From fd01e85b02825953e8f2ef6e4f7caa8b2bd0a406 Mon Sep 17 00:00:00 2001
From: QQQiwi <ulitin.ivan3004@mail.ru>
Date: Sun, 24 Oct 2021 16:21:10 +0400
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---
 sem5/information-theory/lectures/lecture1.tex | 4 ++--
 1 file changed, 2 insertions(+), 2 deletions(-)

(limited to 'sem5/information-theory/lectures/lecture1.tex')

diff --git a/sem5/information-theory/lectures/lecture1.tex b/sem5/information-theory/lectures/lecture1.tex
index 1426835..07586f3 100644
--- a/sem5/information-theory/lectures/lecture1.tex
+++ b/sem5/information-theory/lectures/lecture1.tex
@@ -108,7 +108,7 @@ $\phi(\alpha, t)$ \emph{базисной функцией}. Это модель
 
 \begin{equation*}
   \int_{t_1}^{t_2} \phi_k(t) \phi_l(t) d t =
-  \begin{cases} 0, &k \neq l  \\ 1, &k = l \end{cases}
+  \begin{cases} 0, &k \neq l  \\ \mu, &k = l \end{cases}
   \quad (3)
 \end{equation*}
 
@@ -121,7 +121,7 @@ $\frac{1}{\sqrt{\mu}}$, то мы получим ортонормированн
 
 Пусть имеется модель, удовлетворяющая условию ортонормированности.
 Возьмём модель (1), обе части данной модели умножим на $\phi_l(t)$ и
-\ldots{} . Получим
+проинтегрируем на интервале от $t_1$ до $t_2$. Получим
 
 \begin{equation*}
   \int_{t_1}^{t_2} u(t) \phi_l(t) dt = 
-- 
cgit v1.2.3

