麦斯威尔与基尔霍夫
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麦斯威尔与基尔霍夫CMOS8¤>nO Lecture 2, Sept. 23, 2003
J
§
1. Maxwell Kirchho
D §
2.
1/34
O
3.
4. Smith
B
5.
Và968ê§S-ê
6.
{|9g
7.
L-
π
á
1. Chs. 5-6, Ch. 4 of Thomas Lee’s book
2.1§>:§]§/CMOS8¤>
O0
Maxwell Kirchho§ 2/34
Kirchho’s voltage and current “laws” are approximations which
hold only in the lumped regime. They are derivable from Maxwell’s
equations if we assume quasistatic behavior, thereby eliminating the
coupling terms that give rise to the wave equation.
Maxwell equations:
H = 0 (1)
εE = ρ (2
J
§
1. Maxwell Kirchho
D §
2.
1/34
O
3.
4. Smith
B
5.
Và968ê§S-ê
6.
{|9g
7.
L-
π
á
1. Chs. 5-6, Ch. 4 of Thomas Lee’s book
2.1§>:§]§/CMOS8¤>
O0
Maxwell Kirchho§ 2/34
Kirchho’s voltage and current “laws” are approximations which
hold only in the lumped regime. They are derivable from Maxwell’s
equations if we assume quasistatic behavior, thereby eliminating the
coupling terms that give rise to the wave equation.
Maxwell equations:
H = 0 (1)
εE = ρ (2
关键词： Maxwell Kirchhoff 传输线 微带线 Smith圆图 导纳圆图 双端口网络 交流小信号 阻抗匹配
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