4.05周期信号波形对称性和谐波性质

1. f ( t ) f(t) 为偶函数—对称于纵轴 f ( t ) = f ( t ) f(t)=f(-t)

a n = 2 T T 2 T 2 f ( t ) c o s ( n Ω t ) d t a_n=\frac{2}{T}\int _{-\frac {T}{2}}^\frac{T}2{}f(t)cos(n\Omega t)\rm dt
b n = 2 T T 2 T 2 f ( t ) s i n ( n Ω t ) d t b_n=\frac{2}{T}\int _{-\frac {T}{2}}^\frac{T}2{}f(t)sin(n\Omega t)\rm dt
a n = 2 2 T T 2 T 2 f ( t ) c o s ( n Ω t ) d t a_n = 2* \frac{2}{T}\int _{-\frac {T}{2}}^\frac{T}2{}f(t)cos(n\Omega t)\rm dt
b n = 0 b_n=0 展开为余弦函数。
2. f ( t ) f(t) 为奇函数的时候 f ( t ) = f ( t ) f(t)=-f(-t)
a n = 2 T T 2 T 2 f ( t ) c o s ( n Ω t ) d t a_n=\frac{2}{T}\int _{-\frac {T}{2}}^\frac{T}2{}f(t)cos(n\Omega t)\rm dt
b n = 2 T T 2 T 2 f ( t ) s i n ( n Ω t ) d t b_n=\frac{2}{T}\int _{-\frac {T}{2}}^\frac{T}2{}f(t)sin(n\Omega t)\rm dt
a n = 2 2 T T 2 T 2 f ( t ) c o s ( n Ω t ) a_n = 2* \frac{2}{T}\int _{-\frac {T}{2}}^\frac{T}2{}f(t)cos(n\Omega t)\rm
易得到 a n = 0 a_n=0

3. f ( t ) f(t) 为奇 谐函数--------- f ( t ) = f ( t ± T / 2 ) f(t)=-f(t\pm T/2)

其傅里叶级数中只含有奇次谐波分量,而不含偶次谐波分量,即:

a 0 = a 2 = . . . . . = b 2 = b 4 = . . . = 0 a_0=a_2=.....=b_2=b_4=...=0

4. f ( t ) f(t) 为偶谐函数--------- f ( t ) = f ( t ± T / 2 ) f(t)=f(t\pm T/2)
其傅里叶级数之中只含偶次谐波分量,而不含奇次谐波分量:即
a 1 = a 3 = . . . = b 1 = b 3 = . . . = 0 a_1=a_3=...=b_1=b_3=...=0
在这里插入图片描述

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转载自blog.csdn.net/qq_21104157/article/details/107907744