Example cosh 2π₯β1
Prove that tanh2 π₯ = cosh 2π₯+1 Solution tanh2 π₯ sinh π₯ 2 tanh π₯ = ( ) cosh π₯ 2
sinh2 π₯
= cosh2 π₯ 1 sinh2 π₯ = (π π₯ β π βπ₯ )2 2 cosh2 π₯ =
1 π₯ (π + π βπ₯ )2 2
1 π₯ (π β π βπ₯ )2 cosh 2π₯ β 1 2 = = 1 π₯ (π + π βπ₯ )2 cosh 2π₯ + 1 2 1 2π₯ (π + π β2π₯ β 2) 2 = 1 2π₯ (π + π β2π₯ + 2) 2 π 2π₯ π β2π₯ + 2 β1 = 22π₯ π π β2π₯ + 2 2 +1 1 2π₯ (π + π β2π₯ ) β 1 2 1 2π₯ (π + π β2π₯ ) + 1 2 =
cosh 2π₯ β 1 cosh 2π₯ + 1
Hence proved Example 21.1.3 Prove thatcosh(π΄ + π΅) = cosh π΄ cosh π΅ + sinh π΄ sinh π΅ Solution From the left-hand side
π π΄ + π βπ΄ π π΅ + π βπ΅ π π΄ β π βπ΄ π π΅ β π βπ΅ cosh π΄ cosh π΅ + sinh π΄ sinh π΅ = ( )( )+( )( ) 2 2 2 2 π π΄+π΅ + π π΄βπ΅ + π π΅βπ΄ + π βπ΄βπ΅ π π΄+π΅ β π π΄βπ΅ β π π΅βπ΄ + π βπ΄βπ΅ =( )+( ) 4 4 =
2π π΄+π΅ + 2π βπ΄βπ΅ 4
=
2(π π΄+π΅ + π βπ΄βπ΅ ) 4
(π π΄+π΅ + π β(π΄+π΅) ) = 2 = cosh(π΄ + π΅). Hence cosh(π΄ + π΅) = cosh π΄ cosh π΅ + sinh π΄ sinh π΅
INVERSE HYPERBOLIC FUNCTIONS π¦ = coshβ1 π₯ means π₯ = cosh π¦ , π¦ β₯ 0, π₯ β₯ 1
GRAPHS OF HYPERBOLIC FUNCTIONS π¦ = πππ βπ₯ y
1
π¦ = 2 ππ₯
π¦ = π ππβπ₯ 0
y π¦ = πππ‘βπ₯ π¦=1
x π¦ = β1
π¦ = πππ‘βπ₯
y
π¦ = πππ βπ₯ π¦=1 π¦ = π ππβπ₯ 0
y
x
π¦ = π ππβπ₯
x
π¦ = ππ πβπ₯
ELEMENTARY DIFFERENTIAL CALCULUS The Concept of a Limit Consider the functions π(π₯) =
π₯2 β 4 π₯β2
The function is undefined at π₯ = 2 Let us examine the behavior of the function at π₯ = 2
π₯
π(π₯) =
π₯ 2 β4 π₯β2
π₯
π(π₯) =
1.9
3.9
2.1
4.1
1.99
3.99
2.01
4.01
1.999
3.999
2.001
4.001
1.9999
3.9999
2.0001
4.0001
π₯ 2 β4 π₯β2
Notice that as you move down the first column of the table, the π₯ βvalues get closer to 2 but are less than 2. We use the notation π₯ β 2β to indicate π₯ approaches 2 from the left. π₯ β 2+ to indicate π₯ approaches 2 from the right. We call lim π(π₯) and ππππ(π₯) one sided limit. π₯ β 2β π₯ β 2β Theorem A limit exists if and only if both corresponding one sided limits exists and are equal. That is lim π(π₯) = πΏ for some number πΏif and only if π₯βπ lim π(π₯) = ππππ(π₯) π₯ β aβ π₯ β a+
Example Determine if the limit exists for the following a) lim
π₯ 2 β4
π₯β2 π₯β2 π₯
b) lim |π₯| π₯β0
Solution a) limβ
π₯ 2 β4 π₯β2
π₯β2
= limβ
(π₯β2)(π₯+2) π₯β2
π₯β2
lim (π₯ + 2) = 4
π₯β2β
and lim+
π₯ 2 β4
π₯β2
π₯β2
= lim+
(π₯β2)(π₯+2)
π₯β2
π₯β2
lim (π₯ + 2) = 4
π₯β2β
β΄ limβ = 4 = lim+ π₯β2
π₯β2
Hence the limit exists.
