Oscillating dipoles, energy and brightness

In summary, the problem involves finding the differential equation for the rate of loss of internal energy of a dipole as it radiates power proportional to its dipole moment and angular frequency. This can be solved by using the hint that the brightness is proportional to the total power radiated by the oscillators and assuming that the internal energy of the dipole is not being replenished.
  • #1
milkism
118
15
Homework Statement
Brightness as function of time.
Relevant Equations
See solution.
Problem:
1684351520772.png

Attempt at solution:
So "energy passing through per unit area per unit time" is equal to $$I = \frac{E_i}{A t}$$
So for a the graph will be in the form of ##y=1/x##?
For b) do we have to solve the differential equation $$dI = \frac{E_i}{A dt}$$?
 
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  • #2
milkism said:
Attempt at solution:
So "energy passing through per unit area per unit time" is equal to $$I = \frac{E_i}{A t}$$
##E_i## is not the energy that should appear in the above formula. The intensity of radiation ##I## at some point of space is the flux of radiation energy at that point. But ##E_i## is not radiation energy. ##E_i## is defined in the problem as the internal energy of the ##i##th oscillator.

For this problem, use the hint that the brightness is proportional to the total power radiated by the oscillators.

Note that as a dipole radiates, the internal energy ##E_i## of the dipole is converted into radiation energy. Assume that the internal energy of the dipole is not being replenished. So, the internal energy of the dipole will decrease over time.

Try to discover the differential equation that describes the rate of loss of internal energy of a dipole. I believe you will need to know the formula for the power radiated by an oscillating electric dipole in terms of its angular frequency ##\omega## and its dipole moment ##p##.
 
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FAQ: Oscillating dipoles, energy and brightness

What is an oscillating dipole?

An oscillating dipole consists of two opposite charges or magnetic poles that oscillate back and forth. This oscillation creates a varying electric or magnetic field, which can emit electromagnetic radiation. Oscillating dipoles are fundamental in understanding the behavior of antennas, molecules, and various physical systems.

How does an oscillating dipole emit energy?

An oscillating dipole emits energy in the form of electromagnetic radiation. As the dipole oscillates, it accelerates charges, which in turn generate time-varying electric and magnetic fields. These fields propagate outward as electromagnetic waves, carrying energy away from the dipole.

What factors affect the brightness of radiation from an oscillating dipole?

The brightness of radiation from an oscillating dipole depends on several factors, including the amplitude of the oscillation, the frequency of the oscillation, and the orientation of the dipole relative to the observer. Higher amplitude and frequency generally result in more intense radiation, while the orientation affects the observed intensity due to the dipole's radiation pattern.

How is the energy radiated by an oscillating dipole related to its frequency?

The energy radiated by an oscillating dipole is proportional to the square of the frequency of oscillation. This relationship is derived from the fact that the power radiated by an accelerating charge (which constitutes the oscillating dipole) is proportional to the square of the acceleration, and the acceleration itself is proportional to the frequency of oscillation.

What is the radiation pattern of an oscillating dipole?

The radiation pattern of an oscillating dipole is typically a toroidal shape centered around the axis of oscillation. The intensity of the radiation is strongest in the plane perpendicular to the oscillation axis and drops to zero along the axis itself. This pattern is often described as a figure-eight shape in a two-dimensional cross-section.

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