − < = ≥ 3.2 Differentiability
  • 16. Most of the functions we study in calculus will be differentiable. Differentiability
  • 17. If f has a derivative at x = a, then f is continuous at x = a. Since a function must be continuous to have a derivative, if it has a derivative then it is continuous. 3.2 Differentiability
  • 18. ( ) 1 2 f a′ = ( ) 3f b′ = Intermediate Value Theorem for Derivatives Between a and b, must take on every value between and . f ′ 1 2 3 If a and b are any two points in an interval on which f is differentiable, then takes on every value between and . f ′ ( )f a′ ( )f b′ Differentiability
  • 19. If the derivative of a function is its slope, then for a constant function, the derivative must be zero. ( ) 0 d c dx = example: 3y = 0y′ = The derivative of a constant is zero. 3.3 Rules for Differentiation
  • 20. We saw that if , . 2 y x= 2y x′ = This is part of a pattern. ( ) 1n nd x nx dx − = examples: ( ) 4 f x x= ( ) 3 4f x x′ = 8 y x= 7 8y x′ = power rule Rules for Differentiation
  • 21. ( ) 1n nd x nx dx − = Rules for Differentiation Proof: h xhx x dx d nn h n −+ = → )( lim 0 h xhhnxx x dx d nnnn h n −+++ = − → ... lim 1 0 h hhnx x dx d nn h n ++ = − → ... lim 1 0 1 0 lim − → = n h n nxx dx d
  • 22. ( ) d du cu c dx dx = examples: 1n nd cx cnx dx − = constant multiple rule: 5 4 4 7 7 5 35 d x x x dx = ⋅ = Rules for Differentiation
  • 23. (Each term is treated separately) ( ) d du cu c dx dx =constant multiple rule: sum and difference rules: ( ) d du dv u v dx dx dx + = + ( ) d du dv u v dx dx dx − = − 4 12y x x= + 3 4 12y x′ = + 4 2 2 2y x x= − + 3 4 4 dy x x dx = − 3.3 Rules for Differentiation
  • 24. Find the horizontal tangents of: 4 2 2 2y x x= − + 3 4 4 dy x x dx = − Horizontal tangents occur when slope = zero. 3 4 4 0x x− = 3 0x x− = ( )2 1 0x x − = ( ) ( )1 1 0x x x+ − = 0, 1, 1x = − Substituting the x values into the original equation, we get: 2, 1, 1y y y= = = (The function is even, so we only get two horizontal tangents.) Rules for Differentiation
  • 25. 4 2 2 2y x x= − + 2y = 1y = Rules for Differentiation
  • 26. 4 2 2 2y x x= − + First derivative (slope) is zero at: 0, 1, 1x = − 3 4 4 dy x x dx = − Rules for Differentiation
  • 27. product rule: ( ) d dv du uv u v dx dx dx = + Notice that this is not just the product of two derivatives. This is sometimes memorized as: ( )d uv u dv v du= + ( )( )2 3 3 2 5 d x x x dx  + +  ( )5 3 3 2 5 6 15 d x x x x dx + + + ( )5 3 2 11 15 d x x x dx + + 4 2 10 33 15x x+ + =( )2 3x + ( )2 6 5x + ( )3 2 5x x+ + ( )2x 4 2 2 4 2 6 5 18 15 4 10x x x x x+ + + + + 4 2 10 33 15x x+ + Rules for Differentiation
  • 28. product rule: ( ) d dv du uv u v dx dx dx = + Rules for Differentiation Proof h xvxuhxvhxu uv dx d h )()()()( lim)( 0 −++ = → add and subtract u(x+h)v(x) in the denominator h xvhxuxvhxuxvxuhxvhxu uv dx d h )()()()()()()()( lim)( 0 +−++−++ = → ( ) ( )       −++−++ = → h xuhxuxvxvhxvhxu uv dx d h )()()()()()( lim)( 0 dx du v dx dv uuv dx d +=)(
  • 29. quotient rule: 2 du dv v u d u dx dx dx v v −   =    or 2 u v du u dv d v v −  =    3 2 2 5 3 d x x dx x + + ( )( ) ( )( ) ( ) 2 2 3 2 2 3 6 5 2 5 2 3 x x x x x x + + − + = + Rules for Differentiation
