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Electromagnetism}Small Oscillations


The potential is determined in the previous problem to be V=\frac{Q}{4\pi \epsilon_0 \sqrt{R^2+x^2}}. The field is given by \vec{E}=-\nabla V. Before taking derivatives, one can simplify the potential since it is given that R >> x.

Binomial expand it ((1+y)^n\approx 1+ny, for y small) to get


Taking the derivative, using the equations \vec{E}=-\nabla V, and \vec{F}=q\vec{E}, one gets,


Small oscillations have the same form as simple harmonic oscillations, i.e., \ddot{x} = -\omega^2 x. The angular frequency is \omega=\sqrt{q\frac{Q}{4\pi \epsilon_0 R^3 m}}, as in choice (A).


See below for user comments and alternate solutions! See below for user comments and alternate solutions!
Alternate Solutions
chri5tina
2006-11-27 05:11:24
It is possible to do this problem w/o the binomial expansion.

Take F = -k*x, plug in -dV/dx for F and solve for k.

Plug k into w = (k/m)^1/2 and you'll have an expression with (R^2 + x^2)^3/2 in the denominator.

At this point you can remember that R >> x and simply cancel out x as negligible, which leaves R^3 in the denominator and the correct solution.
Alternate Solution - Unverified
Comments
tinytoon
2008-11-07 14:48:10
Also, you could derive the electric field from first principles to get the answer (although very inefficient). This is, nonetheless, a valid alternative:

E = \int \frac{dq}{4\pi\epsilon_0 r^2}

We only care about the horizontal component because the force in the vertical component is zero:


E = \int \frac{dqcos\theta}{4\pi\epsilon_0 r^2}.

Using cos\theta = \frac{x}{r} = \frac{x}{\sqrt{x^2+R^2}} and r^2 = x^2+R^2, we get:

E = \frac{qx}{4\pi\epsilon_0 (x^2+R^2)^{3/2}}

and

F = \frac{qQx}{4\pi\epsilon_0 (x^2+R^2)^{3/2}} =kx

We can clearly see now that:

k = \frac{qQ}{4\pi\epsilon_0 (x^2+R^2)^{3/2}}.

We know that:

\omega = \sqrt{k/m} = \sqrt{\frac{qQ}{4\pi\epsilon_0 (x^2+R^2)^{3/2}m}}

In the limit that R>>x , this reduces to:

\omega = \sqrt{k/m} = \sqrt{\frac{qQ}{4\pi\epsilon_0 R^3m}}.

NEC
gn0m0n
2008-10-19 17:49:35
What are we expanding, exactly?NEC
dcan
2008-04-09 16:32:33
Can someone tell me why it doesn't work to use conservation of energy? Supposedly the potential energy is qV, but when I solve for \omega I'm off by a factor of 1/\sqrt{2}. NEC
Gaffer
2007-10-26 14:12:55
This problem has some particularly generous writers.

For small oscillations, I believe it is safe to say \omega must be a constant, that is not dependent upon x. This knocks off BDE. Then all you need to remember is that \omega will most likely involve a square root due to the diffEQ yosun mentioned and you have choice A, no dimensional analysis or calculation necessary.

Though of course it is always better to know why a particular formula is correct, sometimes quick and dirty is the way to go.

Oh that they were all this easy!
NEC
rmyers
2006-11-29 16:16:57
This can also be done just by dimensional analysis. Qq/(4pi(e0)R^2) has units of force = kg * m/s^2 and angular frequency is just 1/s. Only A & B are possible answers after this. From there I suppose you can just use the idea that the angular frequency usually doesn't depend on initial displacement in cases like these.
eliasds
2008-08-18 00:58:43
I believe that choice E has the same dimensions as A&B.
eliasds
2008-08-18 01:43:44
I believe that choice E has the same dimensions as A&B.
wangjj0120
2008-10-11 01:12:02
rmyers:
your comment "you can just use the idea that the angular frequency usually doesn't depend on initial displacement" is not always true. You can find the x dependence from the exact solution.
NEC
chri5tina
2006-11-27 05:11:24
It is possible to do this problem w/o the binomial expansion.

Take F = -k*x, plug in -dV/dx for F and solve for k.

Plug k into w = (k/m)^1/2 and you'll have an expression with (R^2 + x^2)^3/2 in the denominator.

At this point you can remember that R >> x and simply cancel out x as negligible, which leaves R^3 in the denominator and the correct solution.
Alternate Solution - Unverified
stiner905
2006-10-29 12:26:06
After the binomial expansion, the potential should have a "-" instead of a "+" in the expansion term. However, a minus exists in the force equation because the test charge has charge -q.NEC

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