mat01a1: implicit differentiation · implicit di erentiation: up until now we have only studied...
TRANSCRIPT
MAT01A1: Implicit Differentiation
Dr Craig
Week: 4 May 2020
We emphasized when we covered Ch 3.4 that
the Chain Rule was a very important topic.
Let us re-cap that with two examples before
we start with the new differentiation
techniques.
Reminder: the Chain Rule
If f and g are both differentiable and
F = f ◦ g is the composite function
defined by
F (x) = f (g(x)),
then F is differentiable and F ′ is given by
F ′(x) = f ′(g(x)).g′(x)
Chain rule examples
Find y′ for each of the following functions
I y = e2x cot( 3√x)
I y = 2etan(x2)
Try these on your own first. Solutions are on
the slides that follow.
Chain rule examples: solutions
d
dx
(e2x cot( 3
√x))
=(cot( 3√x)) ddx
(e2x)+(e2x) ddx
(cot( 3√x))
=(cot( 3√x))e2x
d
dx(2x) +
(e2x) (− csc2( 3
√x)) ddx
( 3√x)
=(cot( 3√x))e2x(2) +
(e2x) (− csc2( 3
√x)) 1
33√x2
= e2x(2 cot( 3
√x)− csc2( 3
√x)
33√x2
)
Chain rule examples: solutions
d
dx
(2e
tan(x2))
=(2e
tan(x2))(ln 2)
d
dx
(etan(x
2))
=(2e
tan(x2))(ln 2)
(etan(x
2)) d
dx
(tan(x2)
)=(2e
tan(x2))(ln 2)
(etan(x
2)) (
sec2(x2)) ddx
(x2)
=(2e
tan(x2))(ln 2)
(etan(x
2)) (
sec2(x2))2x
Implicit differentiation:
Up until now we have only studied functions
where one variable (usually y) is defined in
terms of another variable (usually x).
Now we will consider relations between x
and y values where the two variables are
defined in terms of one another. For
example:
x2 + y2 = 25
Note: this curve is not a function as it does
not pass the vertical line test.
Implicit differentiation:
Up until now we have only studied functions
where one variable (usually y) is defined in
terms of another variable (usually x).
Now we will consider relations between x
and y values where the two variables are
defined in terms of one another.
For
example:
x2 + y2 = 25
Note: this curve is not a function as it does
not pass the vertical line test.
Implicit differentiation:
Up until now we have only studied functions
where one variable (usually y) is defined in
terms of another variable (usually x).
Now we will consider relations between x
and y values where the two variables are
defined in terms of one another. For
example:
x2 + y2 = 25
Note: this curve is not a function as it does
not pass the vertical line test.
Clearly this curve is not a function
x2 + y2 = 25
We want a method of calculating the slope
of the tangent to the curve x2 + y2 = 25.
We could try to solve for y, but then we get
y = ±√
25− x2
Thus the implicit relation x2 + y2 = 25 can
only be fully described by the twofunctions below:
f (x) =√
25− x2 & g(x) = −√
25− x2
We see this in the sketches on the next slide.
We want a method of calculating the slope
of the tangent to the curve x2 + y2 = 25.
We could try to solve for y, but then we get
y = ±√
25− x2
Thus the implicit relation x2 + y2 = 25 can
only be fully described by the twofunctions below:
f (x) =√
25− x2 & g(x) = −√
25− x2
We see this in the sketches on the next slide.
We want a method of calculating the slope
of the tangent to the curve x2 + y2 = 25.
We could try to solve for y, but then we get
y = ±√
25− x2
Thus the implicit relation x2 + y2 = 25 can
only be fully described by the twofunctions below:
f (x) =√
25− x2 & g(x) = −√
25− x2
We see this in the sketches on the next slide.
In pictures...
f (x) =√25− x2 and g(x) = −
√25− x2
We could use existing techniques and these
curves to find the slope of a tangent.
Fortunately there is a much better method.
In pictures...
f (x) =√25− x2 and g(x) = −
√25− x2
We could use existing techniques and these
curves to find the slope of a tangent.
Fortunately there is a much better method.
Implicit differentiation:
We are interested in differentiating relations
which are implicitly defined.