  • 30. Higher Order Derivatives: dy y dx ′ = is the first derivative of y with respect to x. 2 2 dy d dy d y y dx dx dx dx ′ ′′ = = = is the second derivative. (y double prime) dy y dx ′′ ′′′ = is the third derivative. ( )4 d y y dx ′′′= is the fourth derivative. We will learn later what these higher order derivatives are used for. Rules for Differentiation
  • 31. Rules for Differentiation Suppose u and v are functions that are differentiable at x = 3, and that u(3) = 5, u’(3) = -7, v(3) = 1, and v’(3)= 4. Find the following at x = 3 : )(.1 uv dx d '')( vuuvuv dx d += 8)7)(1()3(5 =−+       v u dx d .2 2 '' v uvvu v u dx d − =      2 1 )4)(5()7)(1( −− 27−=       u v dx d .3 2 '' u vuuv u v dx d − =      2 5 )7)(1()4)(5( −− 25 27 =
  • 33. Consider a graph of displacement (distance traveled) vs. time. time (hours) distance (miles) Average velocity can be found by taking: change in position change in time s t ∆ = ∆ t∆ s∆ A B ( ) ( ) ave f t t f ts V t t +∆ −∆ = = ∆ ∆ The speedometer in your car does not measure average velocity, but instantaneous velocity. ( ) ( ) ( ) 0 lim t f t t f tds V t dt t∆ → +∆ − = = ∆ (The velocity at one moment in time.) Velocity and other Rates of Change
  • 34. Velocity and other Rates of Change Velocity is the first derivative of position. Acceleration is the second derivative of position.
  • 35. Example: Free Fall Equation 21 2 s g t= Gravitational Constants: 2 ft 32 sec g = 2 m 9.8 sec g = 2 cm 980 sec g = 21 32 2 s t= ⋅ 2 16s t= 32 ds V t dt = = Speed is the absolute value of velocity. Velocity and other Rates of Change
  • 36. Acceleration is the derivative of velocity. dv a dt = 2 2 d s dt = example: 32v t= 32a = If distance is in: feet Velocity would be in: feet sec Acceleration would be in: ft sec sec 2 ft sec = Velocity and other Rates of Change
  • 37. Rates of Change: Average rate of change = ( ) ( )f x h f x h + − Instantaneous rate of change = ( ) ( ) ( ) 0 lim h f x h f x f x h→ + − ′ = These definitions are true for any function. ( x does not have to represent time. ) Velocity and other Rates of Change
  • 38. For a circle: 2 A rπ= 2dA d r dr dr π= 2 dA r dr π= Instantaneous rate of change of the area with respect to the radius. For tree ring growth, if the change in area is constant then dr must get smaller as r gets larger. 2dA r drπ= Velocity and other Rates of Change
  • 39. from Economics: Marginal cost is the first derivative of the cost function, and represents an approximation of the cost of producing one more unit. Velocity and other Rates of Change
  • 40. Example 13: Suppose it costs: ( ) 3 2 6 15c x x x x= − + to produce x stoves. ( ) 2 3 12 15c x x x′ = − + If you are currently producing 10 stoves, the 11th stove will cost approximately: ( ) 2 10 3 10 12 10 15c′ = × − × + 300 120 15= − + $195= marginal cost The actual cost is: ( ) ( )11 10C C− ( ) ( )3 2 3 2 11 6 11 15 11 10 6 10 15 10= − × + × − − × + × 770 550= − $220= actual cost Velocity and other Rates of Change
  • 42.
  • 43.