π₯
b) lim |π₯| π₯β0
Solution π₯, |π₯| = { βπ₯,
π₯β₯0 π₯<0
π₯ =1 π₯β0 π₯β0 π₯ π₯ limβ π(π₯) = limβ = β1 π₯β0 π₯β0 βπ₯ lim+ π(π₯) = lim+
Since lim+ π(π₯) β limβ π(π₯) the limit does not exist. π₯β0
π₯β0
y 1 π(π₯) 0βπ₯
π₯β0 π(π₯)
-1 By definition π₯
π₯
π(π₯) = π₯ = 1 and π(π₯) = βπ₯ = β1
Theorem 1.2 sin π₯ =1 π₯β0 π₯ lim
Example Evaluate the following a) lim
π₯β0
cos2 π₯
b) lim
π₯
π₯β0
Solution a) lim
π₯β0
b) lim
π₯β0
cos2 π₯ π₯
tan3 π₯ π₯
= 2 lim
cos2 π₯ 2π₯
π₯β0
tan3 π₯
= lim3 ( π₯β0
3π₯
=2
)=3
tan3 π₯ π₯
COMPUTATION OF LIMITS For any constant π and any real number π, lim π = π
(1)
π₯βπ
For any real number π, lim π₯ = π
(2)
π₯βπ
Theorem 2.1 lim π( π₯) and lim π( π₯) both exists, and let π be any constant. The
Suppose that
π₯βπ
π₯βπ
following then apply; i)
lim [π. π(π₯)] = π lim π(π₯)
ii)
lim [π(π₯) Β± π(π₯)] = lim π(π₯) Β± lim π(π₯)
iii)
lim [π(π₯). π(π₯)] = [lim π(π₯)[ lim π(π₯)]
π₯βπ
π₯βπ
π₯βπ
π₯βπ
π₯βπ
π(π₯)
lim π(π₯) =
iv)
π₯βπ
π₯βπ lim π(π₯)
π₯βπ
lim π(π₯)
π₯βπ
π₯βπ
π₯βπ
if lim π(π₯) β 0 π₯βπ
Example Apply the rule of limits to evaluate a) lim(3π₯ 2 β 5π₯ + 4) π₯β2
b) lim
π₯β3
c) lim
π₯ 3 β5π₯+4 π₯ 2 β2 π₯ 2 β1
π₯β1 1βπ₯ βπ₯+2ββ2 π₯ π₯β0
d) lim
Solution a) lim(3π₯ 2 β 5π₯ + 4) = lim3π₯ 2 β lim5π₯ + lim4 π₯β2
= 12 β 10 + 4 =6
π₯β2
π₯β2
π₯β2
b) lim
π₯ 3 β5π₯+4
=
π₯ 2 β2
π₯β3
c) lim
π₯ 2 β1
π₯β1 1βπ₯
(3)3 β5(3)+4
= πππ
(3)2 β2 (π₯β1)(π₯+1) β(π₯β1)
π₯β1
=
16 7
= β2
βπ₯+2ββ2 π₯ π₯β0
d) lim
lim
(βπ₯+2ββ2)(βπ₯+2+β2) π₯(βπ₯+2+β2)
π₯β0
π₯+2β2
lim π₯(βπ₯+2+β2)
π₯β0
π₯
lim
π₯β0 π₯(βπ₯+2+β2)
1
lim
π₯β0 (βπ₯
+ 2 + β2)
1 β2 + β2
=
1 2β2
Theorem 2.2 For any polynomial π(π₯) and any real number π, lim π(π₯) = π(π)
π₯βπ
Theorem 2.3 Suppose that lim π(π₯) = πΏ and π is any positive integer, Then π₯βπ
π
π
lim βπ(π₯) = πβ lim π(π₯) = βπΏ π₯βπ π₯βπ Where for π even, we assume that πΏ > 0
Theorem 2.4 For any real number π, we have; i) ii)
lim sin π₯ = sin π
π₯βπ
