This discussion board is a place to discuss our Daily Challenges and the math and science
related to those challenges. Explanations are more than just a solution — they should
explain the steps and thinking strategies that you used to obtain the solution. Comments
should further the discussion of math and science.
When posting on Brilliant:
Use the emojis to react to an explanation, whether you're congratulating a job well done , or just really confused .
Ask specific questions about the challenge or the steps in somebody's explanation. Well-posed questions can add a lot to the discussion, but posting "I don't understand!" doesn't help anyone.
Try to contribute something new to the discussion, whether it is an extension, generalization or other idea related to the challenge.
Stay on topic — we're all here to learn more about math and science, not to hear about your favorite get-rich-quick scheme or current world events.
Markdown
Appears as
*italics* or _italics_
italics
**bold** or __bold__
bold
- bulleted - list
bulleted
list
1. numbered 2. list
numbered
list
Note: you must add a full line of space before and after lists for them to show up correctly
# I indented these lines
# 4 spaces, and now they show
# up as a code block.
print "hello world"
# I indented these lines
# 4 spaces, and now they show
# up as a code block.
print "hello world"
Math
Appears as
Remember to wrap math in \( ... \) or \[ ... \] to ensure proper formatting.
2 \times 3
2×3
2^{34}
234
a_{i-1}
ai−1
\frac{2}{3}
32
\sqrt{2}
2
\sum_{i=1}^3
∑i=13
\sin \theta
sinθ
\boxed{123}
123
Comments
There is no electric field inside a conductor. Suppose we bring a plus
charge near a conductor. For a very short moment, there will be an electric field inside
the conductor. However, this field will act on and move the electrons, which are free
to move about. The electrons will move close to the plus charge, leaving net positive
charge behind. The conductor’s charges will continue to move until the “external”
E~ -field is cancelled out — at that point there is no longer an E~ -field to move them, so
they stay still.
Alt text
Figure 1: Conductor near an external charge. The charges in the conductor very quickly
rearrange themselves to cancel out the external field.
A more accurate statement of this rule is “After a very short time, there is no
electric field inside a conductor”. How short a time is it? Recall that in cgs units,resistivity (which tells us how good/bad something conducts electricity) is measured
in seconds. It turns out that the time it takes for the charges to rearrange themselves
to cancel out the external E~ -field is just about equal to this resistivity. For metals,
this is a time that is something like 10−16 − 10−17 seconds. This is so short that we
can hardly complain that the original statement isn’t precise enough!
Easy Math Editor
This discussion board is a place to discuss our Daily Challenges and the math and science related to those challenges. Explanations are more than just a solution — they should explain the steps and thinking strategies that you used to obtain the solution. Comments should further the discussion of math and science.
When posting on Brilliant:
*italics*
or_italics_
**bold**
or__bold__
paragraph 1
paragraph 2
[example link](https://brilliant.org)
> This is a quote
\(
...\)
or\[
...\]
to ensure proper formatting.2 \times 3
2^{34}
a_{i-1}
\frac{2}{3}
\sqrt{2}
\sum_{i=1}^3
\sin \theta
\boxed{123}
Comments
There is no electric field inside a conductor. Suppose we bring a plus charge near a conductor. For a very short moment, there will be an electric field inside the conductor. However, this field will act on and move the electrons, which are free to move about. The electrons will move close to the plus charge, leaving net positive charge behind. The conductor’s charges will continue to move until the “external” E~ -field is cancelled out — at that point there is no longer an E~ -field to move them, so they stay still.
Alt text
Figure 1: Conductor near an external charge. The charges in the conductor very quickly rearrange themselves to cancel out the external field.
A more accurate statement of this rule is “After a very short time, there is no electric field inside a conductor”. How short a time is it? Recall that in cgs units,resistivity (which tells us how good/bad something conducts electricity) is measured in seconds. It turns out that the time it takes for the charges to rearrange themselves to cancel out the external E~ -field is just about equal to this resistivity. For metals, this is a time that is something like 10−16 − 10−17 seconds. This is so short that we can hardly complain that the original statement isn’t precise enough!