To do this
we treat y as a function of x
and then apply our existing rules of
differentiation.
A crucial rule will be the
chain rule. For example:
d
dx(y2) = 2y.
d
dx(y) = 2y.y′
Implicit differentiation:
We are interested in differentiating relations
which are implicitly defined.
To do this
we treat y as a function of x
and then apply our existing rules of
differentiation. A crucial rule will be the
chain rule.
For example:
d
dx(y2) = 2y.
d
dx(y) = 2y.y′
Implicit differentiation:
We are interested in differentiating relations
which are implicitly defined.
To do this
we treat y as a function of x
and then apply our existing rules of
differentiation. A crucial rule will be the
chain rule. For example:
d
dx(y2) = 2y.
d
dx(y) = 2y.y′
We apply this approach to our first example:
d
dx
(x2 + y2
)=
d
dx(25)
∴d
dx(x2) +
d
dx(y2) = 0
∴ 2x + 2y.y′ = 0
∴ y′ =−2x2y
=−xy
Note that y′ depends on BOTH x and y so
we can’t talk about the derivative at x = a.
We apply this approach to our first example:d
dx
(x2 + y2
)=
d
dx(25)
∴d
dx(x2) +
d
dx(y2) = 0
∴ 2x + 2y.y′ = 0
∴ y′ =−2x2y
=−xy
Note that y′ depends on BOTH x and y so
we can’t talk about the derivative at x = a.
We apply this approach to our first example:d
dx
(x2 + y2
)=
d
dx(25)
∴d
dx(x2) +
d
dx(y2) = 0
∴ 2x + 2y.y′ = 0
∴ y′ =−2x2y
=−xy
Note that y′ depends on BOTH x and y so
we can’t talk about the derivative at x = a.
We apply this approach to our first example:d
dx
(x2 + y2
)=
d
dx(25)
∴d
dx(x2) +
d
dx(y2) = 0
∴ 2x + 2y.y′ = 0
∴ y′ =−2x2y
=−xy
Note that y′ depends on BOTH x and y so
we can’t talk about the derivative at x = a.
We apply this approach to our first example:d
dx
(x2 + y2
)=
d
dx(25)
∴d
dx(x2) +
d
dx(y2) = 0
∴ 2x + 2y.y′ = 0
∴ y′ =−2x2y
=
−xy
Note that y′ depends on BOTH x and y so
we can’t talk about the derivative at x = a.
We apply this approach to our first example:d
dx
(x2 + y2
)=
d
dx(25)
∴d
dx(x2) +
d
dx(y2) = 0
∴ 2x + 2y.y′ = 0
∴ y′ =−2x2y
=−xy
Note that y′ depends on BOTH x and y so
we can’t talk about the derivative at x = a.
We apply this approach to our first example:d
dx
(x2 + y2
)=
d
dx(25)
∴d
dx(x2) +
d
dx(y2) = 0
∴ 2x + 2y.y′ = 0
∴ y′ =−2x2y
=−xy
Note that y′ depends on BOTH x and y so
we can’t talk about the derivative at x = a.
We apply this approach to our first example:d
dx
(x2 + y2
)=
d
dx(25)
∴d
dx(x2) +
d
dx(y2) = 0
∴ 2x + 2y.y′ = 0
∴ y′ =−2x2y
=−xy
However, we can calculate y′ at a point by
using both the x and y coordinates.
The slope of a tangent at a point
For y2 + x2 = 25 we have y′ =−xy
.
We emphasize that we need both the x and
y coordinate of a point to calculate y′ at that
point. Consider the points (3, 4) and (3,−4).
We get m = −34 for the gradient of the
tangent to the curve at the first point.
Substituting into y = mx + c we get
y = −0.75x + 6.25 as an equation of the
tangent.
The slope of a tangent at a point
For y2 + x2 = 25 we have y′ =−xy
.
We emphasize that we need both the x and
y coordinate of a point to calculate y′ at that
point.
Consider the points (3, 4) and (3,−4).
We get m = −34 for the gradient of the
tangent to the curve at the first point.
Substituting into y = mx + c we get
y = −0.75x + 6.25 as an equation of the
tangent.
