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Solve for c
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mc^{2}\psi _{1}=iℏ\frac{\mathrm{d}(\psi _{1})}{\mathrm{d}t}
Swap sides so that all variable terms are on the left hand side.
c^{2}=\frac{0}{m\psi _{1}}
Dividing by m\psi _{1} undoes the multiplication by m\psi _{1}.
c^{2}=0
Divide 0 by m\psi _{1}.
c=0 c=0
Take the square root of both sides of the equation.
c=0
The equation is now solved. Solutions are the same.
mc^{2}\psi _{1}=iℏ\frac{\mathrm{d}(\psi _{1})}{\mathrm{d}t}
Swap sides so that all variable terms are on the left hand side.
mc^{2}\psi _{1}-iℏ\frac{\mathrm{d}(\psi _{1})}{\mathrm{d}t}=0
Subtract iℏ\frac{\mathrm{d}(\psi _{1})}{\mathrm{d}t} from both sides.
-iℏ\frac{\mathrm{d}(\psi _{1})}{\mathrm{d}t}+m\psi _{1}c^{2}=0
Reorder the terms.
m\psi _{1}c^{2}=0
Quadratic equations like this one, with an x^{2} term but no x term, can still be solved using the quadratic formula, \frac{-b±\sqrt{b^{2}-4ac}}{2a}, once they are put in standard form: ax^{2}+bx+c=0.
c=\frac{0±\sqrt{0^{2}}}{2m\psi _{1}}
This equation is in standard form: ax^{2}+bx+c=0. Substitute m\psi _{1} for a, 0 for b, and 0 for c in the quadratic formula, \frac{-b±\sqrt{b^{2}-4ac}}{2a}.
c=\frac{0±0}{2m\psi _{1}}
Take the square root of 0^{2}.
c=\frac{0}{2m\psi _{1}}
Multiply 2 times m\psi _{1}.
c=0
Divide 0 by 2m\psi _{1}.
mc^{2}\psi _{1}=iℏ\frac{\mathrm{d}(\psi _{1})}{\mathrm{d}t}
Swap sides so that all variable terms are on the left hand side.
\psi _{1}c^{2}m=0
The equation is in standard form.
m=0
Divide 0 by c^{2}\psi _{1}.