From e28d2a982d0c65fcad9a2d2a4c20d06a9848fa8f Mon Sep 17 00:00:00 2001
From: Prefetch
Date: Tue, 5 Oct 2021 19:31:12 +0200
Subject: Expand knowledge base

---
 content/know/concept/maxwell-boltzmann-distribution/index.pdc | 4 ++--
 1 file changed, 2 insertions(+), 2 deletions(-)

(limited to 'content/know/concept/maxwell-boltzmann-distribution/index.pdc')

diff --git a/content/know/concept/maxwell-boltzmann-distribution/index.pdc b/content/know/concept/maxwell-boltzmann-distribution/index.pdc
index 38b56fd..3328eaf 100644
--- a/content/know/concept/maxwell-boltzmann-distribution/index.pdc
+++ b/content/know/concept/maxwell-boltzmann-distribution/index.pdc
@@ -20,7 +20,7 @@ probability distributions with applications in classical statistical physics.
 
 ## Velocity vector distribution
 
-In the canonical ensemble
+In the [canonical ensemble](/know/concept/canonical-ensemble/)
 (where a fixed-size system can exchange energy with its environment),
 the probability of a microstate with energy $E$ is given by the Boltzmann distribution:
 
@@ -31,7 +31,7 @@ $$\begin{aligned}
 
 Where $\beta = 1 / k_B T$.
 We split $E = K + U$,
-where $K$ and $U$ are the total kinetic and potential energy contributions.
+with $K$ and $U$ the total kinetic and potential energy contributions.
 If there are $N$ particles in the system,
 with positions $\tilde{r} = (\vec{r}_1, ..., \vec{r}_N)$
 and momenta $\tilde{p} = (\vec{p}_1, ..., \vec{p}_N)$,
-- 
cgit v1.2.3