The slope of a tangent at a point
For y2 + x2 = 25 we have y′ =−xy
.
We emphasize that we need both the x and
y coordinate of a point to calculate y′ at that
point. Consider the points (3, 4) and (3,−4).
We get m = −34 for the gradient of the
tangent to the curve at the first point.
Substituting into y = mx + c we get
y = −0.75x + 6.25 as an equation of the
tangent.
The slope of a tangent at a point
For y2 + x2 = 25 we have y′ =−xy
.
We emphasize that we need both the x and
y coordinate of a point to calculate y′ at that
point. Consider the points (3, 4) and (3,−4).
We get m = −34 for the gradient of the
tangent to the curve at the first point.
Substituting into y = mx + c we get
y = −0.75x + 6.25 as an equation of the
tangent.
The slope of a tangent at a point
For y2 + x2 = 25 we have y′ =−xy
.
We emphasize that we need both the x and
y coordinate of a point to calculate y′ at that
point. Consider the points (3, 4) and (3,−4).
We get m = −34 for the gradient of the
tangent to the curve at the first point.
Substituting into y = mx + c we get
y = −0.75x + 6.25 as an equation of the
tangent.
An equation for the tangent at the point
(3, 4) is y = −0.75x + 6.25.
An equation for the tangent at the point
(3,−4) is y = 0.75x− 6.25.
The Folium of Descartes
x3 + y3 = (3a)xy
Huh? What is a folium?
The Folium of Descartes continued...
x3 + y3 = (3a)xy
Let us consider the case of a = 2. Now use
implicit differentiation to find y′ of
x3 + y3 = 6xy
Find the equation of the tangent at the point
(3, 3).
We differentiate:
d
dx
(x3 + y3
)=
d
dx(6xy)
Remember: we regard y as function of x.
So, on the RHS we think of 6xy as the
product of 6x and y.
∴ 3x2 + 3y2.y′ =d
dx(6x)y +
d
dx(y)(6x)
∴ 3x2 + 3y2.y′ = 6y + y′6x
Now we solve for y′.
We differentiate:
d
dx
(x3 + y3
)=
d
dx(6xy)
Remember: we regard y as function of x.
So, on the RHS we think of 6xy as the
product of 6x and y.
∴ 3x2 + 3y2.y′ =d
dx(6x)y +
d
dx(y)(6x)
∴ 3x2 + 3y2.y′ = 6y + y′6x
Now we solve for y′.
We differentiate:
d
dx
(x3 + y3
)=
d
dx(6xy)
Remember: we regard y as function of x.
So, on the RHS we think of 6xy as the
product of 6x and y.
∴ 3x2 + 3y2.y′ =d
dx(6x)y +
d
dx(y)(6x)
∴ 3x2 + 3y2.y′ = 6y + y′6x
Now we solve for y′.
We differentiate:
d
dx
(x3 + y3
)=
d
dx(6xy)
Remember: we regard y as function of x.
So, on the RHS we think of 6xy as the
product of 6x and y.
∴ 3x2 + 3y2.y′ =d
dx(6x)y +
d
dx(y)(6x)
∴ 3x2 + 3y2.y′ = 6y + y′6x
Now we solve for y′.
We differentiate:
d
dx
(x3 + y3
)=
d
dx(6xy)
Remember: we regard y as function of x.
So, on the RHS we think of 6xy as the
product of 6x and y.
∴ 3x2 + 3y2.y′ =d
dx(6x)y +
d
dx(y)(6x)
∴ 3x2 + 3y2.y′ = 6y + y′6x
Now we solve for y′.
We had: 3x2 + 3y2.y′ = 6y + y′6x
∴ 3y2.y′ − y′6x = 6y − 3x2
y′ =6y − 3x2
3y2 − 6x=
2y − x2
y2 − 2x
Now, at the point (3, 3) we get y′ = −1.
Substituting into y = −x + c we get
y = −x + 6.
We had: 3x2 + 3y2.y′ = 6y + y′6x
∴ 3y2.y′ − y′6x = 6y − 3x2
y′ =6y − 3x2
3y2 − 6x=
2y − x2
y2 − 2x
Now, at the point (3, 3) we get y′ = −1.