lim cos π₯ = cos π
π₯βπ
lim π π₯ = π π
iii)
π₯βπ
lim ln π₯ = ln π for π > 0
iv)
π₯βπ
lim sinβ1 π₯ = sinβ1 π for β1 < π < 1
v)
π₯βπ
lim cosβ1 π₯ = cosβ1 π for β1 < π < 1
vi)
π₯βπ
lim tanβ1 π₯ = tanβ1 π for ββ < π < β
vii)
π₯βπ
and If P is a polynomial and lim π(π₯) = πΏ, then π₯βπ
lim π(π(π₯)) = πΏ
π₯βπ
Example 5
a) Evaluate lim β3π₯ 2 β 2π₯ π₯β2
b) Evaluate lim sinβ1 (
π₯+1
π₯β0
2
)
c) Evaluate lim(π₯πππ‘π₯) π₯β0
Solution 5
5
a) lim β3π₯ 2 β 2π₯ = 5βlim3π₯ 2 β 2π₯ = β8 π₯β2 π₯β2 b) lim sinβ1 ( π₯β0
π₯+1 2
1
) = sinβ1 (2) =
π 6
c) lim(π₯πππ‘π₯) = (lim π₯) (limπππ‘π₯) = 0.0 ? π₯β0
π₯β0
π₯β0
cos π₯
π₯
β΄ lim(π₯πππ‘π₯) = lim (π₯. sin π₯ ) = lim (sin π₯) (cos π₯) π₯β0
π₯β0
π₯ (lim ) (lim cos π₯) sin π₯ π₯β0 π₯β0
1 sin π₯ ) (lim cos π₯) = 1 lim ( π₯β0 π₯β0 π₯
π₯β0
Theorem 2.5 SQUEEZ THEOREM Suppose that π(π₯) β€ π(π₯) β€ β(π₯) For all π₯ in some interval (π, π), except possibly at the point π β (π, π) and that lim π(π₯) = lim β(π₯) = πΏ
π₯βπ
π₯βπ
For some number πΏ. Then it follows that lim π(π₯) = πΏ also.
π₯βπ
Example 1
Evaluate π‘βπ lim [π₯ 2 cos (π₯)] π₯β0
Solution 1 lim [π₯ 2 cos ( )] π₯β0 π₯ 1 (β1 β€ cos ( ) β€ 1) π₯ 2 π₯ 1 βπ₯ 2 β€ π₯ 2 cos ( ) β€ π₯ 2 π₯ π₯β 0 limβπ₯ 2 = 0 = limπ₯ 2
π₯β0
π₯β0
β΄ from the squeeze theorem, it follows that 1 limπ₯ 2 cos ( ) = 0 π₯β0 π₯
A LIMIT FOR A PIECEWISE FUNCTION Example Evaluate limπ(π₯), where π(π₯) is defined by π₯β0
π₯ 2 + 2πππ π₯ + 1, πππ π₯ < 0, π(π₯) = π(π₯) = { π π₯ β 4,
πππ π₯ β₯ 0
Solution lim π(π₯) = limβ (π₯ 2 + 2πππ π₯ + 1) = 3
π₯β0β
π₯β0
and also lim (π π₯ β 4) = π 0 β 4 = 1 β 4 = β3
π₯β0β
Thus limπ(π₯) does not exist π₯β0
LIMITS INVOLVING INFINITY; ASYMPTOTES Example Examine lim
1
π₯β0 π₯
solution
π(π₯)
0 π(π₯)
lim+
π₯β0
limβ
π₯β0
1 =β π₯ 1 π₯
= ββ the limit does not exist 1
The graph of π¦ = π₯ approaches the vertical line π₯ = 0, as π₯ β 0 as shown above When this occurs, we say that the line π₯ = 0.
