EPSON爱普生石英晶体Q22FA1280048500等效电路与谐振频率和石英振荡器原理
石英晶体等效电路
当石英晶体不振动时,可等效为一个平板电容C0,称为静态电容;其值决定于晶片的几何尺寸和电极面积,一般为几到几十皮法.当晶片产生振动时,进口晶振代理商机械振动的惯性等效为电感L,其值为几毫亨到几十亨.晶片的弹性等效为电容C,其值仅为0.01到01pf,因此C《C0.晶片的摩擦损耗等效为电阻R,其值约为100欧,理想情况下R=0.当等效电路中的L,R,C支路产生串联谐振时,该支路呈纯阻性,谐振频率等效电阻为R.
EPSON爱普生石英晶振,Q22FA1280048500石英晶体谐振器
爱普生晶振编码
长x宽x高
型号
石英晶振频率
负载
频率25°C
频率公差
工作温度范围
ESR最大
驱动电平
Q22FA1280047000
2x1.6x0.5mm
FA-128
26.000000MHz
12pF
+/-10ppm
+/-20ppm
-40to+85°C
≤60Ω
≤100µW
Q22FA1280047100
2x1.6x0.5mm
FA-128
33.330000MHz
7pF
+/-30ppm
+/-30ppm
-20to+75°C
≤60Ω
≤100µW
Q22FA1280047300
2x1.6x0.5mm
FA-128
25.000000MHz
6pF
+/-30ppm
+/-20ppm
-40to+85°C
≤80Ω
≤100µW
Q22FA1280047600
2x1.6x0.5mm
FA-128
27.120000MHz
8pF
+/-15ppm
+/-20ppm
-40to+85°C
≤60Ω
≤100µW
Q22FA1280047900
2x1.6x0.5mm
FA-128
48.000000MHz
8pF
+/-50ppm
+/-30ppm
-20to+75°C
≤60Ω
≤100µW
Q22FA1280048000
2x1.6x0.5mm
FA-128
28.636300MHz
6pF
+/-10ppm
+/-10ppm
-20to+75°C
≤60Ω
≤100µW
Q22FA1280048400
2x1.6x0.5mm
FA-128
48.000000MHz
6pF
+/-10ppm
+/-20ppm
-20to+70°C
≤60Ω
≤100µW
Q22FA1280048500
2x1.6x0.5mm
FA-128
25.000000MHz
20pF
+/-30ppm
+/-30ppm
-20to+85°C
≤80Ω
≤100µW
Q22FA1280048700
2x1.6x0.5mm
FA-128
16.000000MHz
99pF
+/-30ppm
+/-30ppm
-20to+75°C
≤200Ω
≤100µW
Q22FA1280048900
2x1.6x0.5mm
FA-128
24.000000MHz
12pF
+/-10ppm
+/-10ppm
-20to+85°C
≤80Ω
≤100µW
Q22FA1280049500
2x1.6x0.5mm
FA-128
24.000000MHz
6pF
+/-10ppm
+/-50ppm
-40to+85°C
≤80Ω
≤100µW
Q22FA1280049700
2x1.6x0.5mm
FA-128
52.000000MHz
6.7pF
+/-10ppm
+/-10ppm
-20to+75°C
≤60Ω
≤100µW
Q22FA1280049900
2x1.6x0.5mm
FA-128
24.000000MHz
10pF
+/-10ppm
+/-20ppm
-40to+85°C
≤80Ω
≤100µW
Q22FA1280050200
2x1.6x0.5mm
FA-128
32.000000MHz
6pF
+/-20ppm
+/-30ppm
-40to+85°C
≤60Ω
≤100µW
Q22FA1280050600
2x1.6x0.5mm
FA-128
38.400000MHz
12pF
+/-10ppm
+/-20ppm
-40to+85°C
≤60Ω
≤100µW
Q22FA1280050700
2x1.6x0.5mm
FA-128
16.000000MHz
9pF
+/-10ppm
+/-15ppm
-30to+85°C
≤200Ω
≤100µW
Q22FA1280051300
2x1.6x0.5mm
FA-128
16.000000MHz
10pF
+/-30ppm
+/-30ppm
-40to+85°C
≤200Ω
≤100µW
Q22FA1280051400
2x1.6x0.5mm
FA-128
32.000000MHz
12pF
+/-10ppm
+/-20ppm
-40to+85°C
≤60Ω
≤100µW
Q22FA1280051700
2x1.6x0.5mm
FA-128
32.000000MHz
6pF
+/-10ppm
+/-20ppm
-40to+85°C
≤60Ω
≤100µW
Q22FA1280051900
2x1.6x0.5mm
FA-128
52.000000MHz
8pF
+/-10ppm
+/-12ppm
-30to+85°C
≤60Ω
≤100µW
Q22FA1280052600
2x1.6x0.5mm
FA-128
24.000000MHz
8.5pF
+/-9ppm
+/-9ppm
-10to+70°C
≤80Ω
≤100µW
Q22FA1280052900
2x1.6x0.5mm
FA-128
16.000000MHz
6pF
+/-10ppm
+/-10ppm
-20to+75°C
≤200Ω
≤100µW
Q22FA1280053000
2x1.6x0.5mm
FA-128
32.000000MHz
10pF
+/-10ppm
+/-10ppm
-20to+75°C
≤50Ω
≤100µW
Q22FA1280053100
2x1.6x0.5mm
FA-128
50.000000MHz
10pF
+/-15ppm
+/-15ppm
-40to+85°C
≤60Ω
≤100µW
石英振荡器原理
若在晶片的两个极板间加一电场,会使晶体产生机械变形;反之,若在极板间施加机械力,又会在相应的方向上产生电场,这种现象称为压电效应.如在极板间所加的是交变电压,就会产生机械变形振动,同时机械变形振动又会产生交变电场.一般来说,无源贴片晶振这种机械振动的振幅是比较小的,其振动频率则是很稳定的.但当外加交变电压的频率与晶片的固有频率(决定于晶片的尺寸)相等时,机械振动的幅度将急剧增加,这种现象称为压电谐振,因此石英晶体又称为石英晶体谐振器.
EPSON爱普生石英晶振,Q22FA1280048500石英晶体谐振器