Substituting into y = −x + c we get
y = −x + 6.
We had: 3x2 + 3y2.y′ = 6y + y′6x
∴ 3y2.y′ − y′6x = 6y − 3x2
y′ =6y − 3x2
3y2 − 6x=
2y − x2
y2 − 2x
Now, at the point (3, 3) we get y′ = −1.
Substituting into y = −x + c we get
y = −x + 6.
We had: 3x2 + 3y2.y′ = 6y + y′6x
∴ 3y2.y′ − y′6x = 6y − 3x2
y′ =6y − 3x2
3y2 − 6x=
2y − x2
y2 − 2x
Now, at the point (3, 3) we get y′ = −1.
Substituting into y = −x + c we get
y = −x + 6.
We had: 3x2 + 3y2.y′ = 6y + y′6x
∴ 3y2.y′ − y′6x = 6y − 3x2
y′ =6y − 3x2
3y2 − 6x=
2y − x2
y2 − 2x
Now, at the point (3, 3) we get y′ = −1.
Substituting into y = −x + c we get
y = −x + 6.
Examples:
1. Find y′ if sin(x + y) = y2 cosx
2. Find y′′ if x4 + y4 = 16
Remember that we consider y to be a
function of x.
Try each of these and then look at the
solutions on the slides that follow.
A big hint for (2.) is that you should
substitute y′ and the original equation into
your calculation for y′′.
Example: sin(x + y) = y2 cosx
Solution:d
dx(sin(x + y)) =
d
dx(y2 cosx).
We must apply the Chain Rule to the LHS
and treat the RHS as a product. So,
cos(x + y)d
dx(x + y)=
d
dx(y2)(cosx) +
d
dx(cosx)y2
∴ cos(x+y)(1+y′) = 2yy′ cosx−(sinx)y2
∴ cos(x + y) + y′ cos(x + y) = 2yy′ cosx− y2 sinx
∴ y′ cos(x+ y)− y′2y cosx=−y2 sinx− cos(x+ y)
Example: sin(x + y) = y2 cosx
Solution:d
dx(sin(x + y)) =
d
dx(y2 cosx).
We must apply the Chain Rule to the LHS
and treat the RHS as a product. So,
cos(x + y)d
dx(x + y)=
d
dx(y2)(cosx) +
d
dx(cosx)y2
∴ cos(x+y)(1+y′) = 2yy′ cosx−(sinx)y2
∴ cos(x + y) + y′ cos(x + y) = 2yy′ cosx− y2 sinx
∴ y′ cos(x+ y)− y′2y cosx=−y2 sinx− cos(x+ y)
Example: sin(x + y) = y2 cosx
Solution:d
dx(sin(x + y)) =
d
dx(y2 cosx).
We must apply the Chain Rule to the LHS
and treat the RHS as a product. So,
cos(x + y)d
dx(x + y)=
d
dx(y2)(cosx) +
d
dx(cosx)y2
∴ cos(x+y)(1+y′) = 2yy′ cosx−(sinx)y2
∴ cos(x + y) + y′ cos(x + y) = 2yy′ cosx− y2 sinx
∴ y′ cos(x+ y)− y′2y cosx=−y2 sinx− cos(x+ y)
Example: sin(x + y) = y2 cosx
Solution:d
dx(sin(x + y)) =
d
dx(y2 cosx).
We must apply the Chain Rule to the LHS
and treat the RHS as a product. So,
cos(x + y)d
dx(x + y)=
d
dx(y2)(cosx) +
d
dx(cosx)y2
∴ cos(x+y)(1+y′) = 2yy′ cosx−(sinx)y2
∴ cos(x + y) + y′ cos(x + y) = 2yy′ cosx− y2 sinx
∴ y′ cos(x+ y)− y′2y cosx=−y2 sinx− cos(x+ y)
Example: sin(x + y) = y2 cosx
Solution:d
dx(sin(x + y)) =
d
dx(y2 cosx).
