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Show that an electron in a one-dimensional electrical potential, \(V(x)=A x^{2},\) where the constant \(A\) is a positive real number, will execute simple harmonic motion about the origin. What is the period of that motion?

Short Answer

Expert verified
Answer: The period of the electron's simple harmonic motion is given by the expression T = 2π √(m/2A), where m is the mass of the electron and A is a positive constant.

Step by step solution

01

Derive the force experienced by the electron

The force experienced by the electron is given by the negative gradient of the potential, which is: F(x) = -dV(x)/dx = -2Ax
02

Determine the equation of motion for the electron

Now, using Newton's second law of motion, F = ma, we can write the equation of motion for the electron as: ma = -2Ax where m is the mass of the electron and a is its acceleration.
03

Show that the motion is simple harmonic

The motion will be simple harmonic if the acceleration (a) is proportional to the displacement (x) and has the opposite direction. We can rewrite the equation of motion as: a = (-2A/m)x Since A and m are constants, this equation satisfies the condition for simple harmonic motion.
04

Find the angular frequency of the motion

We can relate the angular frequency (ω) to the constants in the equation of motion as follows: ω^2 = 2A/m
05

Find the period of the motion

The period T of the motion is given by: T = 2π/ω Using the expression for ω^2 from step 4, we find: T = 2π √(m/2A) The electron undergoes simple harmonic motion with a period of T = 2π √(m/2A).

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Most popular questions from this chapter

A hollow conducting sphere of radius \(R\) is centered about the origin of an \(x y z\) -coordinate system. A total charge \(Q\) is distributed uniformly over the surface of the sphere. Assuming, as usual, that the electric potential is zero at an infinite distance, what is the electric potential at the center of the sphere? a) zero b) \(2 k Q / R\) c) \(k Q / R\) d) \(k Q / 2 R\) e) \(k Q / 4 R\)

A solid conducting sphere of radius \(R\) has a charge \(Q\) evenly distributed over its surface, producing an electric potential \(V_{0}\) at the surface. How much charge must be added to the sphere to increase the potential at the surface to \(2 V_{0} ?\) a) \(Q / 2\) b) \(Q\) c) \(2 Q\) d) \(Q^{2}\) e) \(2 Q^{2}\)

A point charge of \(+2.00 \mu \mathrm{C}\) is located at \((2.50 \mathrm{~m}, 3.20 \mathrm{~m}) .\) A second point charge of \(-3.10 \mu C\) is located at \((-2.10 \mathrm{~m}, 1.00 \mathrm{~m})\) a) What is the electric potential at the origin? b) Along a line passing through both point charges, at what point(s) is (are) the electric potential(s) equal to zero?

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What would be the consequence of setting the potential at \(+100 \mathrm{~V}\) at infinity, rather than taking it to be zero there? a) Nothing; the field and the potential would have the same values at every finite point. b) The electric potential would become infinite at every finite point, and the electric field could not be defined. c) The electric potential everywhere would be \(100 \mathrm{~V}\) higher, and the electric field would be the same. d) It would depend on the situation. For example, the potential due to a positive point charge would drop off more slowly with distance, so the magnitude of the electric field would be less.

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