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The KJT F58S series Hall-Effect Zero-Speed sensors are suitable, in conjunction with a ferrous pole wheel, for generating square wave signals proportional to rotary speeds. The F58S exhibits a static function, whereby pulse generation down to 0 Hz is guaranteed. The sensor function is independent of the rotational mounting angle.

The KJT-F58A40-LY series Hall-Effect Zero-Speed sensors are suitable, in conjunction with a ferrous pole wheel, for generating square wave signals proportional to rotary speeds. The F58A40 exhibits a static function, whereby pulse generation down to 0 Hz is guaranteed. The sensor function is independent of the rotational mounting angle.

The KJT-F58A25 series Hall-Effect Zero-Speed sensors are suitable, in conjunction with a ferrous pole wheel, for generating square wave signals proportional to rotary speeds. The F58A25 exhibits a static function, whereby pulse generation down to 0 Hz is guaranteed. The sensor function is independent of the rotational mounting angle.

The KJT-F58A series Hall-Effect Zero-Speed sensors are suitable, in conjunction with a ferrous pole wheel, for generating square wave signals proportional to rotary speeds. The F58A exhibits a static function, whereby pulse generation down to 0 Hz is guaranteed. The sensor function is independent of the rotational mounting angle.

The KJT F16S40 series Hall-Effect Zero-Speed sensors are suitable, in conjunction with a ferrous pole wheel, for generating square wave signals proportional to rotary speeds. The F16S40 exhibits a static function, whereby pulse generation down to 0 Hz is guaranteed. The sensor function is independent of the rotational mounting angle.

The KJT-F16S25 series Hall-Effect Zero-Speed sensors are suitable, in conjunction with a ferrous pole wheel, for generating square wave signals proportional to rotary speeds. The F16S25 exhibits a static function, whereby pulse generation down to 0 Hz is guaranteed. The sensor function is independent of the rotational mounting angle.

The Jaquet F16S series Hall-Effect Zero-Speed sensors are suitable, in conjunction with a ferrous pole wheel, for generating square wave signals proportional to rotary speeds. The F16S exhibits a static function, whereby pulse generation down to 0 Hz is guaranteed. The sensor function is independent of the rotational mounting angle.

The KJT-F16A25 series Hall-Effect Zero-Speed sensors are suitable, in conjunction with a ferrous pole wheel, for generating square wave signals proportional to rotary speeds. The F16A25 exhibits a static function, whereby pulse generation down to 0 Hz is guaranteed. The sensor function is independent of the rotational mounting angle.

The KJT-F16A-LY series Hall-Effect Zero-Speed sensors are suitable, in conjunction with a ferrous pole wheel, for generating square wave signals proportional to rotary speeds. The F16A exhibits a static function, whereby pulse generation down to 0 Hz is guaranteed. The sensor function is independent of the rotational mounting angle.

The KJT-F12S-LY series Hall-Effect Zero-Speed sensors are suitable, in conjunction with a ferrous pole wheel, for generating square wave signals proportional to rotary speeds. The F12S exhibits a static function, whereby pulse generation down to 0 Hz is guaranteed. The sensor function is independent of the rotational mounting angle.

The KJT-F12A series Hall-Effect Zero-Speed sensors are suitable, in conjunction with a ferrous pole wheel, for generating square wave signals proportional to rotary speeds. The F12A exhibits a static function, whereby pulse generation down to 0 Hz is guaranteed. The sensor function is independent of the rotational mounting angle.

The KJT EX58S40 series Variable Reluctance Speed (VRS) sensors consist of an iron core, an inductive coil and a permanent magnet. A ferrous pole wheel passing the sensor face changes the magnetic field strength, resulting in an AC Voltage being induced in the coil. The frequency of the output signal is proportional to the speed of the moving target. The amplitude of the signal depends on speed, air gap, geometry of the target, magnetic properties of the target material and the electrical load. VRS sensors, also known as passive or electromagnetic sensors, do not require an external supply.