We must apply the Chain Rule to the LHS
and treat the RHS as a product. So,
cos(x + y)d
dx(x + y)=
d
dx(y2)(cosx) +
d
dx(cosx)y2
∴ cos(x+y)(1+y′) = 2yy′ cosx−(sinx)y2
∴ cos(x + y) + y′ cos(x + y) = 2yy′ cosx− y2 sinx
∴ y′ cos(x+ y)− y′2y cosx=−y2 sinx− cos(x+ y)
We had
y′ cos(x+y)−y′2y cosx = −y2 sinx−cos(x+y)
Taking out y′ as a common factor on the
LHS gives:
y′(cos(x+y)−2y cosx) = −y2 sinx−cos(x+y)
Finally we get:
y′ =y2 sinx + cos(x + y)
2y cosx− cos(x + y)
We had
y′ cos(x+y)−y′2y cosx = −y2 sinx−cos(x+y)
Taking out y′ as a common factor on the
LHS gives:
y′(cos(x+y)−2y cosx) = −y2 sinx−cos(x+y)
Finally we get:
y′ =y2 sinx + cos(x + y)
2y cosx− cos(x + y)
We had
y′ cos(x+y)−y′2y cosx = −y2 sinx−cos(x+y)
Taking out y′ as a common factor on the
LHS gives:
y′(cos(x+y)−2y cosx) = −y2 sinx−cos(x+y)
Finally we get:
y′ =y2 sinx + cos(x + y)
2y cosx− cos(x + y)
Solution:d
dx
(x4 + y4
)=
d
dx(16), so
4x3 + 4y3y′ = 0 and hence y′ =−x3
y3.
We apply the quotient rule to get:
y′′ = −ddx(x
3)y3 − x3 ddx(y3)
y6
∴ y′′ = −3x2y3 − x3(3y2y′)
y6
Now we substitute y′ back in . . .
Solution:d
dx
(x4 + y4
)=
d
dx(16), so
4x3 + 4y3y′ = 0
and hence y′ =−x3
y3.
We apply the quotient rule to get:
y′′ = −ddx(x
3)y3 − x3 ddx(y3)
y6
∴ y′′ = −3x2y3 − x3(3y2y′)
y6
Now we substitute y′ back in . . .
Solution:d
dx
(x4 + y4
)=
d
dx(16), so
4x3 + 4y3y′ = 0 and hence y′ =−x3
y3.
We apply the quotient rule to get:
y′′ = −ddx(x
3)y3 − x3 ddx(y3)
y6
∴ y′′ = −3x2y3 − x3(3y2y′)
y6
Now we substitute y′ back in . . .
Solution:d
dx
(x4 + y4
)=
d
dx(16), so
4x3 + 4y3y′ = 0 and hence y′ =−x3
y3.
We apply the quotient rule to get:
y′′ = −ddx(x
3)y3 − x3 ddx(y3)
y6
∴ y′′ = −3x2y3 − x3(3y2y′)
y6
Now we substitute y′ back in . . .
Solution:d
dx
(x4 + y4
)=
d
dx(16), so
4x3 + 4y3y′ = 0 and hence y′ =−x3
y3.
We apply the quotient rule to get:
y′′ = −ddx(x
3)y3 − x3 ddx(y3)
y6
∴ y′′ = −3x2y3 − x3(3y2y′)
y6
Now we substitute y′ back in . . .
∴ y′′ = −3x2y3 − 3x3y2−x
3
y3
y6
Simplifying gives us
y′′ = −3(x2y4 + x6)
y7= −3x
2(y4 + x4)
y7
Now we substitute the original equation to
get:
y′′ = −3x2(16)
y7=−48x2
y7
∴ y′′ = −3x2y3 − 3x3y2−x
3
y3
y6
Simplifying gives us
y′′ = −3(x2y4 + x6)
y7= −3x
2(y4 + x4)
y7
Now we substitute the original equation to
get:
y′′ = −3x2(16)
y7=−48x2
y7
∴ y′′ = −3x2y3 − 3x3y2−x
3
y3
y6
Simplifying gives us
y′′ = −3(x2y4 + x6)
y7= −3x
2(y4 + x4)
y7
Now we substitute the original equation to
get:
y′′ = −3x2(16)
y7=−48x2
y7
Differentiating inverse trig functions:
The calculation of the derivatives of
y = arcsinx and y = arctanx are shown in
the textbook.
