The document is a lesson on implicit differentiation and related concepts:
1) Implicit differentiation allows one to take the derivative of an implicitly defined relation between x and y, even if y is not explicitly defined as a function of x.
2) Examples are provided to demonstrate implicit differentiation, such as finding the slope of a tangent line to a curve.
3) The van der Waals equation is introduced to describe non-ideal gas properties, and implicit differentiation is used to find the isothermal compressibility of a van der Waals gas.
This is your introduction to domain, range, and functions. You will learn more about domain, range, functions, relations, x-values, and y-values. There are definitions and explanations of each concepts. There are questions to help quiz yourself. Test your abilities. Enjoy.
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Lesson 14: Derivatives of Logarithmic and Exponential Functions (slides)Matthew Leingang
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A functional relationship between y and x can be made explicit. Even if the relation is not functional, however, we can assume the relation usually defines y as a function.
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 041 ...Matthew Leingang
The exponential function is pretty much the only function whose derivative is itself. The derivative of the natural logarithm function is also beautiful as it fills in an important gap. Finally, the technique of logarithmic differentiation allows us to find derivatives without the product rule.
Using implicit differentiation we can treat relations which are not quite functions like they were functions. In particular, we can find the slopes of lines tangent to curves which are not graphs of functions.
Using implicit differentiation we can treat relations which are not quite functions like they were functions. In particular, we can find the slopes of lines tangent to curves which are not graphs of functions.
Using implicit differentiation we can treat relations which are not quite functions like they were functions. In particular, we can find the slopes of lines tangent to curves which are not graphs of functions.
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The derivative of a composition of functions is the product of the derivatives of those functions. This rule is important because compositions are so powerful.
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Lesson 16: Implicit Differentiation
1. Lesson 16 (Section 3.6)
Implicit Differentiation
Derivatives of Inverse Functions
Math 1a
October 31, 2007
Announcements
OH: Mondays 1–2, Tuesdays 3–4, Wednesdays 1–3 (SC 323)
2. Problem
Find the slope of the line which is tangent to the curve
x2 + y2 = 1
at the point (3/5, −4/5).
3. Problem
Find the slope of the line which is tangent to the curve
x2 + y2 = 1
at the point (3/5, −4/5).
Solution (Old Way)
y2 = 1 − x2
=⇒ y = − 1 − x 2
−2x
dy x
=− √ =√
dx 2 1 − x2
2 1−x
dy 3/5 3/5 3
= = =.
dx x=3/5 4/5 4
1 − (3/5)2
4. Solution (New Way)
Differentiating this, but pretend that y is a function of x. We have:
dy
2x + 2y = 0,
dx
or
dy x
=− .
dx y
3 4
So if x = , y = − , and r = 1, then the slope of the line tangent
5 5
to the circle is
dy 3/5 3
= =.
dx ( 3 ,− 4 ) 4/5 4
5 5
5. Summary
any time a relation is given between x and y , we may differentiate
y as a function of x even though it is not explicitly defined
This is called implicit differentiation.
6. Example
Find the equation of the line tangent to the curve
y 2 = x 2 (x + 1) = x 3 + x 2
at the point (3, −6).
7. Example
Find the equation of the line tangent to the curve
y 2 = x 2 (x + 1) = x 3 + x 2
at the point (3, −6).
Solution
Differentiating the expression
implicitly with respect to x
dy
= 3x 2 + 2x, so
gives 2y
dx
3x 2 + 2x
dy
= , and
dx 2y
3 · 32 + 2 · 3
dy 11
=− .
=
dx 2(−6) 4
(3,−6)
8. Example
Find the equation of the line tangent to the curve
y 2 = x 2 (x + 1) = x 3 + x 2
at the point (3, −6).
Solution
Differentiating the expression
implicitly with respect to x
dy
= 3x 2 + 2x, so
gives 2y
dx
3x 2 + 2x
dy
= , and
dx 2y
3 · 32 + 2 · 3
dy 11
=− .
=
Thus the equation of the
dx 2(−6) 4
(3,−6)
tangent line is
11
y +6=− (x − 3).
4
10. Example
Find the horizontal tangent lines to the same curve: y 2 = x 3 + x 2
Solution
1
We need 3x 2 + 1 = 0, or x = √ . Then
3
1 1
y2 = √ + ,
33 3
Thus
1 1
+√
y =±
3 33
11. An example from chemistry
Example
The van der Waals equation
describes nonideal properties
of a gas:
n2
(V −nb) = nRT ,
P +a
V2
where P is the pressure, V
the volume, T the
temperature, n the number of
moles of the gas, R a
constant, a is a measure of
attraction between particles
of the gas, and b a measure
of particle size.
12. An example from chemistry
Example
The van der Waals equation
describes nonideal properties
of a gas:
n2
(V −nb) = nRT ,
P +a
V2
where P is the pressure, V
the volume, T the
temperature, n the number of
moles of the gas, R a
constant, a is a measure of
attraction between particles
of the gas, and b a measure
of particle size.
