Search Results for 422e52: in-line charge converter

In-line charge converter, 10 mV/pC, +/-5V output, -5% frequency 5 Hz. Sensitivity: (±2.5%)10 mV/pC; Output Voltage: ±5.0 V; Temperature Range: -65 to +250 °F (-54 to +121 °C) Housing Material: Stainless Steel

In-line ICP® charge converters play a vital role in converting high impedance charge mode piezoelectric sensor signals into low impedance voltage signals, facilitating input to readout, recording, and analysis instruments.

The 422E5X series charge amplifiers convert the high impedance charge signal from a charge mode transducer to a low impedance voltage signal. This conversion is accomplished by the use of a feedback capacitor across an inverting amplifier (Fig 1). The gain of the amplifier is sufficiently high to make the charge amplifier gain virtually

[1] Tested using voltage source and input capacitor equal to the feedback capacitor, to simulate a charge output sensor. [2] Effective feedback resistance for time constant is 3 times tested value due to circuitry (i.e 1x10E9 = 3x10E9 ohm) [3] High frequency response may be limited by supply current and output cable length. [4] .

converter to the signal conditioner or readout device. These units are well suited for use with high temperature piezoelectric sensors operating in environments up to 500 °F

Model 422E52:In-line charge converter, 10 mV/pC, +/-5V output, -5% frequency 5 Hz . [1] High frequency response may be limited by supply current and output cable length.

Model 422E52:In-line charge converter, 10 mV/pC, +/-5V output, -5% frequency 5 Hz . [1] High frequency response may be limited by supply current and output cable length.

In-line ICP® charge converters serve to convert high impedance charge mode piezoelectric sensor signals into low impedance voltage signals for input into readout, recording, and analysis instruments.

Model 422E52:In-line charge converter, 10 mV/pC, +/-5V output, -5% frequency 5 Hz . [1] High frequency response may be limited by supply current and output cable length.

In-line charge converter, 10 mV/pC, +/-2.5V output, -5% frequency 0.5 Hz. Sensitivity: (±2%)10 mV/pC; Output Voltage: ±2.5 Vpk; Temperature Range: -65 to +250 °F (-54 to +121 °C) Housing Material: Stainless Steel

For example PCB® in-line charge convertor model 422E52 has a time constant of >0.1 seconds and a low frequency response of 5 Hz (-5%). Every charge mode accelerometer has a natural frequency that will restrict the measurement frequency range to some upper limit.

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The 422E series in-line charge converters are designed to convert the high impedance of a charge mode piezoelectric transducer to a low-impedance voltage by means of an ICP ® signal conditioner. These units may be used with either quartz or ceramic charge-mode piezoelectric sensors.

In-line charge converter, 0.5 mV/pC, +/-5V output, -5% frequency 0.5 Hz. Sensitivity: (±2.5%)0.5 mV/pC; Output Voltage: ±5.0 V; Temperature Range: -65 to +250 °F (-54 to +121 °C) Housing Material: Stainless Steel

The 422E series in-line charge converters are designed to convert the high impedance of a charge mode piezoelectric transducer to a low-impedance voltage by means of an ICP ® signal conditioner. These units may be used with either quartz or ceramic charge-mode piezoelectric sensors.

In-line charge converter, 10 mV/pC, +/-2.5V output, -5% frequency 5 Hz, for high temp sensors

The 422E series in-line charge converters are designed to convert the high impedance of a charge mode piezoelectric transducer to a low-impedance voltage by means of an ICP ® signal conditioner. These units may be used with either quartz or ceramic charge-mode piezoelectric sensors.

In-line charge converter, 1 mV/pC, +/-2.5V output, -5% frequency 5 Hz, for high temp sensors. Sensitivity: (±2%)1 mV/pC; Output Voltage: ±2.5 V; Temperature Range: -65 to +250 °F (-54 to +121 °C) Housing Material: Stainless Steel

[1] Tested using voltage source and input capacitor equal to the feedback capacitor, to simulate a charge output sensor. [2] Effective feedback resistance for time constant is 3 times tested value due to circuitry (i.e 1x10E9 = 3x10E9 ohm) [3] High frequency response may be limited by supply current and output cable length. [4] .