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An electron is released from rest and falls under the influence of gravity. In the first centimeter, what fraction of the potential energy lost is radiated away?

Short Answer

Expert verified

The fraction of the potential energy lost is 2.76×10-22.

Step by step solution

01

Expression for a fraction of the potential energy lost:

Write the fraction of the potential energy lost is radiated.

f=UradUpotential …… (1)

Here,Urad is the radiated energy andUpotential is the potential energy.

02

Determine the dipole moment:

Write the expression for the radiated energy.

Urad=P×t …… (2)

Here, P is the power, and t is the time.

Let the distance travelled by the electron be y, and its initial velocity be uu=0.

If an electron travels a distance y in a time t, express the required equation.

y=12gt2t=2yg

Here, g is the gravitational acceleration.

Write the expression for the total radiated power.

P=μ06πcp¨t2 …… (3)

Here, p is the dipole moment which is given as:

p=-eyy^y=-pey^12gt2=-pey^p=-12get2y^.......(4)

03

Determine the radiated energy:

Take the double differentiation of equation (4).

p=-12ge2ty^p¨=-gey^p¨t=ge

Substitutep¨t=ge in equation (3).

P=μ06πcge2

Substitute P=μ06πcge2and t=2ygin equation (2).

Urad=μ06πcge2×2ygUrad=μ0ge26πc2yg

04

Determine the fraction of the potential energy lost:

Write the expression for the loss in potential energy of an electron falling a distance.

Upotential=mgy

SubstituteUrad=μ0ge26πc2yg andUpotential=mgy in equation (1).

f=μ0ge26πc2ygmgyf=μ0g2e26πcmg2ygf=μ0e26πcm2gy

Here, m is the mass of an electron m=9.11×10-31kg.

Substitute μ0=4π×10-7H/m,e=1.6×10-19C,c=3×108m/s,m=9.11×10-31kg,g=9.81m/s2andy=1cm in the above expression.

f=4π×10-7H/m1.6×10-19C26π3×108m/s9.11×10-31kg29.81m/s21cm×10-2m1cmf=2.76×10-22

Therefore, the fraction of the potential energy lost is2.76×10-22 .

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Most popular questions from this chapter

A point charge q, of mass m, is attached to a spring of constant k.Y2<<Ó¬0Attimet=0it is given a kick, so its initial energy is U0=12mv02. Now it oscillates, gradually radiating away this energy.

(a) Confirm that the total energy radiated is equal to U0. Assume the radiation damping is small, so you can write the equation of motion as and the solution as

role="math" localid="1658840767865" x+y+x+Ó¬02x=0,

and the solution as

x(t)=v0Ó¬0e-yt/2sin(Ó¬0t)

with Ӭ0≡k/m,Y=Ӭ02T, and Y2<<Ӭ0 (drop Y2in comparison to Ӭ02, and when you average over a complete cycle, ignore the change in e-yτ).

(b) Suppose now we have two such oscillators, and we start them off with identical kicks. Regardless of their relative positions and orientations, the total energy radiated must be 2U0. But what if they are right on top of each other, so it's equivalent to a single oscillator with twice the charge; the Larmor formula says that the power radiated is four times as great, suggesting that the total will be 4U0. Find the error in this reasoning, and show that the total is actually2U0, as it should be.

In Bohr’s theory of hydrogen, the electron in its ground state was supposed to travel in a circle of radius 5×10-11m, held in orbit by the Coulomb attraction of the proton. According to classical electrodynamics, this electron should radiate, and hence spiral in to the nucleus. Show thatv≪c for most of the trip (so you can use the Larmor formula), and calculate the lifespan of Bohr’s atom. (Assume each revolution is essentially circular.)

An electric dipole rotates at constant angular velocity Ӭin thexy plane. (The charges,±q , are at r±=±R(cosӬtx^+sinӬty^); the magnitude of the dipole moment is p=2qR.)

(a) Find the interaction term in the self-torque (analogous to Eq. 11.99). Assume the motion is nonrelativistic ( Ó¬R<<c).

(b) Use the method of Prob. 11.20(a) to obtain the total radiation reaction torque on this system. [answer: -μ0p2Ó¬36Ï€³¦z^]

(c) Check that this result is consistent with the power radiated (Eq. 11.60).

Apply Eqs. 11.59 and 11.60 to the rotating dipole of Prob. 11.4. Explain any apparent discrepancies with your previous answer

A positive charge q is fired head-on at a distant positive charge Q (which is held stationary), with an initial velocityv0 . It comes in, decelerates to v=0, and returns out to infinity. What fraction of its initial energy(12mv02) is radiated away? Assume v0≪c, and that you can safely ignore the effect of radiative losses on the motion of the particle. [ Answer (1645)(qQ)(v0c)3. ]

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