v = v²(A + B) + v∙(a∙A - a∙B + C) + 1∙(a²∙A - a∙C)
Compare coefficients of same powers of v and find
A + B = 0
a∙A - a∙B + C = 1
a²∙A - a∙C = 0
Solution to this equation system is
A = 1/(3∙a)
B = -1/(3∙a)
C = 1/3
=>
(1/6) ∙ ∫ v/(v³ - (1/6)) dv
= a³ ∙ ∫ v/(v³ - a³) dv
= a³ ∙ ∫ [1/(3∙a)]/(v - a) - ([1/(3∙a)]∙v - [1/3])/(v² + a∙v + a²) dv
= (a²/3) ∙ ∫ 1/(v - a) - (v - a)/(v² + a∙v + a²) dv
= (a²/3) ∙ [ ∫ 1/(v - a) dv - ∫ (v - a)/(v² + a∙v + a²) dv ]
= (a²/3) ∙ [ ln(v - a) - ∫ (v - a)/(v² + a∙v + a²) dv ]
To solve the remaining integral use quadratic supplement to bring you denominator to the form z² + 1. By appropriate substitution you get two integrals of the from:
∫ z/(z² + 1) dz = (1/2)∙ln(z² +1)
and
∫ 1/(z² + 1) dz = tan⁻¹(z)
∫ (v - a)/(v² + a∙v + a²) dv
= ∫ (v - a)/( v² + a∙v + (1/4)∙a² + (3/4)∙a²) dv
= ∫ (v - a)/( (v + (1/2)∙a)² + (3/4)∙a² ) dv
= (4/(3∙a²) ∙ ∫ (v - a)/( [(2/√3)∙(v + (1/2)∙a)/a]² + 1 ) dv
= (4/(3∙a²) ∙ ∫ (v - a)/( [(2∙(v/a) + 1)/√3]² + 1 ) dv
let
z = [(2∙(v/a) + 1)/√3]
<=>
v = (z∙√3 - 1)∙(a/2)
=>
dv = (a∙√3)/2 dz
(4/(3∙a²) ∙ ∫ (v - a) / ( [(2∙(v/a) + 1)/√3]² + 1 ) dv
Answers & Comments
Verified answer
∫ v/(6v³ - 1) dv
= (1/6) ∙ ∫ v/(v³ - (1/6)) dv
You can solve by expanding to partial fractions.
First factorize denominator.
one root is at
v = (∛(1/6)
To improve readability i use symbol a=∛(1/6) in the following
By long division i find
(v³ - a³) / (v - a) = v² + a∙v + a²
<=>
(v³ - a³) = (v - a)∙(v² + a∙v + a²)
Hence you can decompose as follows
v/(v³ - a³) = A/(v - a) + (B∙v + C)/(v² + a∙v + a²)
<=>
v = A∙(v² + a∙v + a²) + B∙v∙(v - a) + C∙(v - a)
<=>
v = v²(A + B) + v∙(a∙A - a∙B + C) + 1∙(a²∙A - a∙C)
Compare coefficients of same powers of v and find
A + B = 0
a∙A - a∙B + C = 1
a²∙A - a∙C = 0
Solution to this equation system is
A = 1/(3∙a)
B = -1/(3∙a)
C = 1/3
=>
(1/6) ∙ ∫ v/(v³ - (1/6)) dv
= a³ ∙ ∫ v/(v³ - a³) dv
= a³ ∙ ∫ [1/(3∙a)]/(v - a) - ([1/(3∙a)]∙v - [1/3])/(v² + a∙v + a²) dv
= (a²/3) ∙ ∫ 1/(v - a) - (v - a)/(v² + a∙v + a²) dv
= (a²/3) ∙ [ ∫ 1/(v - a) dv - ∫ (v - a)/(v² + a∙v + a²) dv ]
= (a²/3) ∙ [ ln(v - a) - ∫ (v - a)/(v² + a∙v + a²) dv ]
To solve the remaining integral use quadratic supplement to bring you denominator to the form z² + 1. By appropriate substitution you get two integrals of the from:
∫ z/(z² + 1) dz = (1/2)∙ln(z² +1)
and
∫ 1/(z² + 1) dz = tan⁻¹(z)
∫ (v - a)/(v² + a∙v + a²) dv
= ∫ (v - a)/( v² + a∙v + (1/4)∙a² + (3/4)∙a²) dv
= ∫ (v - a)/( (v + (1/2)∙a)² + (3/4)∙a² ) dv
= (4/(3∙a²) ∙ ∫ (v - a)/( [(2/√3)∙(v + (1/2)∙a)/a]² + 1 ) dv
= (4/(3∙a²) ∙ ∫ (v - a)/( [(2∙(v/a) + 1)/√3]² + 1 ) dv
let
z = [(2∙(v/a) + 1)/√3]
<=>
v = (z∙√3 - 1)∙(a/2)
=>
dv = (a∙√3)/2 dz
(4/(3∙a²) ∙ ∫ (v - a) / ( [(2∙(v/a) + 1)/√3]² + 1 ) dv
= (2/(a∙√3) ∙ ∫ ((z∙√3 - 1)∙(a/2) - a ) / ( z² + 1 ) dz
= (2/(a∙√3) ∙ ∫ ( z∙√3∙(a/2) - (3/2)∙a ) / ( z² + 1 ) dz
= ∫ z/(z² + ) - √3/(z² + 1) dz
= ∫ z/(z² + ) - √3/(z² + 1) dz
= (1/2)∙ln(z² +1) - √3∙tan⁻¹(z)
substitute back
z = [(2∙(v/a) + 1)/√3]
z² + 1 = v² + a∙v + a²
(1/2)∙ln(z² +1) - √3∙tan⁻¹(z)
= (1/2)∙ln(v² + a∙v + a²) - √3∙tan⁻¹((2∙(v/a) + 1)/√3)
Summary:
∫ v/(6v³ - 1) dv
= a³ ∙ ∫ v/(v³ - a³) dv
= (a²/3) ∙ { ln(v - a) - (1/2)∙ln(v² + a∙v + a²) + √3∙tan⁻¹((2∙(v/a) + 1)/√3) }
= { ln(v - ∛(1/6)) - (1/2)∙ln(v² + ∛(1/6)∙v + ∛(1/36)) + √3∙tan⁻¹((2∙∛6∙v + 1)/√3) } / (3∙∛6)