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Solve for c_1
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T^{2}c_{2}r\left(k-r\right)T-kc_{1}=0
Multiply both sides of the equation by kT^{2}, the least common multiple of k,T^{2}.
T^{3}c_{2}r\left(k-r\right)-kc_{1}=0
To multiply powers of the same base, add their exponents. Add 2 and 1 to get 3.
T^{3}c_{2}rk-T^{3}c_{2}r^{2}-kc_{1}=0
Use the distributive property to multiply T^{3}c_{2}r by k-r.
-T^{3}c_{2}r^{2}-kc_{1}=-T^{3}c_{2}rk
Subtract T^{3}c_{2}rk from both sides. Anything subtracted from zero gives its negation.
-kc_{1}=-T^{3}c_{2}rk+T^{3}c_{2}r^{2}
Add T^{3}c_{2}r^{2} to both sides.
-c_{1}k=c_{2}r^{2}T^{3}-c_{2}krT^{3}
Reorder the terms.
\left(-k\right)c_{1}=c_{2}r^{2}T^{3}-c_{2}krT^{3}
The equation is in standard form.
\frac{\left(-k\right)c_{1}}{-k}=\frac{c_{2}r\left(r-k\right)T^{3}}{-k}
Divide both sides by -k.
c_{1}=\frac{c_{2}r\left(r-k\right)T^{3}}{-k}
Dividing by -k undoes the multiplication by -k.
c_{1}=-\frac{c_{2}r\left(r-k\right)T^{3}}{k}
Divide c_{2}r\left(r-k\right)T^{3} by -k.