  • 44. π 2 π 0 2 π − π− Consider the function ( )siny θ= We could make a graph of the slope: θ slope 1− 0 1 0 1− Now we connect the dots! The resulting curve is a cosine curve. ( )sin cos d x x dx = Derivatives of Trigonometric Functions
  • 45. Derivatives of Trigonometric Functions h xhx x dx d h sin)sin( limsin 0 −+ = → h xxhhx x dx d h sincossincossin limsin 0 −+ = → h xh h hx x dx d hh cossin lim )1(cossin limsin 00 →→ + − = h xhhx x dx d h cossin)1(cossin limsin 0 +− = → Proof
  • 46. Derivatives of Trigonometric Functions h xh h hx x dx d hh cossin lim )1(cossin limsin 00 →→ + − = = 0 = 1 ( )sin cos d x x dx =
  • 47. Derivatives of Trigonometric Functions h xhx x dx d h cos)cos( limcos 0 −+ = → h xxhhx x dx d h cossinsincoscos limcos 0 −− = → h xh h hx x dx d hh sinsin lim )1(coscos limcos 00 →→ − − = h xhhx x dx d h sinsin)1(coscos limcos 0 −− = → Find the derivative of cos x
  • 48. Derivatives of Trigonometric Functions = 0 = 1 h xh h hx x dx d hh sinsin lim )1(coscos limcos 00 →→ − − = ( )cos sin d x x dx = −
  • 49. We can find the derivative of tangent x by using the quotient rule. tan d x dx sin cos d x dx x ( ) 2 cos cos sin sin cos x x x x x × − ×− 2 2 2 cos sin cos x x x + 2 1 cos x 2 sec x ( ) 2 tan sec d x x dx = Derivatives of Trigonometric Functions
  • 50. Derivatives of the remaining trig functions can be determined the same way. sin cos d x x dx = cos sin d x x dx = − 2 tan sec d x x dx = 2 cot csc d x x dx = − sec sec tan d x x x dx = × csc csc cot d x x x dx = − × Derivatives of Trigonometric Functions
  • 51. Derivatives of Trigonometric Functions Jerk A sudden change in acceleration Definition Jerk Jerk is the derivative of acceleration. If a body’s position at time t is s(t), the body’s jerk at time t is 3 3 2 2 )( dt sd dt vd dt da tj ===
  • 52. Consider a simple composite function: 6 10y x= − ( )2 3 5y x= − If 3 5u x= − then 2y u= 6 10y x= − 2y u= 3 5u x= − 6 dy dx = 2 dy du = 3 du dx = dy dy du dx du dx = ⋅ 6 2 3= ⋅ Chain Rule
  • 53. dy dy du dx du dx = ⋅Chain Rule: example: ( ) sinf x x= ( ) 2 4g x x= − Find: ( ) at 2f g x′ =o ( ) cosf x x′ = ( ) 2g x x′ = ( )2 4 4 0g = − = ( ) ( )0 2f g′ ′⋅ ( ) ( )cos 0 2 2⋅ ⋅ 1 4⋅ 4= Chain Rule If is the composite of and , then: f go ( )y f u= ( )u g x= ( ) ( ) atat xu g x f g f g= ′ ′ ′= ⋅o )('))((' xgxgf •=
  • 54. ( )( ) ( )2 sin 4f g x x= − ( )2 sin 4y x= − siny u= 2 4u x= − cos dy u du = 2 du x dx = dy dy du dx du dx = ⋅ cos 2 dy u x dx = ⋅ ( )2 cos 4 2 dy x x dx = − ⋅ ( )2 cos 2 4 2 2 dy dx = − ⋅ ⋅ ( )cos 0 4 dy dx = ⋅ 4 dy dx = Chain Rule
  • 55. Here is a faster way to find the derivative: ( )2 sin 4y x= − ( ) ( )2 2 cos 4 4 d y x x dx = − ⋅ − ( )2 cos 4 2y x x= − ⋅ Differentiate the outside function... …then the inside function At 2, 4x y= = Chain Rule
  • 56. ( )2 cos 3 d x dx ( ) 2 cos 3 d x dx    ( ) ( )2 cos 3 cos 3 d x x dx ⋅   ( ) ( ) ( )2cos 3 sin 3 3 d x x x dx ⋅− ⋅ ( ) ( )2cos 3 sin 3 3x x− ⋅ ⋅ ( ) ( )6cos 3 sin 3x x− The chain rule can be used more than once. (That’s what makes the “chain” in the “chain rule”!) Chain Rule