Example Evaluate lim
1
π₯β0 π₯ 2
π(π₯)
π(π₯)
solution 0
1 =β π₯β0 π₯ 2 1 limβ 2 = ββ π₯β0 π₯ The limit does not exist. lim+
LIMITS AT INFINTY 1
1
Returning to π(π₯) = π₯ , we can see that as π₯ β β, π₯ β 0. In view of this, we write 1 =0 π₯ββ π₯ lim
1 =0 π₯βββ π₯ lim
The graph appears to approach the horizontal line π¦ = 0, as π₯ β β and as π₯ β ββ. In this case, we call π¦ = 0 a horizontal asymptote. A LIMIT OF A QUOTIENT THAT IS NOT THE QUOTIENT OF A LIMIT Example Evaluate lim
5π₯β7
π₯ββ 4π₯+3
Solution lim
π₯ββ
lim (5π₯β7)
5π₯β7
β
= π₯ββ =β ? 4π₯+3 lim (4π₯+3) π₯ββ
NOTE: i) ii) iii) iv)
β
indeterminate form
β β
0 β. β 0.0
Rule of thumbs β
When faced with the indeterminate form β in calculating limits of a rational function, divide numerator and denominator by the highest power of x appearing in the denominator.
Here we have 5π₯ 7 7 βπ₯ 5βπ₯ 5 5π₯ β 7 π₯ lim = = lim = 4π₯ 3 π₯ββ 3 4 π₯ββ 4π₯ + 3 4+π₯ π₯ +π₯
Example Evaluate lim
4π₯ 3 +5
π₯ββ β6π₯ 2 β7π₯
Solution 4π₯ 3 5 + 2 4π₯ 3 + 5 π₯2 π₯ lim = lim π₯ββ β6π₯ 2 β 7π₯ π₯ββ 6π₯ 2 7π₯ β 2 β 2 π₯ π₯ 5 2 π₯ lim = ββ 7 π₯ββ β6 β π₯ 4π₯ +
Two LIMITS OF AN INVERSE TRIGONOMETRIC FUNCTION Evaluate lim tanβ1 π₯ and lim tanβ1 π₯ π₯ββ
π₯ββ
y
y = tanβ1 π₯
π
π
β2
lim tanβ1 π₯ =
π₯ββ
2
π 2
lim tanβ1 π₯ = β
π₯βββ
π 2
π 2
π¦ = tanβ1 π₯
π
β2
Example Evaluate lim (βπ + 1 β βπ) π₯ββ
Solution (βπ+1ββπ)
lim (βπ + 1 β βπ) (
π₯ββ
lim
π + 1 + βπ βπ + 1 β βπ βπ + 1 β π βπ + 1 + βπ
π₯ββ
lim
βπ+1ββπ)
1
π₯ββ βπ
+ 1 + βπ 1
π+1 βπ β π + βπ lim
π₯ββ
lim
π₯ββ
1 1 βπ β ( 1 + π + 1) π β 1 βπ 1 βπ β ( 1 + π + 1) βπ
=
0 =0 2
CONTINUITY Definition A function f is continuous at π₯ = π when π(π₯) is defined lim π(π₯) exists
i) ii)
π₯βπ
lim π(π₯) = π(π)
iii)
π₯βπ
Otherwise,π is said to be discontinuous at π₯ = π As an example of a continuous function, let us investigate π(π₯) = π₯ 2 At some fixed value π₯ = π. certainly π(π) = π 2 at π₯ = π. Furthermore, the difference π(π₯) β π(π) = π₯ 2 β π 2 = (π₯ β π)(π₯ + π) Approaches zero as a limit when π₯ β π approaches zero, since as when π₯ βΆ π, We have lim[π(π₯) β π(π)] = lim(π₯ β π)lim(π₯ + π) 0.2π = 0 β΄ π(π₯) = π₯ 2 is continuous at any point where π₯ = π
Example 3.1 Finding where a rational function is continuous Determine where π(π₯) =
π₯ 2 +2π₯β3 π₯β1
is continuous
Solution π(π₯) =
π₯ 2 +2π₯β3 π₯β1
=
(π₯β1)(π₯+3) π₯β1
=π₯+3
for π₯ β 1 this says that the graph of π is a straight line but with a hole in it at π₯ = 1 β΄ π is discontinuous at π₯ = 1 but continuous everywhere
{π·: π₯ β β|π₯ β 1} y
π¦=
π₯ 2 +2π₯β3 π₯β1
4
5
x
Example Removing a discontinuity Let us redefine example 3.1 to make it continuous everywhere
π₯ 2 + 2π₯ β 3 , ππ π₯ β 1 π(π₯) = { π₯ β 1 π, ππ π₯=1
limπ(π₯) = lim
π₯β1
π₯2 + 2π₯ β 3
π₯β1
π₯β1
=
(π₯ β 1)(π₯ + 3) π₯β1 π₯β1 lim
lim(π₯ + 3) = 4
π₯β1
Now if we choose π = 4,then limπ(π₯) = 4 = π(1) and so g is continuous at π₯ = 1.
