Dipole Radiation Homework: Amplitude & Direction at P2, Total Power

In summary, the problem involves an electric dipole located at the origin of a coordinate system, which creates an electromagnetic wave with a given frequency and amplitude. At point P1, the intensity of the wave is zero, while at point P2, the radiation is a plane monochromatic wave. To find the amplitude and direction of oscillation of E and B at P2, you can use the direction of the Poynting vector and the formula for the amplitude of E and B. The total power radiated by the dipole can be found using the formula for total power emitted.
  • #1
Josephk1508
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Homework Statement



Given a Electric dipole located at the origin of the coordinate system, which oscillates with a given frequency and amplitude, creating an electromagnetic wave. It is found that no power can be detected at point P1 = (3 y) m (i.e. the intensity of the wave at that point is zero). Another measurement is made at the point P2 = (1 x) m where it is found that the radiation is locally a plane monochromatic wave.

Homework Equations



Poynting's vector is <S> = 2.5 x J/m^2s

The Attempt at a Solution



I solved the first part but stuck when it asks me Find the amplitude and direction of oscillation of E and B at P2? And the total power radiated by the dipole? The total power emitted is calculated by using the flux of <S> crossing a spherical surface radius r, but still finding it tricky.
 
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  • #2


Thank you for your post. It seems like you have made some progress in solving the first part of the problem. To find the amplitude and direction of oscillation of E and B at P2, you can use the fact that the radiation at this point is a plane monochromatic wave. This means that the electric and magnetic fields at this point are perpendicular to each other and the direction of propagation. The direction of propagation can be found using the direction of the Poynting vector, which is given as <S> = 2.5 x J/m^2s. This means that the direction of propagation is in the positive x-direction.

To find the amplitude of the fields, you can use the relationship between the Poynting vector and the amplitude of E and B, given by <S> = 1/2 * c * ε0 * E0^2. Here, c is the speed of light and ε0 is the permittivity of free space. You know the value of <S>, so you can solve for E0. Since the radiation is a plane monochromatic wave, the amplitude of E and B will be the same, so you can use this value for both.

Once you have found the amplitude and direction of E and B, you can use the formula for the total power emitted by the dipole, given by P = 1/2 * ε0 * c * E0^2 * A, where A is the surface area of the sphere with radius r. You can use this formula to find the total power radiated by the dipole.

I hope this helps you solve the rest of the problem. Good luck!
 

1. What is dipole radiation and how does it relate to amplitude and direction at P2?

Dipole radiation refers to the electromagnetic radiation emitted by an oscillating electric dipole. The amplitude and direction at P2 refer to the strength and direction of this radiation at a specific point in space, which is typically located at a distance of two wavelengths from the dipole.

2. What factors affect the amplitude and direction of dipole radiation at P2?

The amplitude and direction of dipole radiation at P2 are affected by several factors, including the frequency of the oscillating dipole, the orientation of the dipole, and the distance between the dipole and P2. Additionally, the medium through which the radiation travels can also impact its amplitude and direction.

3. How is total power calculated for dipole radiation at P2?

Total power is calculated by multiplying the amplitude squared by the radiation resistance of the dipole. The radiation resistance takes into account the efficiency of the dipole in converting electrical energy into radiation. Additionally, the total power is also affected by the direction of the dipole and its distance from P2.

4. What is the significance of understanding amplitude and direction at P2 in dipole radiation?

Understanding the amplitude and direction at P2 is important for several reasons. It allows us to accurately measure and predict the strength and direction of dipole radiation, which is crucial for various applications in communication, radar, and astronomy. Additionally, it helps us better understand the behavior of electromagnetic waves and their interactions with different mediums.

5. How can the amplitude and direction at P2 be manipulated for specific purposes?

The amplitude and direction at P2 can be manipulated by changing the orientation of the dipole, adjusting the frequency of oscillation, and altering the medium through which the radiation travels. This manipulation can be used for various purposes, such as increasing the range of communication signals, improving the resolution of radar systems, and studying the properties of different materials through electromagnetic waves.

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