  • 57. Derivative formulas include the chain rule! 1n nd du u nu dx dx − = sin cos d du u u dx dx = cos sin d du u u dx dx = − 2 tan sec d du u u dx dx = etcetera… Chain Rule
  • 58. Chain Rule Find )3cos( 2 xxy += )16)(3sin( 2 ++−= xxx dx dy ))sin(cos(xy = )24(cos 33 xxy += )sin)(cos(cos xx dx dy −= )212))(24sin()(24(cos3 2332 ++−+= xxxxx dx dy ))24sin()(24(cos)636( 3322 xxxxx dx dy +−++= dx dy
  • 59. The chain rule enables us to find the slope of parametrically defined curves: dy dy dx dt dx dt = ⋅ dy dydt dx dx dt = The slope of a parametrized curve is given by: dy dy dt dxdx dt = Chain Rule
  • 60. 2 2 1x y+ = This is not a function, but it would still be nice to be able to find the slope. 2 2 1 d d d x y dx dx dx + = Do the same thing to both sides. 2 2 0 dy x y dx + = Note use of chain rule. 2 2 dy y x dx = − 2 2 dy x dx y − = dy x dx y = − Implicit Differentiation
  • 61. 2 2 siny x y= + 2 2 sin d d d y x y dx dx dx = + This can’t be solved for y. 2 2 cos dy dy x y dx dx = + 2 cos 2 dy dy y x dx dx − = ( ) 22 cos dy xy dx =− 2 2 cos dy x dx y = − This technique is called implicit differentiation. 1 Differentiate both sides w.r.t. x. 2 Solve for . dy dx Implicit Differentiation
  • 62. Implicit Differentiation Implicit Differentiation Process 1. Differentiate both sides of the equation with respect to x. 2. Collect the terms with dy/dx on one side of the equation. 3. Factor out dy/dx . 4. Solve for dy/dx .
  • 63. Find the equations of the lines tangent and normal to the curve at . 2 2 7x xy y− + = ( 1,2)− 2 2 7x xy y− + = 2 2 0 dydy x yx y dxdx  − + =+   Note product rule. 2 2 0 dy dy x x y y dx dx − − + = ( ) 22 dy y xy x dx = −− 2 2 dy y x dx y x − = − ( ) ( ) 2 2 1 2 2 1 m − − = ⋅ − − 2 2 4 1 + = + 4 5 = Implicit Differentiation
  • 64. Find the equations of the lines tangent and normal to the curve at . 2 2 7x xy y− + = ( 1,2)− 4 5 m = tangent: ( ) 4 2 1 5 y x− = + 4 4 2 5 5 y x− = + 4 14 5 5 y x= + normal: ( ) 5 2 1 4 y x− = − + 5 5 2 4 4 y x− = − − 5 3 4 4 y x= − + Implicit Differentiation
  • 65. Find if . 2 2 d y dx 3 2 2 3 7x y− = 3 2 2 3 7x y− = 2 6 6 0x y y′− = 2 6 6y y x′− = − 2 6 6 x y y − ′ = − 2 x y y ′ = 2 2 2y x x y y y ′⋅ − ′′ = 2 2 2x x y y y y ′′ ′= − 2 2 2 2x x y y x yy ′′ = − ⋅ 4 3 2x x y y y ′′ = − Substitute back into the equation. y′ Implicit Differentiation
  • 66. Implicit Differentiation Rational Powers of Differentiable Functions Power Rule for Rational Powers of x If n is any rational number, then 1− = nn nxx dx d
  • 67. Implicit Differentiation Proof: Let p and q be integers with q > 0. q p xy = pq xy = Raise both sides to the q power Differentiate with respect to x 11 −− = pq px dx dy qy Solve for dy/dx
  • 68. Implicit Differentiation 1 1 − − = q p qy px dx dy Substitute for y 1/ 1 )( − − = qqp p xq px dx dy Remove parenthesis qpp p qx px dx dy / 1 − − = Subtract exponents q px dx dy qppp )/(1 −−− = 1)/( − = qp x q p dx dy
  • 73. Look at the graph of x y e= The slope at x = 0 appears to be 1. If we assume this to be true, then: 0 0 0 lim 1 h h e e h + → − = definition of derivative Derivatives of Exponential and Logarithmic Functions