π₯β1
NOTE: When we can remove a discontinuity by redefining the function at that point, we call the discontinuity a removable discontinuity. Example The function f defined by π(π₯) =
sin π₯ π₯
for π₯ β 0
has a removable discontinuity at π₯ = 0 , the formula is not valid when π₯ = 0 but lim
π₯β0
sin π₯ π₯
=1
sin π₯ π(π₯) = { π₯ , 1,
π€βππ π₯ β 0 π€βππ π₯ = 0
by so defining the value of f at 0, we have made f continuous there, since we now have π(π₯) = ππππ(π₯) as π₯ approaches zero. Non-removable discontinuity The discontinuity at π₯ = 0 in the foregoing example could be removed because f had a limit, namely 1, as π₯ approaches zero. On the other hand, if π(π₯) =
|π₯| π₯
for π₯ β 0
Then there is a discontinuity at 0, that can be removed. π₯, ππ π₯ β₯ 0 |π₯| = { βπ₯, π₯<0 π₯ =1 π₯β0 π₯ π₯ limβ = 1 π₯β0 π₯ lim+
β΄ the limit does not exist. If we assign the value 0 to g(0), the resulting function is the signum function ( or sign function) of π₯. +1 signπ₯ = { 0 β1
ππ π₯ > 0 ππ π₯ = 0 ππ π₯ < 0
the signum function is defined for all π₯, but it is not continuous at π₯ = 0. It is continuous for π₯ β 0 Example Non-removable discontinuity π(π₯) =
1 π₯2
Solution We should observe from the diagram 1 =β π₯β0 π₯ 2 lim
β΄ the limit does not exist .
-3
3
Hence π is discontinuous at π₯ = 0 and non- removable. Theorem All polynomials are continuous everywhere. Additionally, π πππ₯, πππ π₯, tanβ1 π₯ πππ π π₯ are π continuous everywhere. βπ₯ is continuous for all π₯, when n is odd and for π₯ β₯ 0 when n is even. We also have that ln π₯ is continuous for π₯ > 0 and sinβ1 π₯ and cos β1 π₯ are continuous for β1 < π₯ < 1 Theorem Suppose that π πππ π are continuous at π₯ = π. Then all of the following are true: i) (π Β± π) is continuous at x=a ii) (π. π) is continuous at x=a and π
iii) (π) is continuous at π₯ = π if π(π) β 0 Theorem Suppose that lim π(π₯) = πΏ and π is continuous at πΏ then, π₯βπ
lim π(π(π₯)) = π(ππππ(π₯)) = π(πΏ) π₯βπ
π₯βπ
Corollary 3.1 Suppose that π is continuous at a and π is continuous at π(π). Then, the composition πππ is continuous at a. Example Continuity for a composite function Determine where β(π₯) = cos(π₯ 2 β 5π₯ + 2) is continuous. Solution Note that β(π₯) = π(π(π₯)) Where π(π₯) = π₯ 2 β 5π₯ + 2 and π(π₯) = πππ π₯ Since both π πππ π are continuous for all x, h is also continuous for all x by corollary 3.1 Definition 3.2 If f is continuous at every point on an open interval (π, π), we say that f is continuous on the closed interval [π, π], if f is continuous on the open interval (π, π) and lim π(π₯) = π(π) and limβπ(π₯) = π(π).
