The velocity is the derivative of distance, with respect
to time:
v = ds/dt
vdt =
ds
We'll integrate both
sides:
Int vdt = Int ds
Int
ln(t)dt/t(1-ln^4t) = s
We notice that if we'll re-write the
function, we'll have:
Int
[ln(t)/(1-ln^4t)]*(dt/t)
If we'll substitute ln t = u and
we'll differentiate, we'll get:
dt/t =
du
We'll re-write the integral, changing the
variable:
Int u
du/(1-u^4)
We'll write the ratio u/(1-u^4) as an algebraic
sum of elemntary fractions:
u/(1-u^4) =
u/(1-u)(1+u)(1+u^2)
u/(1-u)(1+u)(1+u^2) = A/(1-u) + B/(1+u)
+ (Cu+D)/(1+u^2)
We'll multiply the ratios from the right
side, so that w'ell obtain LCD.
u = A(1+u)(1+u^2) +
B(1+u^2)(1-u) + (Cu+D)(1-u^2)
u = A + Au^2 + Au + Au^3 + B
- Bu + Bu^2 - Bu^3 + Cu - Cu^3 + D - Du^2
The
correspondent coefficients from both sides have to be
equal:
u = u^3(A-B-C) + u^2(A+B-D) + u(A-B+C) +
A+B+D
A-B-C=0 (1)
A+B-D=0
(2)
A-B+C=1 (3)
A+B+D=0
(4)
We'll add (1) +
(3):
A-B-C+A-B+C=1
We'll
combine and eliminate like terms:
2A-2B=1
(5)
We'll add (2) +
(4):
A+B-D+A+B+D=0
We'll
combine and eliminate like terms:
2A+2B=0
(6)
We'll add (5)+(6):
4A =
1
A =
1/4
We'll add (1) +
(2):
A-B-C+A+B-D=0
We'll
substitute A and we'll eliminate like terms:
1/2 - C - D =
0
C+D = 1/2 (7)
We'll add (3)
+ (4):
A-B+C+A+B+D=1
We'll
substitute A and we'll eliminate like terms:
1/2 + C+D =
1
C+D = 1 - 1/2
C+D =
1/2
We'll add (2) +
(3):
A+B-D+A-B+C=1
We'll
substitute A and we'll eliminate like terms:
1/2 + C - D =
1
C - D = 1 - 1/2
C - D = 1/2
(8)
We'll add (7) + (8):
2C =
1
C =
1/2
D =
0
B =
-1/4
The integrand will
become:
u/(1-u^4) = 1/4(1-u) - 1/4(1+u) +
u/2(1+u^2)
Int udt/(1-u^4)=(1/4)Int du/(1-u) - (1/4)Int
du/(1+u)+(1/2)Int udu/(1+u^2)
Int
udt/(1-u^4)=(1/4)ln|(1-u)/(+u)| +
(1/4)ln(1+u^2)+C
The expression of distance
is:
s =
(1/4)ln|(1-lnt)/(1+lnt)| + (1/4)ln[1+(ln t)^2]+C
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