  • 74. Now we attempt to find a general formula for the derivative of using the definition. x y e= ( ) 0 lim x h x x h d e e e dx h + → − = 0 lim x h x h e e e h→ ⋅ − = 0 1 lim h x h e e h→  − = ⋅    0 1 lim h x h e e h→  − = ⋅     1x e= ⋅ x e= This is the slope at x = 0, which we have assumed to be 1. Derivatives of Exponential and Logarithmic Functions
  • 75. 75 – More Derivatives 4) Exponents If y = bx y’ = bx ln(b) Therefore If y = ex y’ = ex
  • 76. ( )x xd e e dx = →
  • 77. 77 – More Exciting Derivatives 2) Natural Logs If y=ln(x), y’ = 1/x -chain rule may apply If y=ln(x2 ) y’ = (1/x2 )2x = 2/x
  • 78. x e is its own derivative! If we incorporate the chain rule: u ud du e e dx dx = We can now use this formula to find the derivative of x a Derivatives of Exponential and Logarithmic Functions
  • 79. ( )xd a dx ( )ln x ad e dx ( )lnx ad e dx ( )ln lnx a d e x a dx ⋅ Incorporating the chain rule: ( ) lnu ud du a a a dx dx = Derivatives of Exponential and Logarithmic Functions aaa dx d xx ln=
  • 80. So far today we have: u ud du e e dx dx = ( ) lnu ud du a a a dx dx = Now it is relatively easy to find the derivative of .ln x 3.9 Derivatives of Exponential and Logarithmic Functions
  • 81. lny x= y e x= ( ) ( )yd d e x dx dx = 1y dy e dx = 1 y dy dx e = 1 ln d x dx x = 1 ln d du u dx u dx = Derivatives of Exponential and Logarithmic Functions
  • 82. To find the derivative of a common log function, you could just use the change of base rule for logs: log d x dx ln ln10 d x dx = 1 ln ln10 d x dx = 1 1 ln10 x = ⋅ The formula for the derivative of a log of any base other than e is: 1 log ln a d du u dx u a dx = Derivatives of Exponential and Logarithmic Functions
  • 83. u ud du e e dx dx = ( ) lnu ud du a a a dx dx = 1 log ln a d du u dx u a dx = 1 ln d du u dx u dx = Derivatives of Exponential and Logarithmic Functions
  • 84. 84 – More Derivatives 4b) Exponents and chain rule If y = bkx y’ = bkx ln(b)k Or more generally: If y = bg(x) y’ = bg(x) ln(b) X dg(x)/dx
  • 85. 85 2.1.2 – More Derivatives 4b) Exponents and chain rule If y = 52x y’ = 52x ln(5)2 Or more complicated: If y = 5sin(x) y’ = 5sin(x) ln(5) * cos(x)
  • 86. Derivatives of Exponential and Logarithmic Functions x ey 2 = 2 3x y = 3 ln xy = Find y’ x ey 2 2'= )2)(3ln(3' 2 xy x = x x x y 3 )3( 1 ' 2 3 ==
  • 87. Derivatives of Exponential and Logarithmic Functions Logarithmic differentiation Used when the variable is in the base and the exponent y = xx ln y = ln xx ln y = x ln x x x x dx dy y ln 11 +      = ( )xy dx dy ln1+= ( )xx dx dy x ln1+=
  • 88.
  • 89.
  • 90.
  • 92. Extrema on an Interval
  • 93. Extrema of a Function In calculus, much effort is devoted to determining the behavior of a function f on an interval I. Does f have a maximum value on I? Does it have a minimum value? Where is the function increasing? Where is it decreasing? In this chapter, you will learn how derivatives can be used to answer these questions. You will also see why these questions are important in real-life applications.
