How Long Would an Electron Take to Spiral into the Nucleus?

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The discussion revolves around calculating the time it takes for an electron to spiral into a nucleus, based on classical mechanics and the Larmor formula. Participants explore whether to treat centripetal acceleration as constant or to integrate it as a function of distance from the nucleus. A key suggestion is to express energy as a function of radius and differentiate it with respect to time, noting that both speed and radius are functions of time. The conversation emphasizes the importance of correctly setting up the equations to find a valid expression for the time until the electron crashes into the nucleus. Ultimately, the participants arrive at a satisfactory solution for the problem.
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Homework Statement



Since an electron on a circular orbit around a proton has a centripetal acceleration, it should radiate energy according to the Larmor relation

\frac{dE}{dt} = -2/3(q^2/4\pi\epsilon_o)(a^2/c^3)

where q, a, \epsilon_o and c are respectively the electron charge, its acceleration, the vacuum permittivity and the velocity of light in a vacuum. Therefore, in classical, mechanics, it should spiral and crash on the nucleus. How long would this decay take, supposing that the size of the initial orbit is 10^{-10}m and the nucleus is a point charge (radius=0)?

Homework Equations



a = \frac{F_{coulombic}}{m} = \frac{v^2}{r_n} = \frac{1}{m} \frac{q^2}{4 \pi \epsilon_o r^2_n}

The Attempt at a Solution



I can easily do this if I calculate the centripital acceleration, a, out at 10^{-10}m, and treat it as constant in the Larmor relation.

My question is, do you think this is what the problem wants me to do? Or do you think I have to set up an integral somewhere to vary the acceleration with the distance from the nucleus?

I tried getting a function a(r) by integrating a with respect to r from r=0 to r=10^{-10}m, but then I realized that the integral would be infinite, since r is in the denominator. Which makes me think they want me to treat a as a constant.

Any ideas or thoughts?

Thanks!
 
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My last paragraph was really stupid. a is already a function of r. I did try to find the average acceleration by integrating from 0 to r and dividing by r. But of course the integral is infinite, and that's the problem.
 
Try this: First express E as a function of radius. Then take the derivative with respect to time and set it equal to the Larmor formula; integrate to find time.
 
Awesome! That definitely makes sense, and I wish I would have thought of it!

Thanks, Doc Al.
 
Doc Al said:
Try this: First express E as a function of radius. Then take the derivative with respect to time and set it equal to the Larmor formula; integrate to find time.

Doc Al,

But if you have E as a function of radius, and you differentiate with respect to time, you get 0, since there is no t in that function. Is this what you intended?
 
Wolf of the Ste said:
Doc Al,

But if you have E as a function of radius, and you differentiate with respect to time, you get 0, since there is no t in that function. Is this what you intended?

Your speed "v" is an implicit function of time, and r is a function of time as well.
 
Perhaps it would be helpful to note that;

v = \frac{ds}{dt} = 2\pi\cdot\frac{dr}{dt}

Edit: Dammit patrick
 
Is this the idea?

<br /> <br /> \textnormal{Let A, B, and C be the product of the constants in the functions E, a, and dE/dt respectively. Then,} \\<br />

<br /> E = \frac{-A}{r} \ \textnormal{(1)}\\<br />

<br /> a = \frac{B}{r^2} \ \textnormal{(2)}\\<br />

<br /> \frac{dE}{dt} = C a^2 = \frac{C B^2}{r^4}\ \textnormal{(3)} \ \textnormal{(Lamar Relation)} \\<br />

<br /> \textnormal{Then, using (1)}, \\<br />

<br /> \frac{dE}{dt} = \frac{A}{r^2} \frac{dr}{dt} \textnormal{(4)} \\<br />

<br /> \textnormal{Setting (3) and (4) equal, we get:} \\<br />

<br /> \frac{A}{r^2} \frac{dr}{dt} = \frac{C B^2}{r^4} \\<br />

<br /> A r^2 dr = C B^2 dt \\<br />

<br /> \int{A r^2}dr = \int{C B^2}dt \\<br />

<br /> \frac{A}{3} r^3 = C B^2 t \\<br />

<br /> t = \frac{A r^3}{3C B^2} \\<br />So is this a valid expression for time t needed for the electron to crash into the point nucleus, given an initial distance, r, from the point nucleus??

Thanks.
 
Last edited:
Wolf of the Ste said:
Doc Al,

But if you have E as a function of radius, and you differentiate with respect to time, you get 0, since there is no t in that function. Is this what you intended?
Since the electron is crashing into the nucleus, r must be a function of time and thus E is a function of time (as noted by nrqed and Hoot). If
E = E(r)

Then
dE/dt = E&#039;(r) dr/dt

Start by finding E(r) explicitly, where E is the total energy. (Use the Bohr model.)


Wolf of the Ste said:
Is this the idea?

...
Exactly!
 
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Thanks again. I'm finished, at last! :)
 
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