f : R -> R : x -> axis called an exponential function with base a.
From the graphs we see that
y = 3x ; y = 0.5x ; y = 100.2x-1
f : R -> R : x -> axare either increasing or decreasing, the inverse functions are defined. The inverse function is called the logarithmic function with base a. We write
loga(x)
log10(x) is written as log(x)
So,
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loga(x) = y <=> ay = x |
log2(8) = 3 ; log3(sqrt(3)) = 0.5 ; log(0.01) = -2
From the definition it follows immediately that
for x > 0 we have aloga(x) = x
and
for all x we have loga(ax) = x
|
From the graphs we see that
log2(x) ; log(2x+4) ; log0.5(x)
Let log(x.y) = u then au = x.y (1)
Let log(x) = v then av = x (2)
Let log(y) = w then aw = y (3)
From (1) , (2) and (3)
au = av . aw
=> au = av + w
=> u = v + w
So,
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loga(x.y) = loga(x) + loga(y) |
|
loga(x/y) = loga(x) - loga(y) |
|
loga(xr ) = r.loga(x) |
log(x2 y3) = 2 log(x) + 3 log(y)
log(x2 / y3) = 2 log(x) - 3 log(y)
log( xy )= y log(x)
1
log ------ = log(1) - log((xy)3) = -3log(xy) = -3 (log(x)+log(y))
(xy)3
log(2x) + log(3x) = log(6x2)
3log(x) + a log(x) = (3+a) log(x) = log(x3+a)
0.5 log(x) = log(sqrt(x))
Show that xlog(y) / ylog(x) = 1
The statement implies that x and y are positive, so we can write
xlog(y) / ylog(x) = 1 <=> xlog(y) = ylog(x) <=> log( xlog(y) ) = log( ylog(x) ) <=> log(y).log(x) = log(x).log(y)
1
loga(x) =( -------) . logb(x)
logb(a)
|
logb(a) . loga(x) = logb(x)
Let logb(a) = u then bu = a (1)
Let loga(x) = v then av = x (2)
Let logb(x) = w then bw = x (3)
From (2) and (3) we have
av = bw
Using (1)
bu.v = bw
So,
u.v = w
=> logb(a) . loga(x) = logb(x)
log(12.5) = 1.0969 log2(12) = log(12)/log(2) = 3.58496 log(1/154)= -log(154) = -2.1875 log7(0.514) = 14 log(0.5)/log(7) = -4.9869 log(-12.4) is not defined
f(x) = ax
Appealing on the definition of the derivative, we can write
(f(x+h)-f(x))
f'(x) = lim ---------------
h->0 h
ax+h - ax
= lim ------------
h->0 h
ax (ah - 1)
= lim -----------
h->0 h
(since ax is constant relative to h )
(ah - 1)
= ax . lim -----------
h->0 h
Now,
(ah - 1)
lim ----------- is a constant depending on the value of the base a.
h->0 h
It can be proved that there is a unique value of a, such that this limit is 1.
This very special value of a is called e.
(eh - 1)
lim ----------- = 1
h->0 h
(eh - 1)
lim ----------- = 1
0 h
means that for very very small values of h
eh - 1 is approximately h
<=> eh is approximately h +1
<=> e is approximately (1 + h)1/h
So,
e = lim (1 + h)1/h = 2.718 28...
0
|
e = lim (1 + 1/t)t = 2.718 28...
infty
|
|
loge(x) = ln(x) |
The number a is a strictly positive number.
ak = er <=> ln(ak) = r <=> r = k.ln(a) Then (ak)x = (er)x <=> r = k.ln(a) for all x <=> akx = erx <=> r = k.ln(a) for all xThe functions A.akx and A.erx are identical if and only if r = k.ln(a)
Example:
14 . 32.7x is identical with 14 . e2.97x
6 . (0.25)-x is identical with 6 . e1.39x
Working with the functions with base e, has many benefits for algebraic calculations.