Here we show how to get the derivative of
y = cos−1(x)
Remember that inverse trig functions are
functions. Therefore we should expect to be
able to get their derivatives as functions of x.
Differentiating inverse trig functions:
The calculation of the derivatives of
y = arcsinx and y = arctanx are shown in
the textbook.
Here we show how to get the derivative of
y = cos−1(x)
Remember that inverse trig functions are
functions. Therefore we should expect to be
able to get their derivatives as functions of x.
Differentiating inverse trig functions:
Recall that
y = cos−1(x) ⇐⇒ x = cos y and 0 6 y 6 π
Instead of trying to differentiate
y = cos−1(x), we rather apply implicit
differentiation to cos y = x.
∴d
dxcos y =
d
dxx
∴ (− sin y)(y′) = 1 ⇒ y′ = −1/(sin y)
But, we want to express y′ in terms of x.
Differentiating inverse trig functions:
Recall that
y = cos−1(x) ⇐⇒ x = cos y and 0 6 y 6 π
Instead of trying to differentiate
y = cos−1(x), we rather apply implicit
differentiation to cos y = x.
∴d
dxcos y =
d
dxx
∴ (− sin y)(y′) = 1 ⇒ y′ = −1/(sin y)
But, we want to express y′ in terms of x.
Differentiating inverse trig functions:
Recall that
y = cos−1(x) ⇐⇒ x = cos y and 0 6 y 6 π
Instead of trying to differentiate
y = cos−1(x), we rather apply implicit
differentiation to cos y = x.
∴d
dxcos y =
d
dxx
∴ (− sin y)(y′) = 1 ⇒ y′ = −1/(sin y)
But, we want to express y′ in terms of x.
Differentiating inverse trig functions:
Recall that
y = cos−1(x) ⇐⇒ x = cos y and 0 6 y 6 π
Instead of trying to differentiate
y = cos−1(x), we rather apply implicit
differentiation to cos y = x.
∴d
dxcos y =
d
dxx
∴ (− sin y)(y′) = 1
⇒ y′ = −1/(sin y)
But, we want to express y′ in terms of x.
Differentiating inverse trig functions:
Recall that
y = cos−1(x) ⇐⇒ x = cos y and 0 6 y 6 π
Instead of trying to differentiate
y = cos−1(x), we rather apply implicit
differentiation to cos y = x.
∴d
dxcos y =
d
dxx
∴ (− sin y)(y′) = 1 ⇒ y′ = −1/(sin y)
But, we want to express y′ in terms of x.
Differentiating inverse trig functions:
Recall that
y = cos−1(x) ⇐⇒ x = cos y and 0 6 y 6 π
Instead of trying to differentiate
y = cos−1(x), we rather apply implicit
differentiation to cos y = x.
∴d
dxcos y =
d
dxx
∴ (− sin y)(y′) = 1 ⇒ y′ = −1/(sin y)
But, we want to express y′ in terms of x.
Differentiating y = cos−1(x) continued. . .
Since cos y = x we get cos2(y) = x2.
∴ 1−sin2(y) = x2 (cos2 θ+sin2 θ = 1)
∴ 1− x2 = sin2(y)
∴√
1− x2 =√
sin2 y
∴√
1− x2 = | sin y| = sin y (0 6 y 6 π)
Finally: y′ =−1√1− x2
Differentiating y = cos−1(x) continued. . .
Since cos y = x we get cos2(y) = x2.
∴ 1−sin2(y) = x2 (cos2 θ+sin2 θ = 1)
∴ 1− x2 = sin2(y)
∴√
1− x2 =√
sin2 y
∴√
1− x2 = | sin y| = sin y (0 6 y 6 π)
Finally: y′ =−1√1− x2
Differentiating y = cos−1(x) continued. . .
Since cos y = x we get cos2(y) = x2.
∴ 1−sin2(y) = x2 (cos2 θ+sin2 θ = 1)
∴ 1− x2 = sin2(y)
∴√
1− x2 =√
sin2 y
∴√
1− x2 = | sin y| = sin y (0 6 y 6 π)
Finally: y′ =−1√1− x2
Differentiating y = cos−1(x) continued. . .