16. Let’s find the compressibility of a van der Waals gas.
Differentiating the van der Waals equation by treating V as a
function of P gives
an2 2an2 dV
dV
+ (V − bn) 1 −
P+ = 0,
V2 V 3 dP
dP
17. Let’s find the compressibility of a van der Waals gas.
Differentiating the van der Waals equation by treating V as a
function of P gives
an2 2an2 dV
dV
+ (V − bn) 1 −
P+ = 0,
V2 V 3 dP
dP
so
V 2 (V − nb)
1 dV
β=− =
2abn3 − an2 V + PV 3
V dP
18. Let’s find the compressibility of a van der Waals gas.
Differentiating the van der Waals equation by treating V as a
function of P gives
an2 2an2 dV
dV
+ (V − bn) 1 −
P+ = 0,
V2 V 3 dP
dP
so
V 2 (V − nb)
1 dV
β=− =
2abn3 − an2 V + PV 3
V dP
What if a = b = 0?
19. Let’s find the compressibility of a van der Waals gas.
Differentiating the van der Waals equation by treating V as a
function of P gives
an2 2an2 dV
dV
+ (V − bn) 1 −
P+ = 0,
V2 V 3 dP
dP
so
V 2 (V − nb)
1 dV
β=− =
2abn3 − an2 V + PV 3
V dP
What if a = b = 0?
dβ
What is the sign of ?
db
20. Let’s find the compressibility of a van der Waals gas.
Differentiating the van der Waals equation by treating V as a
function of P gives
an2 2an2 dV
dV
+ (V − bn) 1 −
P+ = 0,
V2 V 3 dP
dP
so
V 2 (V − nb)
1 dV
β=− =
2abn3 − an2 V + PV 3
V dP
What if a = b = 0?
dβ
What is the sign of ?
db
dβ
What is the sign of ?
da
21.
22. Theorem (The Inverse Function Theorem)
Let f be differentiable at a, and f (a) = 0. Then f −1 is defined in
a neighborhood of b = f (a), and
1
(f −1 ) (b) =
(f −1 (b))
f
23. Theorem (The Inverse Function Theorem)
Let f be differentiable at a, and f (a) = 0. Then f −1 is defined in
a neighborhood of b = f (a), and
1
(f −1 ) (b) =
(f −1 (b))
f
“Proof”.
If y = f (x), take f −1 of both sides to get
x = f −1 (f (x)),
so
1 = (f −1 ) (f (x))f (x).
25. Using implicit differentiation to find derivatives
Example
√
dy
Find if y = x.
dx
Solution
√
If y = x, then
y 2 = x,
so
dy dy 1 1
= √.
2y = 1 =⇒ =
dx dx 2y 2x
26. The power rule for rational numbers
Example
dy
if y = x p/q , where p and q are integers.
Find
dx
27. The power rule for rational numbers
Example
dy
if y = x p/q , where p and q are integers.
Find
dx
Solution
We have
yq = xp
dy
qy q−1 = px p−1
dx
p x p−1
dy
= · q−1
dx qy
28. The power rule for rational numbers
Example
dy
if y = x p/q , where p and q are integers.
Find
dx
Solution
We have
yq = xp
dy
qy q−1 = px p−1
dx
p x p−1
dy
= · q−1
dx qy
Now y q−1 = x p(q−1)/q = x p−p/q so
x p−1
= x p−1−(p−p/q) = x p/q−1
y q−1
29. Arcsin
Remember that
1
arcsin x = sin−1 x =
sin x
30. Arcsin
Remember that
1
arcsin x = sin−1 x =
sin x
Example
Find the derivative of arcsin.
31.
32. Arcsin
Remember that
1
arcsin x = sin−1 x =
sin x
Example
Find the derivative of arcsin.
Solution
We have y = arcsin x =⇒ x = sin y , so
dy dy 1
1 = cos y =⇒ = .
dx dx cos y
We would like to express this in terms of x. Since x = sin y , we
have
d 1
cos y = 1 − x 2 =⇒ arcsin x = √ .
dx 1 − x2
37. Arctan
Example
Find the derivative of arctan.
Solution
From y = arctan x we have
dy
x = tan y =⇒ 1 = sec2 y ,
dx
so
dy 1
= .
sec2 y
dx
38. Arctan
Example
Find the derivative of arctan.
Solution
From y = arctan x we have
dy
x = tan y =⇒ 1 = sec2 y ,
dx
so
dy 1
= .
sec2 y
dx
But for all y
dy 1
1 + tan2 y = sec2 y , =⇒ = .
1 + x2
dx
40. Arcsec
Example
Find the derivative of arcsec.
Solution
If y = arcsec x then x = sec y , so
dy
1 = sec y tan y .
dx
Thus
dy 1 1
=√
= .
dx x tan y x x2 − 1