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- Amplification rate: 50 times - Output range: -20V to +150V - Output average current: 2A - Example of drive targets: stacked piezoelectric actuators, bimorphs, unimorphs - Example of applications: punchers, precision stages, pumps, valves, precision grippers - Dimensions: W360 x D300 x H185mm - Power supply: AC100V - Output impedance: approximately 3Ω - Amplification bandwidth: DC to 70kHz (resistive load 100Ω, 100Vp-p output) - Input impedance: approximately 100KΩ - Waveform monitor: 1/10 output voltage waveform - Ripple noise: below 5mVp-p (bias point 100V, 3uF capacitive load)
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Free membership registration- Amplification rate: 15 times - Output range: 0V to +150V - Output average current: 0.7A - Example of drive targets: stacked piezoelectric actuators, bimorphs, unimorphs - Example of applications: punchers, precision stages, pumps, valves, precision grippers - Dimensions: W440 x D350 x H200mm - Power supply: AC100V - Output impedance: approximately 0Ω - Amplification degree: 15 times - Input trigger voltage: 0V to +24V (square wave) - Input impedance: 4.7KΩ
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Free membership registration- Amplification rate: 50 times (customizable) - Output range: 0V to +150V - Output average current: 3A - Examples of drive targets: stacked piezoelectric actuators, bimorphs, unimorphs - Examples of applications: punchers, precision stages, pumps, valves, precision grippers - Dimensions: W440 x D350 x H185 mm - Power supply: AC100V - Output waveform: DC to 70KHz (resistive load 200Ω 100Vp-p) - Output stability: 1×10^-4/H (typically after 1 hour) - Ripple noise: below 5mVp-p (with 3uF capacitive load) - Input voltage: ±3V max - Waveform monitor: 1/10 output voltage waveform Overview: This device is a high-precision, low-noise high-output DC amplifier designed to drive various electrostrictive elements that have capacitive loads. It can be used as the final stage amplifier in various control systems utilizing electrostrictive elements, responding quickly around the bias point. It is easy to handle; simply connect the piezo element load and apply a control signal to drive it with any desired waveform.
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Free membership registration- Amplification rate: 50 times (customizable) - Output range: 0V to +150V - Output average current: 2A - Example of drive targets: stacked piezoelectric actuators, bimorphs, unimorphs - Example of applications: punchers, precision stages, pumps, valves, precision grippers - Dimensions: W360 x D300 x H185 mm - Power supply: AC100V - Output waveform: DC to 70KHz (resistive load 200Ω 100Vp-p) - Output stability: 1×10^-4/H (usually after 1 hour) - Ripple noise: 5mVp-p or less (with 3uF capacitive load) - Input voltage: ±3V max - Waveform monitor: 1/10 output voltage waveform Overview: This device is a high-precision, low-noise high-output DC amplifier designed to drive various electrostrictive elements that have capacitive loads. It can be used as a final stage amplifier in various control systems utilizing electrostrictive elements, responding quickly around the bias point. It is easy to handle; simply connect the piezo element load, apply a control signal, and drive it with any desired waveform.
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Free membership registration- Amplification rate: 50 times (customizable) - Output range: -20V to +150V - Output average current: 2A - Example of drive targets: stacked piezoelectric actuators, bimorphs, unimorphs - Example of applications: punchers, precision stages, pumps, valves, precision grippers - Dimensions: W360 x D300 x H185 mm - Power supply: AC100V Operation description: This device uses a MOS-type FET in the output stage to form a quasi-complementary amplifier, achieving stabilization of amplification and low noise wideband characteristics through a negative feedback circuit. The input signal is buffered and enters the gain adjuster for gain setting. Meanwhile, the bias voltage generated by a temperature-compensated reference voltage generator can be set to an arbitrary value using a bias voltage adjuster and is added to the aforementioned signal before entering the output amplifier. The output amplification section receives the input signal through an operational amplifier, and to achieve high output, four MOS-type FETs are connected in parallel, further reducing impedance through a quasi-complementary circuit. Negative feedback is achieved by returning an inverted signal to the operational amplifier in the input section, and the output terminal is designed to cut off the output in case of overcurrent protection.
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Free membership registration- Amplification rate: 50 times - Voltage output range: 0V to +150V - Output average current: 1A - Drive targets: stacked piezoelectric actuators, bimorphs, unimorphs - Dimensions: W145 x D325 x H125 mm - Power supply: AC 100V 50/60Hz or AC 230V 50/60Hz
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Free membership registration- Amplification rate: 15 times - Voltage output range: 0V to +150 - Output average current: 100mA - Drive targets: stacked piezoelectric actuators, bimorphs, unimorphs - Dimensions: 53 x 220 x 124 mm - Power supply: AC100V
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Free membership registration- High-speed response (for piezoelectric elements in standalone or external mechanism connection: both at one-third of the resonance frequency) - Conversion efficiency from electrical energy to mechanical energy (approximately 60%) - High generated mechanical energy per unit volume (about 20 mJ per cm³) - Large generated force (approximately 3500 N per cm²) - Optimal as an energy source for displacement amplification mechanisms - High positioning resolution - Low driving voltage, easy to use
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Free membership registrationThe pressure-driven piezoelectric actuator is a frame-integrated piezoelectric actuator that incorporates piezoelectric elements within a frame (pressure case). It is possible to create piezo actuators that meet your desired output force and displacement by combining the pressure case with piezoelectric elements of various standard sizes. Additionally, the pressure case complements the piezoelectric element's weakness to tension, making it a durable piezoelectric actuator.
