Deflection angle of a particle integral

Lightf
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Homework Statement



Find the deflection angle of the particle if it is scattered by this central field.

$$ U = \frac{α - β r - γ r^2}{r^2} $$


Homework Equations


Angle of deflection is given by:
$$θ = ∫ \frac{Mdr}{r^2\sqrt{2m(E-U) - \frac{M^2}{r^2}}}$$


The Attempt at a Solution



$$θ = ∫ \frac{Mdr}{r^2\sqrt{2m(E-U) - \frac{M^2}{r^2}}}$$
$$θ = ∫ \frac{Mdr}{r^2\sqrt{2m(E-\frac{α-βr-γr^2}{r^2}) - \frac{M^2}{r^2}}}$$
$$θ = ∫ \frac{Mdr}{r\sqrt{2m(Er^2 - α - βr - γr^2) - M^2}}$$
$$θ = ∫ \frac{Mdr}{r\sqrt{2m(E-γ)r^2 - 2mβr - (2mα - M^2)}}$$

I am not sure how to solve this integral.
 
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Renaming the constants, it is
\int \frac{dr}{r\sqrt{Ar^2+ Br+ C}}
Seeing that quadratic in the square root, my first thought would be to "complete the square" in the square root:
Ar^2+ Br+ C= A(x^2+ (B/A)r )+ C= A(r^2+ (B/A)r+ B^2/4A^2)- B^2/4A+ C= A(r+B/2A)^2+ C- B^2/4A
Let u= r+ B/2A so that dr= du and r= u- B/2A.

How you integrate that will depend upon whether C- B^2/4A is positive or negative.
 
How do you deal with the r outside the square root.

When you sub in u you get

$$ ∫\frac{du}{(u-\frac{B}{2A})\sqrt{Au^2 +C-\frac{B^2}{4A}}}$$

The (u- B/2A) part throws me off how to solve this. I tried doing it by integration by parts but it just made it more complex.

I am also assuming C - B^2/4A will be positive.
 
Look up Euler's substitutions.
 
Lightf said:
$$θ = ∫ \frac{Mdr}{r^2\sqrt{2m(E-\frac{α-βr-γr^2}{r^2}) - \frac{M^2}{r^2}}}$$
$$θ = ∫ \frac{Mdr}{r\sqrt{2m(Er^2 - α - βr - γr^2) - M^2}}$$
Check those signs.
 
There are two things I don't understand about this problem. First, when finding the nth root of a number, there should in theory be n solutions. However, the formula produces n+1 roots. Here is how. The first root is simply ##\left(r\right)^{\left(\frac{1}{n}\right)}##. Then you multiply this first root by n additional expressions given by the formula, as you go through k=0,1,...n-1. So you end up with n+1 roots, which cannot be correct. Let me illustrate what I mean. For this...
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