How to solve for an unknown in two different denominators?
In this equation: $$F = \frac{GMm_3}{r_2} - \frac{Gmm_3}{d-r_2}.$$
Everything is given except for $r_2$. How do I solve for $r_2$? Is it possible?
How to solve for an unknown in two different denominators?
In this equation: $$F = \frac{GMm_3}{r_2} - \frac{Gmm_3}{d-r_2}.$$
Everything is given except for $r_2$. How do I solve for $r_2$? Is it possible?
On
Try multiplying each side by both denominators, i.e. both $r_2$ and $d-r_2$, so that there are no fractions left. Combine like terms - in other words, group the terms with $r_2^2$ in them, the terms with $r_2$ in them, and the terms with no $r_2$'s in them. Then, treating $r_2$ as a variable we are solving for, we can apply the quadratic formula.
On
You can, but you will probably use the quadratic formula.
$$f = \frac{GMm_3}{r_2} - \frac{Gmm_3}{d-r_2}.$$
$$f \cdot (r_2)(d-r_2) = GMm_3 \cdot (d-r_2) - Gmm_3 \cdot r_2$$
$$ -f \cdot r_2^2 + (fd + GMm_3 + Gmm_3) \cdot r_2 - GMm_3 d = 0$$
And this is quadratic in $r_2$, so solve using the quadratic formula. Aha - just as I am ready to post, this tells me that Zev has posted a similar answer. Well, this is his, except Texed up.
On
A brief plea for symmetry!
The problem probably came from a situation in which there are two distances, $r_1$ and $r_2$, whose sum is $d$. It could make life easier to use $r_1$ instead of $d-r_2$. We then need to specify additionally that $r_1+r_2=d$.
So instead of a single equation, we have a system of two equations. But there is much more symmetry. Calculations often are more pleasant, and the calculation is more likely to reveal structural information.
First, rewrite the right hand side as a single fraction by adding the fractions; factoring out $Gm_3$ simplifies matters a bit: $$\begin{align*} f &= \frac{GMm_3}{r_2} - \frac{Gmm_3}{d-r_2}\\ &= Gm_3\left(\frac{M}{r_2} - \frac{m}{d-r_2}\right)\\ &= Gm_3\left(\frac{M(d-r_2) - mr_2}{r_2(d-r_2)}\right). \end{align*}$$ Then clear denominators by cross multiplying, and collect appropriate powers of $r_2$; you'll end up with a quadratic equation in $r_2$ that can be solved using the quadratic formula or other methods: $$\begin{align*} f & = Gm_3\left(\frac{Md - (M+m)r_2}{r_2(d-r_2)}\right)\\ fr_2(d-r_2) &= Gm_3\left(Md - (M+m)r_2\right)\\ fdr_2 - f(r_2)^2 &= Gm_3Md - Gm_3(M+m)r_2\\ 0&= GMm_3d - \Bigl(Gm_3(M+m)+fd\Bigr)r_2 + f(r_2)^2. \end{align*}$$
Added. If $f=0$, as you now write, then the equation becomes $$0 = Gm_3\left(\frac {Md - (M+m)r_2}{r_2(d-r_2)}\right).$$ If $G\neq 0$ and $m_3\neq 0$, then this holds if and only if the numerator is $0$, if and only if $$0 = Md - (M+m)r_2,$$ which is easy to solve.
If, as Ross suggests, the denominators should be squared and $f=0$, then you would instead get $$0 = M(d-r_2)^2 - m{r_2}^2$$ which yields a quadratic equation in $r_2$ again, namely $$(M-m){r_2}^2 - 2Mdr_2 + Md^2 = 0.$$