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目录
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开始
1
低通滤波器
切换低通滤波器子部分
1.1
LR 网络
1.2
RC 网络
2
总结
切换目录
实用电子学/低通滤波器
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来自维基教科书,开放的书籍,开放的世界
<
实用电子学
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低通滤波器
[
编辑
|
编辑源代码
]
LR 网络
[
编辑
|
编辑源代码
]
V
o
V
i
=
Z
R
Z
R
+
Z
L
=
R
R
+
j
ω
L
=
1
1
+
j
ω
T
{\displaystyle {\frac {V_{o}}{V_{i}}}={\frac {Z_{R}}{Z_{R}+Z_{L}}}={\frac {R}{R+j\omega L}}={\frac {1}{1+j\omega T}}}
T
=
L
R
{\displaystyle T={\frac {L}{R}}}
ω
o
=
1
T
=
R
L
{\displaystyle \omega _{o}={\frac {1}{T}}={\frac {R}{L}}}
ω
=
0
V
o
=
V
i
{\displaystyle \omega =0V_{o}=V_{i}}
ω
o
=
1
L
C
V
o
=
V
i
2
{\displaystyle \omega _{o}={\sqrt {\frac {1}{LC}}}V_{o}={\frac {V_{i}}{2}}}
ω
=
00
V
o
=
0
{\displaystyle \omega =00V_{o}=0}
绘制上面的三个点,我们得到一个图
V
o
−
ω
{\displaystyle Vo-\omega }
。从图中,我们看到电压在低频下不会随频率变化,因此 LR 网络可以被用作低通滤波器
RC 网络
[
编辑
|
编辑源代码
]
V
o
V
i
=
Z
C
Z
R
+
Z
C
=
1
j
ω
C
R
+
1
j
ω
C
=
1
1
+
j
ω
T
{\displaystyle {\frac {V_{o}}{V_{i}}}={\frac {Z_{C}}{Z_{R}+Z_{C}}}={\frac {\frac {1}{j\omega C}}{R+{\frac {1}{j\omega C}}}}={\frac {1}{1+j\omega T}}}
T
=
R
C
{\displaystyle T=RC}
ω
o
=
1
T
=
1
R
C
{\displaystyle \omega _{o}={\frac {1}{T}}={\frac {1}{RC}}}
ω
=
0
V
o
=
V
i
{\displaystyle \omega =0V_{o}=V_{i}}
ω
o
=
1
L
C
V
o
=
V
i
2
{\displaystyle \omega _{o}={\sqrt {\frac {1}{LC}}}V_{o}={\frac {V_{i}}{2}}}
ω
=
00
V
o
=
0
{\displaystyle \omega =00V_{o}=0}
绘制上面的三个点,我们得到一个图
V
o
−
ω
{\displaystyle Vo-\omega }
。从图中,我们看到电压在低频下不会随频率变化,因此 LR 网络可以被用作低通滤波器
总结
[
编辑
|
编辑源代码
]
一般而言
低通滤波器可以由两种网络 LR 或 RC 构成。
低通滤波器在低频下具有稳定的电压,不会随频率变化。
低通滤波器可以用以下数学形式表示
V
o
V
i
=
1
1
+
j
ω
T
{\displaystyle {\frac {V_{o}}{V_{i}}}={\frac {1}{1+j\omega T}}}
对于 RC 网络,T = RC
T
=
L
R
{\displaystyle T={\frac {L}{R}}}
对于 RL 网络
类别
:
书籍:实用电子学
华夏公益教科书