  • 94. Extrema of a Function
  • 95. A function need not have a minimum or a maximum on an interval. For instance, in Figure 3.1(a) and (b), you can see that the function f(x) = x2 + 1 has both a minimum and a maximum on the closed interval [–1, 2], but does not have a maximum on the open interval (–1, 2). Figure 3.1(a) Figure 3.1(b) Extrema of a Function
  • 96. Moreover, in Figure 3.1(c), you can see that continuity (or the lack of it) can affect the existence of an extremum on the interval. This suggests the theorem below. Figure 3.1(c) Extrema of a Function
  • 97. Relative Extrema and Critical Numbers
  • 98. Relative Extrema and Critical Numbers In Figure 3.2, the graph of f(x) = x3 – 3x2 has a relative maximum at the point (0, 0) and a relative minimum at the point (2, –4). Informally, for a continuous function, you can think of a relative maximum as occurring on a “hill” on the graph, and a relative minimum as occurring in a “valley” on the graph. Figure 3.2
  • 99. Such a hill and valley can occur in two ways. When the hill (or valley) is smooth and rounded, the graph has a horizontal tangent line at the high point (or low point). When the hill (or valley) is sharp and peaked, the graph represents a function that is not differentiable at the high point (or low point). Relative Extrema and Critical Numbers
  • 100. Relative Extrema and Critical Numbers
  • 101. Example 1 – The Value of the Derivative at Relative Extrema Find the value of the derivative at each relative extremum shown in Figure 3.3. Figure 3.3
  • 102. Example 1(a) – Solution At the point (3, 2), the value of the derivative is f'(3) = 0 [see Figure 3.3(a)]. The derivative of is Figure 3.3(a)
  • 103. Example 1(b) – Solution At x = 0, the derivative of f(x) = |x| does not exist because the following one-sided limits differ [see Figure 3.3(b)]. cont’d Figure 3.3(b)
  • 104. Example 1(c) – Solution The derivative of f(x) = sin x is f'(x) = cos x. At the point (π/2, 1), the value of the derivative is f'(π/2) = cos(π/2) = 0. At the point (3π/2, –1), the value of the derivative is f'(3π/2) = cos(3π/2) = 0 [see Figure 3.3(c)]. cont’d Figure 3.3(c)
  • 105. Note in Example 1 that at each relative extremum, the derivative either is zero or does not exist. The x-values at these special points are called critical numbers. Figure 3.4 illustrates the two types of critical numbers. Figure 3.4 Relative Extrema and Critical Numbers
  • 106. Relative Extrema and Critical Numbers Notice in the definition above that the critical number c has to be in the domain of f, but c does not have to been in the domain of f'.
  • 107. Finding Extrema on a Closed Interval Theorem 3.2 states that the relative extrema of a function can occur only at the critical number of the function. Knowing this, you can use the following guidelines to find extrema on a closed interval.
  • 108. Example 2 – Finding Extrema on a Closed Interval Find the extrema of f(x) = 3x4 – 4x3 on the interval [–1, 2]. Solution: Begin by differentiating the function. f(x) = 3x4 – 4x3 Write original function. f'(x) = 12x3 – 12x2 Differentiate.
  • 109. Example 2 – Solution To find the critical numbers on the interval (– 1,2), you must find all x-values for which f'(x) = 0 and all x-values for which f'(x) does not exist. f'(x) = 12x3 – 12x2 = 0 Set f'(x) equal to 0. 12x2 (x– 1) = 0 Factor. x = 0, 1 Critical numbers Because f' is defined for all x, you can conclude that these are the only critical numbers of f. cont’d
  • 110. By evaluating f at these two critical numbers and at the endpoints of [–1, 2], you can determine that the maximum is f(2) = 16 and the minimum is f(1) = –1, as shown in the table. Example 2 – Solution cont’d
  • 111. The graph of f is shown in Figure 3.5. Figure 3.5 Example 2 – Solution cont’d
  • 112. cont’d In Figure 3.5, note that the critical number x = 0 does not yield a relative minimum or a relative maximum. This tells you that the converse of Theorem 3.2 is not true. In other words, the critical numbers of a function need not produce relative extrema. Example 2 – Solution