The product of the functions with base e, from the previous example, is much easier to work with.
Compare the expressions: 14 e2.97 x 6 e1.39 x and 14 32.7x 6 (0.25)-x.
We'll find the value of h, such that y2 = y1/2.
y2 = (1/2) y1
<=> e-r(a+h) = (1/2) e-ra
<=> e-ra e-rh = (1/2) e-ra
<=> e-rh = (1/2)
<=> - rh = ln(1/2)
<=> - rh = ln(1) -ln(2)
<=> - rh = -ln(2)
<=> h = ln(2)/r
If we increase x with ln(2)/r, then the image of e-rx reduces to half the initial value.
Remarkable is that ln(2)/r does not depend on our initial value a.
This means that the image is halved, when a random initial value of x increases with ln(2)/r.
That's why ln(2)/r is called the 'half value' of the function e-rx.
Example : Take the function y = e-0.5x.
The half value is ln(2)/0.5 = 1.386
Exercise: plot the graph and check all previous properties.
Let f(x) = log(x) , then
(f(x+h)-f(x))
f'(x) = lim ---------------
h->0 h
(log(x+h)-log(x))
<=> f'(x) = lim -------------------
h->0 h
log( (x+h)/x )
<=> f'(x) = lim -------------------
h->0 h
1
<=> f'(x) = lim --- . log( (x+h)/x )
h->0 h
<=> f'(x) = lim log( (x+h)/x )1/h
h->0
<=> f'(x) = lim log( (x+h)/x )1/h
h->0
<=> f'(x) = lim log(1 + h/x)1/h
h->0
<=> f'(x) = lim log((1 + h/x)x/h )1/x
h->0
<=> f'(x) = lim (1/x).log(1 + h/x)x/h
h->0
<=> f'(x) =(1/x). lim log(1 + h/x)x/h
h->0
<=> f'(x) =(1/x). lim log(1 + h/x)x/h
h/x->0
<=> f'(x) =(1/x).log lim (1 + h/x)x/h
h/x->0
<=> f'(x) =(1/x).log(e)
<=> f'(x) =(1/x).ln(e)/ln(a)
<=> f'(x) =(1/x)/ln(a)
1
<=> f'(x) = ----------
x. ln(a)
d 1
-- loga(x) = ----------
dx x. ln(a)
d 1
-- loga(u) = ---------- . u'
dx u. ln(a)
d 1
-- ln(x) = ---
dx x
d 1
-- ln(u) = ---.u'
dx u
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y = ln(2x2+6)
y' = (1/(2x2+6)). 4x
---------------------------
y = ln2(x)
y' = 2 ln(x) . (1/x)
---------------------------
y = ln(1/x)
y'= x.(-1/x2) = -1/x
---------------------------
y = ln(ln(x))
y'= (1/ln(x)) . (1/x)
---------------------------
y = x3 ln(x)
y'= (3x2).ln(x) + (x3).(1/x) = (3x2).ln(x) + x2
---------------------------
y = log3(x2)
y'= (1/(x2.ln(3)).(2x) = 2/(x ln(3))
---------------------------
y = ln(x)/x
x.(1/x) - ln(x) 1 - ln(x)
y'= ------------------ = ------------
x2 x2
---------------------------
y = ln(sqrt(2x2+x))
first we rewrite y
y = 0.5 ln(2x2+x)
4x+1
y'= 0.5 ----------
2x2+x
---------------------------
y = sqrt(ln(x2))
1
y'= --------------- .(2/x)
2 sqrt(ln(x2))
Let f(x) = ax, then loga(ax ) and x are identical functions.
Hence, the derivative of both functions is the same.
