Part | RoHS | Manufacturer | Crystal or Resonator Type | Mounting Feature | Frequency Tolerance | Minimum Operating Frequency | Maximum Operating Frequency | Aging | Load Capacitance | Additional Features | Series Resistance | Frequency Stability | Minimum Operating Temperature | Terminal Finish | JESD-609 Code | Nominal Operating Frequency | Drive Level | Physical Dimension | Manufacturer Series | Maximum Operating Temperature |
---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
|
Cts |
SERIES - FUNDAMENTAL |
THROUGH HOLE MOUNT |
45 ppm |
AT-CUT CRYSTAL; BULK |
150 ohm |
50 % |
-20 Cel |
TIN SILVER COPPER |
e1 |
4 MHz |
100 uW |
L10.85XB4.5XH13.46 (mm)/L0.427XB0.177XH0.53 (inch) |
70 Cel |
||||||
|
Murata Manufacturing |
PARALLEL - FUNDAMENTAL |
SURFACE MOUNT |
45 ppm |
6 pF |
100 ohm |
40 % |
-30 Cel |
48 MHz |
300 uW |
L2.0XB1.6XH0.7 (mm)/L0.079XB0.063XH0.028 (inch) |
85 Cel |
||||||||
|
Cts |
PARALLEL - FUNDAMENTAL |
THROUGH HOLE MOUNT |
45 ppm |
20 pF |
AT-CUT CRYSTAL; BULK |
75 ohm |
50 % |
-20 Cel |
TIN SILVER COPPER |
e1 |
4.9152 MHz |
100 uW |
L10.85XB4.5XH13.46 (mm)/L0.427XB0.177XH0.53 (inch) |
70 Cel |
|||||
|
Cts |
PARALLEL - FUNDAMENTAL |
THROUGH HOLE MOUNT |
45 ppm |
20 pF |
AT-CUT CRYSTAL; BULK |
50 ohm |
50 % |
-20 Cel |
TIN SILVER COPPER |
e1 |
6.144 MHz |
100 uW |
L10.85XB4.5XH13.46 (mm)/L0.427XB0.177XH0.53 (inch) |
70 Cel |
|||||
|
Cts |
PARALLEL - FUNDAMENTAL |
THROUGH HOLE MOUNT |
45 ppm |
13 pF |
AT-CUT CRYSTAL; BULK |
750 ohm |
50 % |
-20 Cel |
Tin/Silver/Copper (Sn/Ag/Cu) |
e1 |
1.8432 MHz |
100 uW |
L10.85XB4.5XH13.46 (mm)/L0.427XB0.177XH0.53 (inch) |
MP |
70 Cel |
||||
|
Cts |
PARALLEL - FUNDAMENTAL |
THROUGH HOLE MOUNT |
45 ppm |
20 pF |
AT-CUT CRYSTAL; BULK |
750 ohm |
50 % |
-20 Cel |
TIN SILVER COPPER |
e1 |
2 MHz |
100 uW |
L10.85XB4.5XH13.46 (mm)/L0.427XB0.177XH0.53 (inch) |
70 Cel |
|||||
|
Cts |
PARALLEL - FUNDAMENTAL |
THROUGH HOLE MOUNT |
45 ppm |
32 pF |
AT-CUT CRYSTAL; BULK |
300 ohm |
50 % |
-20 Cel |
TIN SILVER COPPER |
e1 |
2.4576 MHz |
100 uW |
L10.85XB4.5XH13.46 (mm)/L0.427XB0.177XH0.53 (inch) |
MP |
70 Cel |
||||
|
Cts |
PARALLEL - FUNDAMENTAL |
THROUGH HOLE MOUNT |
45 ppm |
20 pF |
AT-CUT CRYSTAL; BULK |
150 ohm |
50 % |
-20 Cel |
TIN SILVER COPPER |
e1 |
3.6864 MHz |
100 uW |
L10.85XB4.5XH13.46 (mm)/L0.427XB0.177XH0.53 (inch) |
70 Cel |
|||||
|
Cts |
PARALLEL - FUNDAMENTAL |
THROUGH HOLE MOUNT |
45 ppm |
20 pF |
AT-CUT CRYSTAL; BULK |
150 ohm |
50 % |
-20 Cel |
TIN SILVER COPPER |
e1 |
4 MHz |
100 uW |
L10.85XB4.5XH13.46 (mm)/L0.427XB0.177XH0.53 (inch) |
70 Cel |
|||||
|
Cts |
PARALLEL - FUNDAMENTAL |
THROUGH HOLE MOUNT |
45 ppm |
12 pF |
AT-CUT CRYSTAL; BULK |
75 ohm |
50 % |
-20 Cel |
Tin/Silver/Copper (Sn/Ag/Cu) |
e1 |
4.194304 MHz |
100 uW |
L10.85XB4.5XH13.46 (mm)/L0.427XB0.177XH0.53 (inch) |
MP |
70 Cel |
||||
|
Cts |
SERIES - FUNDAMENTAL |
SURFACE MOUNT |
45 ppm |
AT-CUT CRYSTAL; TAPE AND REEL |
35 ohm |
50 % |
-20 Cel |
TIN SILVER COPPER OVER NICKEL |
15 MHz |
100 uW |
L13.48XB10.85XH4.5 (mm)/L0.531XB0.427XH0.177 (inch) |
MP |
70 Cel |
||||||
|
Cts |
SERIES - FUNDAMENTAL |
THROUGH HOLE MOUNT |
45 ppm |
AT-CUT CRYSTAL; BULK |
35 ohm |
50 % |
-20 Cel |
TIN SILVER COPPER |
e1 |
24 MHz |
100 uW |
L10.85XB4.5XH13.46 (mm)/L0.427XB0.177XH0.53 (inch) |
70 Cel |
Crystal oscillators are electronic components that generate stable and precise frequency signals for various applications. They are widely used in electronic devices and systems that require a precise frequency source, such as clocks, radios, and telecommunications equipment.
Crystal oscillators consist of a quartz crystal resonator, which is cut to vibrate at a specific frequency when an AC voltage is applied across it. The resonance frequency is determined by the dimensions of the crystal and the properties of the quartz material, which have a high Q-factor and temperature stability. The crystal resonator is connected to an amplifier circuit that provides feedback and controls the frequency of the output signal.
Crystal oscillators offer several advantages over other types of frequency sources, including high accuracy, stability, and low phase noise. They can operate at a wide range of frequencies, ranging from a few kilohertz to several gigahertz, and they are available in different package sizes and configurations, including through-hole and surface-mount.
Crystal oscillators come in different types, such as Pierce, Colpitts, and Butler, each with different characteristics and performance levels. They are also available in different tolerances and stability levels, depending on the application and the required performance