  • 113. • Determine the absolute extrema for the following function and interval[-4,2]. •
  • 114. First, a review problem: Consider a sphere of radius 10 cm. If the radius changes 0.1 cm (a very small amount) how much does the volume change? 34 3 V rπ= 2 4dV r drπ= ( ) 2 4 10cm 0.1cmdV π= ⋅ 3 40 cmdV π= The volume would change by approximately 40π cm3 Related Rates
  • 115. Now, suppose that the radius is changing at an instantaneous rate of 0.1 cm/sec. 34 3 V rπ= 2 4 dV dr r dt dt π= ( ) 2 cm 4 10cm 0.1 sec dV dt π   = ⋅    3 cm 40 sec dV dt π= The sphere is growing at a rate of 40π cm3 /sec . Note: This is an exact answer, not an approximation like we got with the differential problems. Related Rates
  • 116. Water is draining from a cylindrical tank at 3 liters/second. How fast is the surface dropping? L 3 sec dV dt = − 3 cm 3000 sec = − Find dh dt 2 V r hπ= 2dV dh r dt dt π= (r is a constant.) 3 2cm 3000 sec dh r dt π− = 3 2 cm 3000 secdh dt rπ = − (We need a formula to relate V and h. ) Related Rates
  • 117. Steps for Related Rates Problems: 1. Draw a picture (sketch). 2. Write down known information. 3. Write down what you are looking for. 4. Write an equation to relate the variables. 5. Differentiate both sides with respect to t. 6. Evaluate. Related Rates
  • 118. Hot Air Balloon Problem: Given: 4 π θ = rad 0.14 min d dt θ = How fast is the balloon rising? Find dh dt tan 500 h θ = 2 1 sec 500 d dh dt dt θ θ = ( ) 2 1 sec 0.14 4 500 dh dt π  =    h θ 500ft Related Rates
  • 119. Hot Air Balloon Problem: Given: 4 π θ = rad 0.14 min d dt θ = How fast is the balloon rising? Find dh dt tan 500 h θ = 2 1 sec 500 d dh dt dt θ θ = ( ) 2 1 sec 0.14 4 500 dh dt π  =    h θ 500ft ( ) ( ) 2 2 0.14 500 dh dt ⋅ = 1 1 2 4 π sec 2 4 π = ft 140 min dh dt = Related Rates
  • 120. 4x = 3y = B A 5z = Truck Problem: Truck A travels east at 40 mi/hr. Truck B travels north at 30 mi/hr. How fast is the distance between the trucks changing 6 minutes later? r t d⋅ = 1 40 4 10 ⋅ = 1 30 3 10 ⋅ = 2 2 2 3 4 z+ = 2 9 16 z+ = 2 25 z= 5 z= Related Rates
  • 121. 4x = 3y = 30 dy dt = 40 dx dt = B A 5z = Truck Problem: How fast is the distance between the trucks changing 6 minutes later? r t d⋅ = 1 40 4 10 ⋅ = 1 30 3 10 ⋅ = 2 2 2 3 4 z+ = 2 9 16 z+ = 2 2 2 x y z+ = 2 2 2 dx dy dz x y z dt dt dt + = 4 40 3 30 5 dz dt ⋅ + ⋅ = Truck A travels east at 40 mi/hr. Truck B travels north at 30 mi/hr. Related Rates
  • 122. 250 5 dz dt = 50 dz dt = miles 50 hour 4Related Rates Truck Problem: How fast is the distance between the trucks changing 6 minutes later? Truck A travels east at 40 mi/hr. Truck B travels north at 30 mi/hr.
  • 123. A stone dropped in a pond sends out a circular ripple whose radius increases at a constant rate of 4 ft/sec. After 12 seconds, how rapidly is the area enclosed by the ripple increasing?
  • 124.
  • 125. Library Work # 2 •1. Sketch the graph of f. Find the absolute and local maximum and minimum values of f. Use the interval [-1,4] •2. f(x)= X4 + 4x3 -2x2 -12x
  • 126. Maxima Minima Problems •3. A farmer has 800 m fencing material to enclose a rectangular pen adjacent to a long existing wall. He will use the wall for one side of the pen and the available fencing material for the remaining three sides. What is the maximum area that can be enclosed this way?
  • 127. 4. Differentiate each of the following:    . 10x4  − 18xy2  + 10y3  = 48
  • 128. 5. Find the derivative of each function. 5. y = e–3xsin4x
  • 129. 6. Solve the Related Rates problem. •An airplane is flying west at 500 ft/sec at an altitude of 4000 ft and a searchlight on the ground lies directly under the path of the plane. If the light is kept on the plane , how fast is the searchlight revolving when the airline distance of the plane from the searchlight is 2000 feet due east?