Field transformation laws - Relativity

In summary, two field-measuring devices are used to measure the electric and magnetic fields of a 1 Coulomb charge Q. One device is stationary at (0,1,0) while the other is moving at high speed along the line y = 1. The components of the electric and magnetic field vectors measured by the stationary device can be calculated using the electric field equation and the Biot-Savart law. The Lorentz transformation equations and the EM strength tensor can be used to calculate the components of the fields measured by the moving device. The distance between the charge Q and the moving device can also be calculated using the Lorentz transformation equations and the time at which the photograph was taken.
  • #1
erisedk
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Homework Statement


The electric and magnetic fields of a 1 Coulomb charge Q are measured by a pair of field measuring instruments. From the perspective of observers in frame O, the charge is at rest at the origin and one of the field-measuring devices is also at rest, with position (x,y,z) = (0,1,0). Observers in O see the second field-measuring device moving at high speed, with velocity v = βc (x direction) (it travels along the line y = 1)

(a) At time t = 0 this device passes very close to the stationary device at (x,y,z) = (0,1,0). The readings on the dials of the moving device were photographed by observers in O as it was illuminated by the lights from the stationary device's panel lights.

1. Calculate the components of the electric and magnetic field vectors measured by the stationary device at the time the photograph was taken.

2. Calculate the components of the electric and magnetic field vectors measured by the moving device.

3. According to observers in the rest frame of the moving device, how far away is the charge Q?

Homework Equations



The Attempt at a Solution


1. Electric field vector at stationary device = kQ/r2 (j) = (9 × 109 × 1)/12 = 9 × 109 V/m

Magnetic field vector at stationary device = 0 because there is no relative motion between the point charge and the stationary device.

2. I don't understand how to do this at all. We're supposed to used this large matrix (EM strength tensor) I think, but I don't really understand how to do that.

If I were to do it without relativity, I'd just treat Q as a line of charge (or a current carrying wire) and solve, but that's definitely wrong.

3. Wouldn't it keep changing as a function of time?
d = ##\sqrt{1^2 + v^2t^2} ## where v = βc

Please help.
 
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  • #2


1. Your calculation for the electric field vector at the stationary device is correct. However, the magnetic field vector is not necessarily zero. Since the charge Q is moving, there will be a magnetic field at the location of the stationary device. The magnetic field vector can be calculated using the Biot-Savart law.

2. To calculate the components of the electric and magnetic field vectors measured by the moving device, you will need to use the Lorentz transformation equations. These equations relate the measurements made in one frame of reference (in this case, frame O) to the measurements made in a different frame of reference (the frame of the moving device). The EM strength tensor you mentioned is a mathematical tool that is used to represent the electric and magnetic fields in relativity. You can use this tensor to calculate the components of the fields in the moving frame of reference.

3. Yes, the distance between the charge Q and the moving device will change as a function of time. However, the distance at the time the photograph was taken can be calculated using the Lorentz transformation equations. You can use the distance formula you mentioned, but you will need to use the velocity in the x direction (βc) and the time at which the photograph was taken.
 

1. How do the field transformation laws in relativity affect our understanding of space and time?

The field transformation laws in relativity are a set of equations that describe how physical quantities, such as space and time, change when observed from different reference frames. They show that space and time are not absolute, but rather relative to the observer's frame of reference. This means that different observers can measure different values for space and time intervals, depending on their relative motion.

2. What is the significance of the Lorentz transformation in the field transformation laws of relativity?

The Lorentz transformation is a set of equations that describe how space and time intervals change when observed from different inertial frames of reference. It is a fundamental part of the field transformation laws of relativity and is crucial in understanding the effects of time dilation and length contraction.

3. How do the field transformation laws in relativity impact our understanding of the speed of light?

The field transformation laws in relativity state that the speed of light in a vacuum is constant and is the same for all observers, regardless of their relative motion. This concept, known as the speed of light postulate, is a fundamental principle of relativity and has far-reaching implications for our understanding of space and time.

4. Can the field transformation laws in relativity be applied to all types of fields, or are they limited to certain types of fields?

The field transformation laws in relativity can be applied to all types of fields, including electromagnetic fields, gravitational fields, and quantum fields. They provide a framework for understanding how these fields behave and interact in different reference frames, allowing for a more comprehensive understanding of the universe.

5. How do the field transformation laws in relativity relate to Einstein's famous equation, E=mc^2?

The field transformation laws in relativity are closely related to Einstein's famous equation, E=mc^2. This equation describes the relationship between energy, mass, and the speed of light, and is a direct consequence of the field transformation laws. It shows that energy and mass are equivalent and can be converted into one another, providing a deeper understanding of the fundamental nature of the universe.

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