Completing the Square Homework Statement

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SUMMARY

The discussion focuses on simplifying the potential energy of a charged particle in a harmonic oscillator under an external electric field using the method of completing the square. The potential is given by V(x) = 1/2 mw²x² - qεx. By completing the square, the potential can be rewritten as V(x) = (√(1/2 mw²)x - qε/√(2mw²))² - q²ε²/2mw², effectively transforming the problem into one involving only a harmonic oscillator potential. This method allows for a clearer understanding of the particle's behavior in the presence of both the harmonic potential and the electric field.

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  • Understanding of harmonic oscillator potential
  • Familiarity with completing the square in quadratic equations
  • Knowledge of electric fields and their effects on charged particles
  • Basic grasp of classical mechanics concepts
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  • Study the derivation of the harmonic oscillator potential in classical mechanics
  • Learn advanced techniques for completing the square in various contexts
  • Explore the effects of external electric fields on charged particles
  • Investigate the applications of harmonic oscillators in quantum mechanics
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Homework Statement



Consider a charged particle of mass m in a harmonic potential and in the presence also of an
external electric field E = E\hat{i}. The potential for this problem is simply

V(x) = 1/2 mw^{2}x^{2} - qεx

where q is the charge of the particle.

1) Show that a simple change of variables turns this problem into one of a particle under
only a harmonic oscillator potential. (Hint: Complete the square.)

Homework Equations



(ax-b)^{2} = a^{2}x^{2} - 2abx + b^{2}

The Attempt at a Solution



So I know the way to simplify the potential is by completing the square. I only know the way of completing the square when a quadratic equation is equal to 0 but in this case it's a function. So with that formula for (ax-b)^{2} I believe 1/2 mw^{2} is a^{2} and -2ab is -qε but I'm unsure.

So what I got was that b = qε/(2mw^{2}) so the equation is

V(x) = 1/2 mw^{2}x^{2} - qεx + q^{2}ε^{2}/2mw^{2} - q^{2}ε^{2}/2mw^{2} = (\sqrt{1/2 mw^{2}}x - qε/\sqrt{2mw^2})^2 - q^{2}ε^{2}/2mw^{2}
 
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denjay said:

Homework Statement



Consider a charged particle of mass m in a harmonic potential and in the presence also of an
external electric field E = E\hat{i}. The potential for this problem is simply

V(x) = 1/2 mw^{2}x^{2} - qεx

where q is the charge of the particle.

1) Show that a simple change of variables turns this problem into one of a particle under
only a harmonic oscillator potential. (Hint: Complete the square.)

Homework Equations



(ax-b)^{2} = a^{2}x^{2} - 2abx + b^{2}

The Attempt at a Solution



So I know the way to simplify the potential is by completing the square. I only know the way of completing the square when a quadratic equation is equal to 0 but in this case it's a function. So with that formula for (ax-b)^{2} I believe 1/2 mw^{2} is a^{2} and -2ab is -qε but I'm unsure.

You don't have to have an equation. Here's an example, complete the square on: ##2x^2-12x##. You factor out the ##2## getting ##2(x^2-6x)##. Now inside the parentheses you need a ##9## so add it and subtract it: ##2(x^2-6x + 9 - 9)## which is the same as ##2(x-3)^2 - 18##. Try something like that.
 
Cool yeah, I did it the way you suggested and got the same answer as I did in my original post. Thanks!
 

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