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Piezo-electric Charge Amplifiers
- 04NA System
- (DJB Instruments: Piezo-electric Charge Amplifiers)
- Applications:
- Vibration Sensors Vibration Monitoring and Analysis
- Signal Conditioning and Displays
Other DJB Instruments products >
- Mono-Axial Charge Output - A20 Series
- Mono-Axial Charge Output - A21 Series
- Mono-Axial Charge Output - A22 Series
- Mono-Axial Charge Output - A23 Series
- Mono-Axial Charge Output - A23SI Series
- Mono-Axial Charge Output - A24 Series
- Mono-Axial Charge Output - A25 Series
- Mono-Axial Charge Output - A26 Series
- Mono-Axial Charge Output - A28 Series
- Mono-Axial Charge Output - A29 Series
- Mono-Axial Charge Output - A600 Series
- Mono-Axial Charge Output - A800 Series
- Mono-Axial Voltage Output with Integrated Electronics - A120 Series
- Mono-Axial Voltage Output with Integrated Electronics - A121 Series
- Mono-Axial Voltage Output with Integrated Electronics - A122 Series
- Mono-Axial Voltage Output with Integrated Electronics - A123 Series
- Mono-Axial Voltage Output with Integrated Electronics - A124 Series
- Tri axial Charged Output - A31 Series
- Tri axial Charged Output - A32 Series
- Tri axial Charged Output - A33 Series
- Tri axial Charged Output - A30 Series
- Tri axial Charged Output - A34 Series
- Tri axial Charged Output - A38 Series
- Tri axial Charged Output - AT04 Series
- Tri-Axial Voltage Output with Integrated Electronics - A130 Series
- Tri-Axial Voltage Output with Integrated Electronics - A131 Series
- Differential Charge Amplifier - 04DA System
- Charge amplifier velocity converter - 04VA System
- Hybrid Charge amplifier - CA100 System
- Hybrid two wire voltage source line driver - QV01
- 4 channel voltage source amplifier - V404A System
- Bandpass Filter - BP04
- Highpass/ Lowpass Filter - HP04/ LP04
- Tunable Bandpass Filter - TF04
- Portable Vibration Accesaries - PVA
- Handheld Vibration Meter - VT1
- Handheld Vibration Meter - VT2
- High intensity piezo-electric microphone - M01
- High intensity piezo-electric microphone - M02
- Ultra high Temperature piezo-electric microphone - M02TI
The dominant source is input voltage noise en, amplified by the non-inverting gain of the transducer interface section. This latter is a function of the signal source impedance, 1/w (Ct+Cc), and charge amplifier transfer impedance 1/wCf being unity (best case) for open circuit input.
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