Pioneering the Power of Piezoelectric Accelerometer: Precision Vibration Sensing Redefined
Discover the cornerstone of vibration sensor technology with our Piezoelectric Accelerometer range. These ingenious sensors harness the power of piezoelectric materials to generate an electrical charge proportional to applied acceleration, offering unmatched accuracy and reliability.
Step into the world of vibration analysis with confidence, as our Piezoelectric Charge Accelerometers offer robust designs capable of withstanding high temperatures and harsh environments. Say goodbye to internal electronics limitations and hello to limitless possibilities in monitoring and control.
The utilization of Piezoelectric Accelerometers does demand attention to detail. To ensure accurate measurements free from interference, high-quality low-noise cables with clean connectors are essential. A phenomenon known as triboelectric noise caused by cable flexing can affect any type of charge accelerometer. Additionally, external charge amplifiers are required to convert the natural charge output into volts for compatibility with DAQ or vibration controller hardware. This means there is an increased risk of noise within the measurement chain, but this can be controlled and minimised.
Our triaxial piezoelectric charge accelerometer range will revolutionize your sensing experience, providing comprehensive insights into multidimensional vibrations. And for those seeking simplicity without compromise, explore our IEPE accelerometers featuring built-in amplifier electronics, ready to integrate seamlessly with your DAQ systems. But that’s not all – to complete your setup, dive into our selection of charge amplifiers, meticulously crafted to enhance the performance of your Piezoelectric Accelerometers.
Experience innovation, precision, and reliability like never before with Piezoelectric Accelerometers from Kemo. Welcome to a world where vibration sensing reaches new heights!
High Temperature General Purpose Monoaxial Piezoelectric Charge Output Accelerometers
HGC50T-T
50pC/g
-55°C to +250°C
±1000g
36grams
18x31 (mm) (inc. Connector)
HGC50T-T
0.5 to 6kHz(±10%)
Stainless steel
10/32UNF Microdot top connector
10/32UNF tapped base
HGC30T-T
30pC/g
-55°C to +250°C
±1000g
12.5grams
14x23 (mm)
HGC30T-T
9kHz
Titanium
10/32UNF Microdot top connector
10/32UNF tapped base
HGC30S-T
30pC/g
-55°C to +250°C
±1000g
12.5grams
14x18 (mm)
HGC30S-T
9kHz
Titanium
10/32UNF Microdot side connector
10/32UNF tapped base
HGC10T-T
10pC/g
-55°C to +250°C
±1000g
6.5grams
11x22 (mm)
HGC10T-T
9kHz
Titanium
10/32UNF Microdot top connector
10/32UNF tapped base
HGC10S-T
10pC/g
-55°C to +250°C
±1000g
6.5grams
11x16 (mm)
HGC10S-T
9kHz
Titanium
10/32UNF Microdot side connector
10/32UNF tapped base
General Purpose Monoaxial Piezoelectric Charge Output Accelerometers
GC10S-T
10pC/g
±5000g
5.8grams
11x16 (mm)
GC10S-T
11kHz
Titanium
10/32UNF Microdot side connector
10/32UNF tapped base
GC20S-T
20pC/g
±2500g
11grams
13x17.5 (mm)
GC20S-T
10kHz
Titanium
10/32UNF Microdot side connector
10/32UNF tapped base
GC50S-T
50pC/g
±1000g
22grams
16x20 (mm)
GC50S-T
6kHz
Titanium
10/32UNF Microdot side connector
10/32UNF tapped base
GC100S-T
100pC/g
±800g
26grams
16x20 (mm)
GC100S-T
6kHz
Titanium
10/32UNF Microdot side connector
10/32UNF tapped base
GC200S-T
200pC/g
±300g
61grams
22x30 (mm)
GC200S-T
3kHz
Titanium
10/32UNF Microdot side connector
10/32UNF tapped base
GC10T-T
10pC/g
±5000g
5.8grams
11x21 (mm)
GC10T-T
11kHz
Titanium
10/32UNF Microdot top connector
10/32UNF tapped base
GC20T-T
20pC/g
±2500g
11grams
13x22.5 (mm)
GC20T-T
10kHz
Titanium
10/32UNF Microdot top connector
10/32UNF tapped base
GC50T-T
50pC/g
±1000g
22grams
16x25 (mm)
GC50T-T
6kHz
Titanium
10/32UNF Microdot top connector
10/32UNF tapped base
GC100T-T
100pC/g
±800g
26grams
16x25 (mm)
GC100T-T
6kHz
Titanium
10/32UNF Microdot top connector
10/32UNF tapped base
GC200T-T
200pC/g
±500g
30grams
16x28 (mm)
GC200T-T
5kHz
Titanium
10/32UNF Microdot top connector
10/32UNF tapped base
Triaxial Piezoelectric Charge Output Accelerometers
GCT2-T
2pC/g
±2000g
15grams
22x22x10 (mm)
GCT2-T
9kHz
Titanium
3 x 10/32UNF Microdot connector
2 x Ø4mm through holes
GCT5-T
5pC/g
±2000g
15grams
22x22x10 (mm)
GCT5-T
9kHz
Titanium
3 x 10/32UNF Microdot connector
2 x Ø4mm through holes
GCT10-H
10pC/g
±1000g
22grams
27.4x22x13 (mm)
GCT10-H
8kHz
Titanium
3 x 10/32UNF Microdot connector
2 x Ø4mm through holes
GCT20-H
20pC/g
±1000g
22grams
27.4x22x13 (mm)
GCT20-H
8kHz
Titanium
3 x 10/32UNF Microdot connector
2 x Ø4mm through holes
GCT10-TH
10pC/g
±1000g
25grams
25x25x14 (mm)
GCT10-TH
7kHz
Titanium
3 x 10/32UNF Microdot connector
1 x Ø5mm through hole
GCT20-TH
20pC/g
±1000g
28grams
25x25x14 (mm)
GCT20-TH
7kHz
Titanium
3 x 10/32UNF Microdot connector
1 x Ø5mm through hole
Piezoelectric Shock Accelerometers
CS-10K
±10000g
0.5pC/g
9grams
12.5x19.5 (mm)
CS-10K
11kHz
Titanium
0.5m Integral Cable
M6 Integral Stud
CS-30K
±30000g
0.3pC/g
9grams
12.5x19.5 (mm)
CS-30K
11kHz
Titanium
0.5m Integral Cable
M6 Integral Stud
CS-50K
±50000g
0.2pC/g
9grams
12.5x19.5 (mm)
CS-50K
11kHz
Titanium
0.5m Integral Cable
M6 Integral Stud
CS-100K
±50000g
0.2pC/g
4.3grams
10.2x19 (mm)
CS-100K
11kHz
Titanium
0.5m Integral Cable
M6 Integral Stud