From 88537b82784f71104c3a2771330c9e492f57fb03 Mon Sep 17 00:00:00 2001
From: Prefetch
Date: Sun, 30 Jan 2022 11:27:00 +0100
Subject: Expand knowledge base, remove comments

---
 content/know/concept/drude-model/index.pdc | 2 --
 1 file changed, 2 deletions(-)

(limited to 'content/know/concept/drude-model/index.pdc')

diff --git a/content/know/concept/drude-model/index.pdc b/content/know/concept/drude-model/index.pdc
index a738dff..703ddbb 100644
--- a/content/know/concept/drude-model/index.pdc
+++ b/content/know/concept/drude-model/index.pdc
@@ -74,7 +74,6 @@ which depends on $\omega$:
 $$\begin{aligned}
     \boxed{
         \varepsilon_r(\omega)
-        %= 1 - \frac{N q^2}{\varepsilon_0 m} \frac{1}{\omega^2 + i \gamma \omega}
         = 1 - \frac{\omega_p^2}{\omega^2 + i \gamma \omega}
     }
 \end{aligned}$$
@@ -190,7 +189,6 @@ The dielectric function $\varepsilon_r(\omega)$ is therefore given by:
 $$\begin{aligned}
     \boxed{
         \varepsilon_r(\omega)
-        %= \varepsilon_{\mathrm{int}}(\omega) - \frac{N q^2}{\varepsilon_0 m^*} \frac{1}{\omega^2 + i \gamma \omega}
         = \varepsilon_{\mathrm{int}} \Big( 1 - \frac{\omega_p^2}{\omega^2 + i \gamma \omega} \Big)
     }
 \end{aligned}$$
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