Skip to content
GitLab
Explore
Sign in
Register
Primary navigation
Search or go to…
Project
lectures
Manage
Activity
Members
Labels
Plan
Issues
Issue boards
Milestones
Wiki
Code
Merge requests
Repository
Branches
Commits
Tags
Repository graph
Compare revisions
Snippets
Build
Pipelines
Jobs
Pipeline schedules
Artifacts
Deploy
Releases
Container Registry
Model registry
Operate
Environments
Monitor
Incidents
Service Desk
Analyze
Value stream analytics
Contributor analytics
CI/CD analytics
Repository analytics
Model experiments
Help
Help
Support
GitLab documentation
Compare GitLab plans
Community forum
Contribute to GitLab
Provide feedback
Keyboard shortcuts
?
Snippets
Groups
Projects
Show more breadcrumbs
Solid state physics
lectures
Commits
46379505
Commit
46379505
authored
5 years ago
by
Anton Akhmerov
Browse files
Options
Downloads
Plain Diff
Merge branch 'drude_better_calc' into 'master'
rework the drude derivation See merge request
!72
parents
f7741401
de268634
No related branches found
Branches containing commit
No related tags found
1 merge request
!72
rework the drude derivation
Pipeline
#28698
passed
5 years ago
Stage: build
Stage: deploy
Changes
1
Pipelines
1
Hide whitespace changes
Inline
Side-by-side
Showing
1 changed file
src/3_drude_model.md
+12
-10
12 additions, 10 deletions
src/3_drude_model.md
with
12 additions
and
10 deletions
src/3_drude_model.md
+
12
−
10
View file @
46379505
...
...
@@ -135,20 +135,22 @@ Our goal is then to compute the *average* velocity.
happens with each individual element.
**
Let us compute how the average velocity changes with time.
The equation with the Lorentz force we just average right away:
Consider the effect that scattering has over a small time $dt$.
A fraction $dt/τ$ of the electrons scatters, and that their average velocity becomes zero.
The rest of the electrons $(1 - dt/τ)$ are accelerated by the Lorentz force, and after $dt$ their velocity becomes
$$
m
\
f
rac{d⟨
\m
athbf{v}⟩}{dt} = -e
\l
eft
(
\m
athbf{E}
+⟨
\m
athbf{v}
⟩×
\m
athbf{B}
\r
ight)
.
m
\
m
athbf{v}(t + dt) - m
\m
athbf{v}(t) = - e
(
\m
athbf{E}
+
\m
athbf{v}
×
\m
athbf{B}
)⋅dt
.
$$
Almost there, but we still need to do something with the change of the average velocity due to scattering.
Consider the effect that scattering has over a small time $dt$.
Most electrons continue with the same velocity, however a fraction $dt/τ$ will scatter, and that their average velocity becomes zero.
Therefore we get
Averaging the velocity of the two groups of particles, we get
$$
⟨
\m
athbf{v}(t+dt)⟩ = ⟨
\m
athbf{v}(t)⟩(1 - dt/τ) + 0⋅(dt/τ) ⇒
\f
rac{d⟨
\m
athbf{v}⟩}{dt} = -
\f
rac{⟨
\m
athbf{v}⟩}{τ}.
\b
egin{align}
m⟨
\m
athbf{v}(t+dt)⟩ &= [m⟨
\m
athbf{v}(t)⟩ - e (
\m
athbf{E} +
\m
athbf{v} ×
\m
athbf{B})dt]
\l
eft(1 -
\f
rac{dt}{
\t
au}
\r
ight) + 0⋅
\f
rac{dt}{
\t
au}
\\
&= m⟨
\m
athbf{v}(t)⟩ - dt [e (
\m
athbf{E} +
\m
athbf{v} ×
\m
athbf{B}) - m⟨
\m
athbf{v}(t)⟩/τ]
\\
&
\q
uad
\q
uad
\q
uad
\q
uad + e (
\m
athbf{E} +
\m
athbf{v} ×
\m
athbf{B}) m⟨
\m
athbf{v}(t)⟩dt²/τ.
\e
nd{align}
$$
That's it!
We now combine both contributions into a single equation and get
We now neglect the term proportional to $dt²$ (it vanishes when $dt → ∞$).
Finally, we recognize that $(⟨
\m
athbf{v}(t+dt)⟩ - (⟨
\m
athbf{v}(t)⟩)/dt = d⟨
\m
athbf{v}(t)⟩)/dt$, and arrive to
$$
m
\f
rac{d⟨
\m
athbf{v}⟩}{dt} = -m
\f
rac{⟨
\m
athbf{v}⟩}{τ} -e
\l
eft(
\m
athbf{E}+⟨
\m
athbf{v}⟩×
\m
athbf{B}
\r
ight).
$$
...
...
This diff is collapsed.
Click to expand it.
Preview
0%
Loading
Try again
or
attach a new file
.
Cancel
You are about to add
0
people
to the discussion. Proceed with caution.
Finish editing this message first!
Save comment
Cancel
Please
register
or
sign in
to comment