The KJT EX58S25 series Variable Reluctance Speed (VRS) sensors consist of an iron core, an inductive coil and a permanent magnet. A ferrous pole wheel passing the sensor face changes the magnetic field strength, resulting in an AC Voltage being induced in the coil. The frequency of the output signal is proportional to the speed of the moving target. The amplitude of the signal depends on speed, air gap, geometry of the target, magnetic properties of the target material and the electrical load. VRS sensors, also known as passive or electromagnetic sensors, do not require an external supply. The EX58S25 is specifically designed for use in explosive atmospheres.

The KJT-EX58H35-LY series Variable Reluctance Speed (VRS) sensors consist of an iron core, an inductive coil and a permanent magnet. A ferrous pole wheel passing the sensor face changes the magnetic field strength, resulting in an AC Voltage being induced in the coil. The frequency of the output signal is proportional to the speed of the moving target. The amplitude of the signal depends on speed, air gap, geometry of the target, magnetic properties of the target material and the electrical load. VRS sensors, also known as passive or electromagnetic sensors, do not require an external supply. The EX58H35 is specifically designed for use in explosive atmospheres.

The KJTDQ-EX58H-LY series Variable Reluctance Speed (VRS) sensors consist of an iron core, an inductive coil and a permanent magnet. A ferrous pole wheel passing the sensor face changes the magnetic field strength, resulting in an AC Voltage being induced in the coil. The frequency of the output signal is proportional to the speed of the moving target. The amplitude of the signal depends on speed, air gap, geometry of the target, magnetic properties of the target material and the electrical load. VRS sensors, also known as passive or electromagnetic sensors, do not require an external supply. The EX58H is specifically designed for use in explosive atmospheres.

The KJT-EX58AM40-LY series Variable Reluctance Speed (VRS) sensors consist of an iron core, an inductive coil and a permanent magnet. A ferrous pole wheel passing the sensor face changes the magnetic field strength, resulting in an AC Voltage being induced in the coil. The frequency of the output signal is proportional to the speed of the moving target. The amplitude of the signal depends on speed, air gap, geometry of the target, magnetic properties of the target material and the electrical load. VRS sensors, also known as passive or electromagnetic sensors, do not require an external supply. The EX58AM40 is specifically designed for use in explosive atmospheres.

The KJT EX58AM25 series Variable Reluctance Speed (VRS) sensors consist of an iron core, an inductive coil and a permanent magnet. A ferrous pole wheel passing the sensor face changes the magnetic field strength, resulting in an AC Voltage being induced in the coil. The frequency of the output signal is proportional to the speed of the moving target. The amplitude of the signal depends on speed, air gap, geometry of the target, magnetic properties of the target material and the electrical load. VRS sensors, also known as passive or electromagnetic sensors, do not require an external supply. The EX58AM25 is specifically designed for use in explosive atmospheres.

The KJT-EX58AM-LY series Variable Reluctance Speed (VRS) sensors consist of an iron core, an inductive coil and a permanent magnet. A ferrous pole wheel passing the sensor face changes the magnetic field strength, resulting in an AC Voltage being induced in the coil. The frequency of the output signal is proportional to the speed of the moving target. The amplitude of the signal depends on speed, air gap, geometry of the target, magnetic properties of the target material and the electrical load. VRS sensors, also known as passive or electromagnetic sensors, do not require an external supply. The EX58AM is specifically designed for use in explosive atmospheres.

The KJT-EX38S-LY series Variable Reluctance Speed (VRS) sensors consist of an iron core, an inductive coil and a permanent magnet. A ferrous pole wheel passing the sensor face changes the magnetic field strength, resulting in an AC Voltage being induced in the coil. The frequency of the output signal is proportional to the speed of the moving target. The amplitude of the signal depends on speed, air gap, geometry of the target, magnetic properties of the target material and the electrical load. VRS sensors, also known as passive or electromagnetic sensors, do not require an external supply. The EX38S is specifically designed for use in explosive atmospheres.