I was given this formula at the end of Astrophysics lecture today. It was so helpful to see the derivation and explanation (I'm an Advanced Chemistry major, not physics). Thank you!
HitAndMissLab, you are right that this formula is expressedly non-relativistic. In the relativistic form, there is a "beaming" effect. Because of relativistic length contraction, radiation is preferentially emitted parallel to the axis of motion, Rather than perpendicular. Moreover, the Doppler shifting of photons makes emission in the forward direction more energetic than in the reverse direction.
Feynman felt it was wrong (as did Pauli) From the 'Feynman lectures on Gravitation' Lecture 9, P123 Larmor equation (9.1.1) This is usually derived from calculating the flow from Poynting's theorem far away, and it is only valid for cyclic motions, or at least motions which do not grow forever in time (as a constant acceleration does). It does not suffice to tell us "when" the energy is radiated. This can only be determined by finding the force of radiation resistance, ... Feynman's version had P ~ da/dt v, rather than a^2; which avoids the paradox 'does a charge on a table radiate, as it is equivalent to an accelerating charge'
Hellou! awesome video and perfect explanation! I'm trying to find/understand a way of determining the frequency of the EM wave generate by the accelerated charge, considering that one knows the aspects of that acceleration. Have you any idea of how to do so? Maybe the lenght of that ring (ct) have that information?
But the outer and inner shell are not strictly concentric. If delta-v is large, say, 0.5*c, than there will be an offset +/- (delta-v * delta-t). Since we are talking particles here, that is realistic assumption. How would that change the outcome?
Problem with this formula: A charge oscillating in a sinusoidal way, at the location farthest from the equilibrium position its acceleration is maximum, yet P=Fv must be zero since v=0. How can it be radiating energy at this moment when it's not absorbing energy to radiate? Please resolve.
@ 17:51 By pulling the plates of a capacitor apart you transfer energy to the plates, NOT to the field. In W = F . dx, dx is the displacement of the plates. So where is the field-energy? P.S. "In the end nothing is moving" (18:08). But you just said you moved the plates!
I was given this formula at the end of Astrophysics lecture today. It was so helpful to see the derivation and explanation (I'm an Advanced Chemistry major, not physics). Thank you!
HitAndMissLab, you are right that this formula is expressedly non-relativistic. In the relativistic form, there is a "beaming" effect. Because of relativistic length contraction, radiation is preferentially emitted parallel to the axis of motion,
Rather than perpendicular. Moreover, the Doppler shifting of photons makes emission in the forward direction more energetic than in the reverse direction.
+Aaron Parsons thank you sir
Feynman felt it was wrong (as did Pauli)
From the 'Feynman lectures on Gravitation'
Lecture 9, P123
Larmor equation (9.1.1)
This is usually derived from calculating the flow from Poynting's theorem far away, and it is only valid for cyclic motions, or at least motions which do not grow forever in time (as a constant acceleration does). It does not suffice to tell us "when" the energy is radiated. This can only be determined by finding the force of radiation resistance, ...
Feynman's version had P ~ da/dt v, rather than a^2; which avoids the paradox 'does a charge on a table radiate, as it is equivalent to an accelerating charge'
hi very nice presentation In r direction there not radiation?
Hellou! awesome video and perfect explanation! I'm trying to find/understand a way of determining the frequency of the EM wave generate by the accelerated charge, considering that one knows the aspects of that acceleration. Have you any idea of how to do so? Maybe the lenght of that ring (ct) have that information?
Larmor derive it in 1897 i can't imagine !!!
But the outer and inner shell are not strictly concentric. If delta-v is large, say, 0.5*c, than there will be an offset +/- (delta-v * delta-t). Since we are talking particles here, that is realistic assumption.
How would that change the outcome?
Problem with this formula: A charge oscillating in a sinusoidal way, at the location farthest from the equilibrium position its acceleration is maximum, yet P=Fv must be zero since v=0. How can it be radiating energy at this moment when it's not absorbing energy to radiate? Please resolve.
How will the electric field act in case of a charge moving with a constant velocity?
If the charge moves, then the qv component is nonzero, and the resultant force changes.
you cannot determine if you are in an elevated ground within the "ether", if the ether is itself elevated
@ 17:51 By pulling the plates of a capacitor apart you transfer energy to the plates, NOT to the field. In W = F . dx, dx is the displacement of the plates. So where is the field-energy? P.S. "In the end nothing is moving" (18:08). But you just said you moved the plates!