So,
1
---------- .(ax )' = 1
ax .ln(a)
d
<=> ---(ax ) = ax .ln(a)
dx
d
---(ax ) = ax .ln(a)
dx
d
--(ex ) = ex
dx
d
--(au ) = au .ln(a).u'
dx
d
--(eu ) = eu .u'
dx
|
y = x.e-5x
y'= e-5x + x.(-5)e-5x
---------------------------
y = 32x
y'= 32x ln(3) 2 = 32x ln(9)
---------------------------
y = ex/x2
x2 ex - ex 2x
y'= ------------------
x4
ex (x-2)
= ------------
x3
---------------------------
y = (3e)x
y'= (3e)x ln(3e) = (3e)x (ln3 +lne) = (3e)x (ln3 + 1)
---------------------------
y = arcsin(2x)
2x ln(2)
y'= -----------------
sqrt(1-22x)
Let f(x) = xr with r any real number.
xr = er.ln(x)
=>
d
--(xr) = er.ln(x).(r.ln(x))'
dx
= xr.r.(1/x)
= r.xr-1
Thus,
For any real number r, we have
d --(ur) = r.ur-1.u' dx |
uv = ev.ln(u)
d
--(uv) = ev.ln(u).(v.ln(u))'
dx
= uv . (v' ln(u) + v.(1/u).u'
= v uv-1 u' + uv.ln(u).v'
d --(uv) = v uv-1 u' + uv.ln(u).v' dx |
y = xx y'= xx ln(x) + x xx-1 = xx (1 + ln(x)) y = (ln(x))2x y'= (ln(x))2x ln(ln(x)).2 + 2x.(ln(x))2x-1 (1/x) y = (ex)x we rewrite y: y = ex2 y'= ex2 2x
ln(x) 1/x
lim ------- = lim ------- = 0
infty x infty 1
xn n.xn-1
lim ------ = lim ---------
infty ex ex
n.(n-1)xn-2
= lim --------------
ex
= ...
n!
= lim ------ = 0
ex
ln(x) 1/x
lim xln(x) = lim ------ = lim ------ = - lim x = 0
0 1/x -1/x2
lim xx = lim ex.ln(x) = elim x.ln(x)
0 0
and from previous example
= e0 = 1
lim (cos(x))1/x
0
= lim e(1/x).ln(cos(x))
0
= elim (1/x).ln(cos(x))
but lim (1/x).ln(cos(x))
0
ln(cos(x))
= lim ---------------
0 x
-sin(x)/cos(x)
= lim ---------------- = 0
0 1
So, lim (cos(x))1/x = e0 = 1
0
lim ( x ln(e + 1/x) -x )
infty
= lim x ( ln(e + 1/x) - 1)
ln(e + 1/x) - 1
= lim -----------------
1/x
-1/x2
= lim -------------------
(e + 1/x) . (-1/x2)
= 1/e
We calculate the following limit for x --> + infinity
lim x1/x
First we calculate
lim ln( x1/x ) = lim (1/x) ln(x) = lim ln(x)/x ( case infinity / infinity)
de l'Hospital
= lim 1/x = 0
The initial limit is e0 = 1
We calculate the following right limit for x --> 0
lim ( tan(x) )xFirst we calculate
lim ln ( tan(x) )x = lim x.ln(tan(x)) ( case 0. infinity )
ln (tan(x))
= lim -------------- ( case infinity / infinity)
1/x
de l'Hospital
- x2
= lim --------------------
tan(x) cos2(x)
x2
= - lim ----------
tan(x)
x
= - lim --------- . x = 1.0 = 0
tan(x)
The initial limit is e0 = 1
We calculate the following right limit for x --> 0
lim sin(x)sin(x)First we calculate
lim ln sin(x)sin(x)
= lim sin(x) ln(sin(x)) ( case 0.infinity )
ln(sin(x)
= lim ---------------- ( case infinity / infinity)
( 1/ sin(x))
de l'Hospital
( 1/ sin(x)).cos(x)
= lim -------------------------
(-1/ sin2(x)) . cos(x)
( 1/ sin(x))
= lim -----------------
(-1/ sin2(x))
= - lim sin(x) = 0
The initial limit is e0 = 1