Since cos y = x we get cos2(y) = x2.
∴ 1−sin2(y) = x2 (cos2 θ+sin2 θ = 1)
∴ 1− x2 = sin2(y)
∴√
1− x2 =√
sin2 y
∴√
1− x2 = | sin y| = sin y (0 6 y 6 π)
Finally: y′ =−1√1− x2
Differentiating y = cos−1(x) continued. . .
Since cos y = x we get cos2(y) = x2.
∴ 1−sin2(y) = x2 (cos2 θ+sin2 θ = 1)
∴ 1− x2 = sin2(y)
∴√
1− x2 =√
sin2 y
∴√1− x2 = | sin y| = sin y (0 6 y 6 π)
Finally: y′ =−1√1− x2
Differentiating y = cos−1(x) continued. . .
Since cos y = x we get cos2(y) = x2.
∴ 1−sin2(y) = x2 (cos2 θ+sin2 θ = 1)
∴ 1− x2 = sin2(y)
∴√
1− x2 =√
sin2 y
∴√1− x2 = | sin y| = sin y (0 6 y 6 π)
Finally: y′ =−1√1− x2
Note: the previous slide presents one way of
getting sin y in terms of x.
Since cos y = x =x
1, we could also draw a
triangle with an angle of y and Hyp. = 1,
Adj. = x.
That would give us Opp. =√1− x2.
Therefore
sin y =√1− x2.
Derivatives of inverse trig functions:
d
dx(sin−1 x) =
1√1− x2
d
dx(csc−1 x) =
−1x√x2 − 1
d
dx(cos−1 x) =
−1√1− x2
d
dx(sec−1 x) =
1
x√x2 − 1
d
dx(tan−1 x) =
1
1 + x2d
dx(cot−1 x) =
−11 + x2
Comparing y = arctanx and its derivative
y = tan−1(x) andd
dx
(tan−1 x
)=
1
1+ x2
Example: Differentiate y = x arctan√x.
Solution:
dy
dx=
d
dx(x) arctan
√x + x
d
dx
(arctan
√x)
= arctan√x + x
(1
1 + (√x)2
)· ddx
√x
= arctan√x + x
(1
1 + x
)· 1
2√x
= arctan√x +
√x
2(1 + x)
Example: Differentiate y = x arctan√x.
Solution:
dy
dx=
d
dx(x) arctan
√x + x
d
dx
(arctan
√x)
= arctan√x + x
(1
1 + (√x)2
)· ddx
√x
= arctan√x + x
(1
1 + x
)· 1
2√x
= arctan√x +
√x
2(1 + x)
Example: Differentiate y = x arctan√x.
Solution:
dy
dx=
d
dx(x) arctan
√x + x
d
dx
(arctan
√x)
= arctan√x + x
(1
1 + (√x)2
)· ddx
√x
= arctan√x + x
(1
1 + x
)· 1
2√x
= arctan√x +
√x
2(1 + x)
Example: Differentiate y = x arctan√x.
Solution:
dy
dx=
d
dx(x) arctan
√x + x
d
dx
(arctan
√x)
= arctan√x + x
(1
1 + (√x)2
)· ddx
√x
= arctan√x + x
(1
1 + x
)· 1
2√x
= arctan√x +
√x
2(1 + x)
Example: Differentiate y = x arctan√x.
Solution:
dy
dx=
d
dx(x) arctan
√x + x
d
dx
(arctan
√x)
= arctan√x + x
(1
1 + (√x)2
)· ddx
√x
= arctan√x + x
(1
1 + x
)· 1
2√x
= arctan√x +
√x
2(1 + x)
The prescribed tut problems for this section
are on the next slide. You should complete
them before going through the slides for
Ch 3.6.
But first, here is an interesting story about
Rene Descartes (remember our second
example of implicit differentiation used the
Folium of Descartes):
https://wild.maths.org/rene-descartes-and-
fly-ceiling
Prescribed tut problems:
Complete the following exercises from the
8th edition:
Ch 3.5:
1, 3, 5, 7, 11, 17, 19, 20, 25, 27, 35, 37, 49,
53, 60