A Solving Schwarzschild Field Equations in this Form

bolbteppa
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Applying Cartan's first and second structural equations to the vielbein forms
\begin{align}
e^t = A(r) dt , \ \ \ \ \ e^r = B(r) dr , \ \ \ \ \ e^{\theta} = C(r) d \theta , \ \ \ \ \ e^{\phi} = C(r) \sin \theta d \phi ,
\end{align}
taken from the metric
\begin{align}
ds^2 = A^2(r) dt^2 - B^2(r) dr^2 - C^2(r) d \theta^2 - C^2(r) \sin^2 (\theta) d \phi^2 , \ \ \ \ C(r) = r,
\end{align}
we end up with the Ricci curvature in the form
\begin{align}
R^t \, _t &= - \frac{1}{B^2}[\frac{A''}{A} - \frac{A'B'}{AB} + 2 \frac{A'}{Ar}] \\
R^r \, _r &= - \frac{1}{B^2}[\frac{A''}{A} - \frac{A'B'}{AB} - 2\frac{B'}{Br}] \\
R^{\theta} \, _{\theta} &= - \frac{1}{B^2}[- \frac{B'}{rB} + \frac{A'}{Ar} + \frac{1}{r^2}] + \frac{1}{r^2}= R^{\phi} \, _{\phi}.
\end{align}
This is the result in Zee's gravity, page 611, and at around 46 mins in this video (on setting ##C = r##).

My question is solving the equation
\begin{align}
R_{\mu \nu} = 0
\end{align}
with the Ricci curvature in this form to find the Schwarzschild line element, noting the curvature is a bit different from the usual form. By subtracting ##R^r \, _r## from ##R^t \, _t## we find
\begin{align}
\frac{A'}{A} + \frac{B'}{B} = 0,
\end{align}
but now using this in the ##R^{\theta} \, _{\theta}## curvature term, we get
\begin{align}
0 &= - \frac{1}{B^2}[- \frac{B'}{rB} + \frac{A'}{Ar} + \frac{1}{r^2}] + \frac{1}{r^2} \\
&= - \frac{1}{B^2}[- \frac{B'}{rB} - \frac{B'}{Br} + \frac{1}{r^2}] + \frac{1}{r^2} \\
&= - \frac{1}{B^2}[- 2 \frac{B'}{rB} + \frac{1}{r^2}] + \frac{1}{r^2} \\
&= \frac{1}{B^2}[2r \frac{B'}{B} - 1] + 1 \\
&= 2r \frac{B'}{B} - 1 + B^2 \\
&= 2rB' - B + B^3
\end{align}
which does not reduce to a total derivative (as it usually should) allowing us to solve the equations.

What has gone wrong and how does one solve the equations in this form?
 
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If all the calculations a correct, the last equation can be solved. You can separate the variables.
 
Thank you, yes this does seem to give the right solution

https://www.symbolab.com/solver/ordinary-differential-equation-calculator/2xy'-y+y^{3}=0

I was more expecting it to be literally the exact same as the method in the link (ending up with a total derivative) and didn't even think to solve it directly yet, wonder why it doesn't (perhaps need to make it an exact ode using integrating factors or something).
 
In the link that you call the usual form the equations is ##R_{\theta\theta}=0##, here you are looking at ##R^\theta_{\;\;\theta}=0##.
 
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