π₯βπ+
π₯βπ
Finally, if π is continuous on all of π(ββ, β), we simply say that π is continuous. Example Determine the interval where π is continuous for, a) π(π₯) = β4 β π₯ 2 b) π(π₯) = ln(π₯ β 3) solution a) π(π₯) = β4 β π₯ 2 β4 β π₯ 2 β₯ 0 2
(β4 β π₯ 2 ) β₯ (0)2 4 β π₯2 β₯ 0 (β1) β π₯ 2 β₯ β4(β1) π₯2 β€ 4 βπ₯ 2 β€ Β±β4 |π₯| β€ Β±2
recall that |π₯| = βπ₯ 2
β2 β€ π₯ β€ 2
b)
π(π₯) = ln(π₯ β 3)
solution π₯β3>0 βΉπ₯ >3 β΄ π is continuous on the interval (3, β).
Theorem The intermediate value theorem Suppose that π is continuous on the closed interval [π, π] and w is any number between π(π) and π(π). Then there is a number π β [π, π] for which π(π) = π€.
CORRALARY Suppose that π is continuous on [π, π] and π(π) and π(π) have opposite signs [π. π π(π). π(π) < 0]. Then there is at least one number π β (π, π) for which π(π) = 0 (recall that c is then a zero of f) Note: Lemma lim
πβ0
1βcos π π
=0
DIFFERENTIATION THE GENERAL CASE To find the slope of the tangent line to π¦ = π(π₯) ππ‘ π₯ = π, first pick two points on the curve, one point is the point of tangency (π, π(π)). Call the x-coordinate of the secant point π₯ = π + β, for some small number corresponding y-coordinates is π(π + β).It is natural to think of h as being positive , as shown in figure (a), h can also be negative as shown in figure (b)
β
β π
π+β
π+β
π
a)
b) secant line β > 0
secant line β < 0
the slope of the secant line through the point (π, π(π)) and (π + β, π(π + β) is given by
ππ ππ =
π(π+β)βπ(π) (π+β)βπ
=
π(π+β)βπ(π) β
1.1
Notice that the expression in 1.1 is called a difference quotient gives the slope of the secant line for any secant point we might choose (that is for any β β 0)
In order to obtain an improved approximation to the tangent line, we zoom in closer and closer towards the point of tangency. This makes the two points closer together to 0 as shown below. y
π
β
β π β β β x
Notice that as the point Q approaches the point P(π. π , ππ β β 0), the secant line approaches the tangent line at P. Definition The slope ππ‘ππ of the tangent line to π¦ = π(π₯) at π₯ = π is given by
π(π + β) β π(π) ββ0 β
π β² (π) = lim
Provided the limit exists. If the limit exists, we say that π is differentiable at π₯ = π. π(π₯+β)βπ(π₯) β ββ0
Or the derivative of π(π₯) is the function π β² (π₯) given by π β² (π₯) = lim
provided
the limit exists. The process of computing a derivative is called differentiation. Further, f is differentiable at a point on an interval πΌ if it is differentiable at every point in πΌ. This is also called the 1π π‘ principle of derivative. Example Use the definition to find the derivative function of the following. a) π(π₯) = βπ₯ πππ π₯ > 0 b) π(π₯) = sin π₯
