The amplitude of the magnetic field of a harmonic electromagnetic wave in vacuum is \( B_0 = 610 \) nT. The amplitude of the electric field of the wave is:
\( 183 \, NC^{-1} \)
An electromagnetic wave, or EM wave, is a form of energy that travels through space or through a medium in the form of waves. These waves consist of oscillating electric and magnetic fields that are perpendicular to each other and to the direction of propagation.
In a vacuum, electromagnetic waves travel at a constant speed, which is the speed of light, denoted by \(c\). There is a fundamental relationship between the amplitudes of the electric field (\(E_0\)) and the magnetic field (\(B_0\)) of a harmonic electromagnetic wave in a vacuum. This relationship is given by the equation:
\( c = \frac{E_0}{B_0} \)
Where:
The question provides the amplitude of the magnetic field (\(B_0\)) and asks for the amplitude of the electric field (\(E_0\)). We can rearrange the formula to solve for \(E_0\):
\( E_0 = c \times B_0 \)
We are given:
First, we need to convert the magnetic field amplitude from nanotesla (nT) to Tesla (T). The conversion is \( 1 \, \text{nT} = 10^{-9} \, \text{T} \).
\( B_0 = 610 \, \text{nT} = 610 \times 10^{-9} \, \text{T} \)
Now we can substitute the values of \(c\) and \(B_0\) into the rearranged formula:
\( E_0 = (3 \times 10^8 \, \text{m/s}) \times (610 \times 10^{-9} \, \text{T}) \)
Let's perform the multiplication:
\( E_0 = 3 \times 610 \times 10^8 \times 10^{-9} \, \frac{\text{m}}{\text{s}} \cdot \text{T} \)
\( E_0 = 1830 \times 10^{8 - 9} \, \frac{\text{m}}{\text{s}} \cdot \text{T} \)
\( E_0 = 1830 \times 10^{-1} \, \frac{\text{m}}{\text{s}} \cdot \text{T} \)
\( E_0 = 183 \, \frac{\text{m}}{\text{s}} \cdot \text{T} \)
The units for electric field amplitude are typically Newtons per Coulomb (N/C) or Volts per meter (V/m). Let's check if the units match:
Recall that \( 1 \, \text{T} = 1 \, \frac{\text{N}}{\text{A} \cdot \text{m}} \) and \( 1 \, \text{A} = 1 \, \frac{\text{C}}{\text{s}} \). So, \( 1 \, \text{T} = 1 \, \frac{\text{N}}{(\text{C/s}) \cdot \text{m}} = 1 \, \frac{\text{N} \cdot \text{s}}{\text{C} \cdot \text{m}} \).
Now, let's look at the combined units from our calculation:
\( \frac{\text{m}}{\text{s}} \cdot \text{T} = \frac{\text{m}}{\text{s}} \cdot \frac{\text{N} \cdot \text{s}}{\text{C} \cdot \text{m}} \)
The 'm' and 's' units cancel out:
\( \frac{\cancel{\text{m}}}{\cancel{\text{s}}} \cdot \frac{\text{N} \cdot \cancel{\text{s}}}{\text{C} \cdot \cancel{\text{m}}} = \frac{\text{N}}{\text{C}} \)
The units match the standard unit for electric field. Therefore, the amplitude of the electric field is \( 183 \, \text{N/C} \).
Comparing this result with the given options, we find that it matches one of them.
Based on the calculation using the relationship \( E_0 = c B_0 \) and the given magnetic field amplitude of \( 610 \, \text{nT} \), the amplitude of the electric field is \( 183 \, \text{NC}^{-1} \).
| Quantity | Symbol | Value | Units |
|---|---|---|---|
| Magnetic Field Amplitude | \( B_0 \) | 610 nT | \( 610 \times 10^{-9} \, \text{T} \) |
| Speed of Light in Vacuum | \( c \) | \( 3 \times 10^8 \) | m/s |
| Electric Field Amplitude | \( E_0 \) | Calculated | N/C (or \( \text{NC}^{-1} \)) |
| Property | Description | Relationship in Vacuum |
|---|---|---|
| Nature | Transverse waves of oscillating electric (\( \vec{E} \)) and magnetic (\( \vec{B} \)) fields. | \( \vec{E} \perp \vec{B} \), \( \vec{E} \perp \) direction of propagation, \( \vec{B} \perp \) direction of propagation. |
| Speed in Vacuum | Constant speed, \( c \). | \( c = \frac{1}{\sqrt{\mu_0 \epsilon_0}} \approx 3 \times 10^8 \, \text{m/s} \). |
| Amplitude Relation | Ratio of electric field amplitude to magnetic field amplitude. | \( \frac{E_0}{B_0} = c \) or \( E_0 = c B_0 \) |
| Energy Propagation | Carries energy and momentum. Described by the Poynting vector. | Intensity is proportional to \( E_0^2 \) and \( B_0^2 \). |
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