Practice
practice problem 1
Determine the following quanities at a distance of one meter from a 100 W light bulb …
- the peak electric field
- the peak magnetic field
- the radiation pressure
solution
- Use the definition of power density and the pointing vector to determine
the electric field. Imagine the radiation spreading outward to cover
the surface area of a sphere.
| |
| S = |
P |
= |
1 |
EB = |
1 |
E |
E |
= |
E2 |
⇒ |
E = √ |
Pμ0c |
| A |
μ0 |
μ0 |
c |
μ0c |
A |
| |
Solve for the electric field and imagine the energy spread out over the
surface of a 1 m radius sphere.
| |
| E = √ |
Pμ0c |
= √ |
Pμ0c |
= √ |
(100 W)(4π × 10−7 N/A2)(3.00 × 108 m/s) |
= √(3000 N2/C2) = 54.8 N/C |
| A |
4πr2 |
4π(1 m)2 |
| |
This is a field strength that could be measured with fairly inexpensive
equipment if it weren't fluctuating so rapidly. (Visible light frequencies
are very high).
- Use these results and the fact that the ratio of the electric to magnetic
fields is the speed of light.
| |
| c = |
E |
⇒ |
B = |
E |
= |
54.8 N/C |
= 1.83 × 10−7 T = 183 nT |
| B |
c |
3.00 × 108 m/s |
| |
Compared to the electric field, the magnetic field is less easily detected.
For comparison, the earth's magnetic field is 250 times stronger and
does not vary much with time.
- Use the radiation pressure formula to determine the radiation pressure
(duh).
| |
| P = |
1 |
ε0E2 = |
1 |
(8.85 × 10−12 C2/Nm2)(54.8 N/C)2 = 1.33 × 10−8 Pa = 13.3 nPa |
| 2 |
2 |
| |
Such a weak pressure is imperceptible under ordinary circumstances and
difficult to measure in the laboratory without exceptionally delicate
apparatus.
practice problem 2
Write something.
solution
Answer it.
practice problem 3
Write something.
solution
Answer it.
practice problem 4
Write something completely different.
solution
Answer it.