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Free membership registration1. High energy efficiency It is characterized by a very high efficiency of about 25% in converting electrical energy to mechanical energy. Additionally, to maintain a certain displacement state, it is sufficient to maintain a specified applied voltage, and the current when maintaining the voltage is effectively zero. 2. Capable of high-speed operation In general, it can operate at high speeds compared to actuators that utilize electromagnetic attraction. For the driving limit, which is the resonance frequency, please refer to the technical note "Operation under dynamic load." 3. Possible miniaturization and thinness Compared to actuators that utilize electromagnetic attraction to generate equivalent displacement and force, it is possible to achieve miniaturization, especially in terms of thickness. 4. Good controllability Since the relationship between voltage and displacement is almost proportional, it is possible to obtain a specified displacement through voltage control. However, due to the presence of hysteresis, the displacement generated at the same applied voltage will not be the same with changes in voltage (rise and fall), so a displacement sensor is necessary when precise displacement generation is required.
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Free membership registrationThe Mechatron MTK series is a piezo actuator that emphasizes high rigidity and fast response time. During the operation of the displacement amplification mechanism, the piezoelectric elements do not involve positional movement compared to the MTDD series and MTD series, so the inertial mass of the piezoelectric elements does not hinder rapid startup motion. In the Mechatron MTK series, not only does the operation of displacement amplification not involve positional movement of the piezoelectric elements, but it also maintains the characteristics of being flat and thin. When a voltage is applied, this piezo actuator operates in the direction of contraction. The main features are as follows.
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Free membership registrationThe Mechatron MTKK series is a piezo actuator that emphasizes high rigidity and fast response time. Unlike the MTDD and MTD series, the piezo elements in this series do not involve positional movement during the operation of the displacement amplification mechanism, which means that the inertial mass of the piezo elements does not hinder rapid startup motion. The Mechatron MTKK series not only does not involve positional movement of the piezo elements during displacement amplification but also maintains a flat and thin structure. When voltage is applied, this piezo actuator operates in the direction of elongation. The main features are as follows: 【Features】 ■ High resonance frequency ranging from 1.6 to 6.5 kHz. ■ High generated force ranging from 20N to 140N. ■ Flat and thin shape suitable for compact device design. ■ The direction of generated displacement of the actuator is perpendicular to the displacement direction of the piezo elements by 90 degrees. ■ It elongates with the increase in applied voltage. ■ Ideal for applications that require particularly fast response speeds. ■ The direction of generated displacement is opposite to that of the MTK series. *For more details, please download the catalog or contact us directly.
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Free membership registrationThe MechaTrans MTD series is a piezo actuator that can generate large displacements in a compact size. It amplifies the displacement generated by the piezoelectric element by more than ten times, effectively resolving the actuator's displacement shortfall. Additionally, its flat and thin shape makes it advantageous for installation in small spaces. The displacement amplification mechanism minimizes wasted space, resulting in very high space utilization efficiency. The direction of the generated displacement is converted 90 degrees from the displacement direction of the piezoelectric element, making it easy to arrange for use. When a voltage is applied, this piezo actuator operates in the direction of contraction.
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Free membership registrationThe MechaTrans MTDD series is a piezo actuator that can generate large displacements in a compact size. It amplifies the displacement generated by the piezoelectric element by more than ten times, effectively resolving the issue of insufficient displacement in the actuator. Additionally, its flat and slim design makes it advantageous for installation in small spaces. The displacement amplification mechanism minimizes wasted space, resulting in very high space utilization efficiency. The direction of the generated displacement is converted 90 degrees from the displacement direction of the piezoelectric element, making it easy to arrange for use. When a voltage is applied, this piezo actuator operates in the direction of elongation.
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Free membership registrationUtilizing the numerous advantages of piezoelectric methods, we achieve high-speed, large-displacement actuators that can amplify small displacements by several to tens of times! 【Features】 ○ Mechanically amplifies and reduces the displacement generated by piezoelectric actuator elements ○ The efficiency of converting electrical energy to mechanical energy is very high at approximately 25% ○ To maintain the displacement state, only a specified applied voltage needs to be maintained, with the current effectively being zero when the voltage is held ○ Generally capable of operating at high speeds compared to actuators that utilize electromagnetic attraction ○ Can be miniaturized, especially in terms of thickness, compared to actuators that utilize electromagnetic attraction to generate equivalent displacement and force ○ Controllable *For more details, please contact us.
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