solution
π(π₯ + β) β π(π₯) ββ0 β
π β² (π₯) = lim
βπ₯+βββπ₯ β ββ0
= lim = lim
(βπ₯ + β β βπ₯)(βπ₯ + β + βπ₯) β(βπ₯ + β + βπ₯)
ββ0
(π₯+β)βπ₯
= lim β(βπ₯+β+
βπ₯)
ββ0
1
= lim
ββ0 βπ₯
= =
+ β + βπ₯
1 βπ₯ + 0 + βπ₯ 1 2 βπ₯
b) π(π₯) = sin π₯ π(π₯ + β) β π(π₯) ββ0 β
π β² (π₯) = lim
sin(π₯ + β) β π πππ₯ ββ0 β
= lim
π πππ₯ πππ β + πππ π₯ π πππ₯ β π πππ₯ ββ0 β
= lim
(πππ π₯ β 1) π ππβ + πππ π₯ lim ββ0 ββ0 β β
= π πππ₯ lim
= π πππ₯(0) + πππ π₯(1) = πππ π₯
ALTERNATIVE DERIVATIVE NOTATIONS We have denoted the derivative function by π β² (π₯). There are other Commonly used notations, each with advantages and disadvantages. One of the ππ
converts of calculus, Leibniz, used the notation ππ₯ (Leibniz notation) for the derivative. If we write π¦ = π(π₯), the following are all alternatives for denoting the derivative
π β² (π₯) = π¦ β² =
ππ¦ ππ₯
=
ππ ππ₯
=
π ππ₯
π(π₯)
π
The expression ππ₯ is called a differential operator and tells you to take the derivative of whatever expression follows. THEOREM If π(π₯) is differentiable at π₯ = π ,then π(π₯) is continuous at π₯ = π. Example Show that π(π₯) = {
4, ππ π₯ < 2 2π₯ ππ, π₯ β₯ 2
is not differentiable at π₯ = 2
Solution
π(π₯+β)βπ(π₯)
π β² (π₯) = limβ
β
ββ0
limβ
π(π₯+β)βπ(π₯)
= limβ
β
ββ0
π(π₯+β)βπ(π₯) β
ββ0
2π₯+2ββ2π₯
ββ0
β
ββ0
π β² (π₯) = lim+ lim+
π(2+β)βπ(2)
= lim+
ββ0
2(π₯+β)β2(π₯)
ββ0
=2
2
β΄ π β² (π₯) β π β² (π₯) lim
ββ0β
lim
ββ0+
The function is not continuous at π₯ = 2 COMPUTATION OF DERIVATIVES For any constant c, π ππ₯
(π) = 0
Similarly, π ππ₯
π₯=1
Theorem (power rule) For any integer π > 0, π ππ₯
π₯ π = ππ₯ πβ1
Theorem (General power rule) For any real number π ,
π ππ₯
= limβ
π₯ π = ππ₯ πβ1
β
4β4 β
=0
Example Find the derivatives of the following a)
1 π₯ 19 3
b) βπ₯ 2 c)
π₯π
solution a)
1 π₯ 19 π
( ππ₯
19 1 π ) = ππ₯ π₯ β19 = β19π₯ β19β1 = β19π₯ β20 = π₯ β20 19 π₯ 2
3
b) βπ₯ 2 = π₯ 3 π 3
2
π
2
2
2
1
βπ₯ 2 = ππ₯ π₯ 3 = 3 π₯ 3β1 = 3 π₯ β3 = ππ₯ c)
π ππ₯
2 1 3π₯ 3
=
2 3
3 βπ₯
π₯ π = ππ₯ πβ1
GENERAL DERIVATIVE RULES THEOREM If π(π₯) and π(π₯) are differentiable at π₯ and π is any constant, then (i) (ii) (iii)
π ππ₯ π ππ₯ π ππ₯
[π(π₯) + π(π₯)] = π β² (π₯) + πβ² (π₯) [π(π₯) β π(π₯)] = π β² (π₯) β πβ² (π₯) and [ππ(π₯)] = ππ β² (π₯)
Example Find the derivative of a) π(π₯) = 2π₯ 6 + 3βπ₯ b) π(π₯) =
4π₯ 2 β3π₯+2βπ₯ π₯
Solution π
π
a) π β² (π₯) = ππ₯ (2π₯ 6 ) + ππ₯ (3βπ₯) π
π
1
1
= 2 ππ₯ (π₯ 6 ) + 3 ππ₯ (βπ₯) = 2(6π₯ 5 ) + 3 (2) π₯ β2 = 12π₯ 5 + 2
3
βπ₯
b)