1-999 Pieces
$10.00
≥1000 Pieces
$9.50
The mechanism of ultrasonic cleaning is to make use of the physical effects such as cavitation, radiation pressure and sound flow in the cleaning liquid. It can exfoliate the machinery produced by the dirt on the cleaning parts, and can also promote the chemical reaction between the cleaning liquid and the dirt, so as to achieve the purpose of cleaning the object. The frequency of the ultrasonic cleaning machine can be selected by 10~500 kHz according to the size and purpose of the cleaning material, generally more than 20~50 kHz. With the increase of the frequency of ultrasonic transducer, Langerhans oscillator, longitudinal oscillator and thickness oscillator can be used. In the miniaturization aspect, radial vibration and flexural vibration are also adopted. Ultrasonic cleaning has become more and more widely used in various industries, agriculture, household equipment, electronics, automobile, rubber, printing, aircraft, food, hospital and medical research.
Ultrasonic transducer is to convert electrical energy into sound energy which also is called ultrasonic.it is composed of outer shell,matching tier,ring piezoelectric ceramic,backing material,outgoing cable and cymbal. The characteristics of transducers depend on material selection and manufacturing process. The performance and service life of transducers of the same size and shape are very different.
Features:
1: High mechanical Q value.
2: High transfer efficiency.
3: High quality piezoelectric ceramic material with good heat resistence.
4: Large range of working temperature.
5: Lower resonant Impedance.
6: Large amplitude,high vibration speed.
7: Clean and tidy appearance,without corrosion,deformation and scratch.
8: Frequency and static capacitance keep more consistency.
9: High output power.
10: ight with bolt ,be easy to install,reliable .
Specification List | ||||||
Model | Frequency | Capacitance | Resonance Impedance | Size | Power | Insulation resistance |
(KHz) | (pF) | (Ω) | Radiation head*Height (mm) | (W) | (2500VDC) | |
ARS-4QXHNQ-17K60W | 17±0.5 | 4800±10% | ≤25Ω | 78*90 | 60w | ≥100MΩ |
ARS-4QXHNQ-20K50W | 20±0.5 | 4000±10% | ≤25Ω | 57*94 | 50w | ≥100MΩ |
ARS-8QXHNQ-20K70W | 20±0.5 | 3250±10% | ≤20Ω | 78*94 | 70w | ≥100MΩ |
ARS-4QXHNQ-20K100W | 20±0.5 | 7600±10% | ≤20Ω | 67*92 | 100w | ≥100MΩ |
ARS-8QXHNQ-20K100W | 20±0.5 | 4500±10% | ≤20Ω | 67*92 | 100w | ≥100MΩ |
ARS-8QXHNQ-20K120W | 20±0.5 | 4650±10% | ≤25Ω | 79*94 | 120w | ≥100MΩ |
ARS-4QXHNQ-25K60W | 25±0.8 | 4800±10% | ≤20Ω | 59*80 | 60w | ≥100MΩ |
ARS-4QXHNQ-25K100W | 25±0.5 | 7600±10% | ≤20Ω | 67*76 | 100w | ≥100MΩ |
ARS-4QXHNQ-28K50WN | 28 ±0.5 | 4000±10% | ≤20Ω | 45*79 | 50w | ≥100MΩ |
ARS-4QXHNQ-28K60W | 28±0.5 | 4800±10% | ≤20Ω | 59*68 | 60w | ≥100MΩ |
ARS-4QXHNQ-28K100W | 28±0.5 | 7600±10% | ≤20Ω | 67*68 | 100w | ≥100MΩ |
ARS-8QXHNQ-28K100W | 28±0.5 | 5800±10% | ≤20Ω | 67*68 | 100w | ≥100MΩ |
ARS-4QXHNQ-28K120W | 28±0.5 | 9600±10% | ≤20Ω | 67*68 | 120w | ≥100MΩ |
ARS-8QXHNQ-28K120W | 28±0.5 | 6500±10% | ≤20Ω | 67*68 | 120w | ≥100MΩ |
ARS-4QXHNQ-33K60W | 33±0.5 | 4800±10% | ≤20Ω | 48*62 | 60w | ≥100MΩ |
ARS-8QXHNQ-33K60W | 33±0.5 | 3750±10% | ≤20Ω | 48*62 | 60w | ≥100MΩ |
ARS-4QXHNQ-35K60W | 35±0.5 | 4800±10% | ≤20Ω | 45*55 | 60w | ≥100MΩ |
ARS-4QXHNQ-40K30W | 40±0.8 | 2400±10% | ≤30Ω | 30*50 | 30w | ≥100MΩ |
ARS-4QXHNQ-40K50W | 40 ±1.0 | 4000±10% | ≤20Ω | 45*55 | 50w | ≥100MΩ |
ARS-4QXHNQ-40K50WN | 40 ±1.0 | 4000±10% | ≤20Ω | 45*53 | 50w | ≥100MΩ |
ARS-8QXHNQ-40K50WN | 40 ±1.0 | 3250±10% | ≤20Ω | 45*53 | 50w | ≥100MΩ |
ARS-4QXHNQ-40K60W | 40±0.5 | 4800±10% | ≤20Ω | 48*52 | 60w | ≥100MΩ |
ARS-8QXHNQ-40K60WN | 40±0.5 | 3850±10% | ≤20Ω | 48*50 | 60w | ≥100MΩ |
ARS-4QXHNQ-40K100W | 40±0.5 | 7600±10% | ≤20Ω | 55*53 | 100w | ≥100MΩ |
ARS-4QXHNQ-54K35W | 54±1.0 | 3100±10% | ≤35Ω | 30*42 | 35w | ≥100MΩ |
ARS-4QXHNQ-60K20W | 60±1.5 | 2300±10% | ≤35Ω | 30*35 | 20w | ≥100MΩ |
ARS-4QXHNQ-65K20W | 65±1.5 | 2300±10% | ≤35Ω | 25*31 | 20w | ≥100MΩ |
ARS-4QXHNQ-68K50W | 68±2.0 | 4800±10% | ≤20Ω | 50*65 | 50w | ≥100MΩ |
ARS-4QXHNQ-80K60W | 80±1.5 | 4800±10% | ≤25Ω | 40*54 | 60w | ≥100MΩ |
ARS-4QXHNQ-100K60W | 100±1.5 | 4800±10% | ≤25Ω | 40*57 | 60w | ≥100MΩ |
ARS-4QXHNQ-120K60W | 120±1.5 | 4800±10% | ≤25Ω | 40*58 | 60w | ≥100MΩ |
ARS-4QXHNQ-130K50W | 130±1.5 | 4200±10% | ≤25Ω | 36*54 | 50w | ≥100MΩ |
ARS-4QXHNQ-160K50W | 160±1.5 | 4800±10% | ≤25Ω | 40*57 | 60w | ≥100MΩ |
ARS-4QXHNQ-165K40W | 165±5.0 | 4100±10% | ≤60Ω | 42*61 | 40w | ≥100MΩ |
ARS-4QXHNQ-200K20W | 200±2.0 | 2300±10% | ≤35Ω | 30*35 | 20w | ≥100MΩ |
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