MagTest System

The MagTest System is a system to generate magnetic fields and to perform tests regarding the susceptibility against magnetic fields in accordance to military, civil, automotive and manufacturer’s standards.

At least the system consists of a function generator as signal source, a power amplifier and a radiating loop or Helmholtz coil.

The generated fields are in a linear relation to the coil current. The coil current is measured by an rms-voltmeter and a shunt or a current probe. The magnetic field strength can be checked with a monitoring loop and a rms-voltmeter.

To fulfil highest requirements on large Helmholtz-coils a compensation network is needed. It compensates the reactance of the coil with capacitors.

With the Schwarzbeck Magtest System Software AC immunity testing is fully automatized.
Overview MagTest System combinations for immunity testing
MagTest System Description

SW 9605 - Current Clamp was designed to measure RF-currents.

SW 9605 – Current Clamp

Insertion Loss in 50 Ω System: 34 dB

The SW 9605 Current Clamp was designed to measure RF-currents on conductors or conductor bundles with a maximum diameter of 23 mm. The conversion ratio is 1:1 in the nominal frequency range, therefore the receiver-reading in dBµV corresponds directly to the current in dBµA.

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SHUNT 9571 - High power shunt resistor with low inductance.

SHUNT 9571 – Measuring Resistor

Frequency range (nominal): DC – 250 kHz

The SHUNT 9571 is a measuring resistor which can be used in systems where magnetic fields have to be generated. When connected in series between an amplifier and a Helmholtz coil, the current can be measured indirectly. The voltage drop is proportional to the current through the coil.

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Measuring Resistor 0.5 Ohm - High power resistor with low inductance.

Resistor 0.5 Ohm – Measuring Resistor 0.5 Ohm

Resistance: 500 mΩ

High power resistor with low inductance, which can be used in systems where magnetic fields have to be gener-ated. When connected in series between an amplifier and a Helmholtz coil, the current can be measured indirectly. The voltage drop is proportional to the current through the coil. It can be used for testing according to MIL STD 461 (CS101) and ISO 11452 10.

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HHS 5206 – Circular Helmholtz Coils

HHS 5206-4 – Circular Helmholtz Coils

  • Number of turns: 4
  • Frequency Range: DC - 1.5 MHz
  • Coil Shape: Circular
  • Nominal Coil Current (continuous): 34 A
  • Maximum Coil Current (5 min.): 55 A
  • Magnetic Field Strength Nominal (continuos): 330 A/m
  • Magnetic Field Strength Maximum (5 min.): 530 A/m
  • Magnetic field strength at 1 A Coil Current: 9.64 A/m; 139.68 dBµA/m
  • Diameter/Side: 0.584 m
  • Resonance Frequency (pair of coils): 3000 kHz
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HHS 5205-1 - Circular Helmholtz Coils

HHS 5205-1 – Circular Helmholtz Coils

  • Number of turns: 1
  • Frequency Range: DC - 30 MHz
  • Coil Shape: Circular
  • Nominal Coil Current (continuous): 15 A
  • Maximum Coil Current (5 min.): 20 A
  • Magnetic Field Strength Nominal (continuos): 14.3 A/m
  • Magnetic Field Strength Maximum (5 min.): 28.6 A/m
  • Magnetic field strength at 1 A Coil Current: 1.43 A/m; 123.11 dBµA/m
  • Diameter/Side: 0.5 m
  • Resonance Frequency (pair of coils): 44000 kHz
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HHS 5206 – Circular Helmholtz Coils

HHS 5206-132 – Circular Helmholtz Coil

  • Number of turns: 132
  • Frequency Range: DC - 30 kHz
  • Coil Shape: Circular
  • Nominal Coil Current (continuous): 10 A
  • Maximum Coil Current (5 min.): 15 A
  • Magnetic Field Strength Nominal (continuos): 3142 A/m
  • Magnetic Field Strength Maximum (5 min.): 4713 A/m
  • Magnetic field strength at 1 A Coil Current: 314.2 A/m; 169.97 dBµA/m
  • Diameter/Side: 0.6 m
  • Resonance Frequency (pair of coils): 50 kHz
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Schwarzbeck FESP 5133-9 - Circular Screened Coil

FESP 5133-9 – Circular Screened Coil

Usable Frequency Range: 10 kHz - 3 MHz

The magnetic, handheld coil FESP 5133 was designed to generate defined magnetic field strength in the audio frequency range up to 3 MHz. The main application is immunity testing against magnetic fields according to VG 95377 Part 13 and many others. Depending on the current source characteristics magnetic fields up to 400 A/m can be generated for a short time.

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HHS 5206 – Circular Helmholtz Coils

HHS 5206-16 – Circular Helmholtz Coils

  • Number of turns: 16
  • Frequency Range: DC - 500 kHz
  • Coil Shape: Circular
  • Nominal Coil Current (continuous): 33 A
  • Maximum Coil Current (5 min.): 55 A
  • Magnetic Field Strength Nominal (continuos): 1260 A/m
  • Magnetic Field Strength Maximum (5 min.): 2100 A/m
  • Magnetic field strength at 1 A Coil Current: 38.17 A/m; 151.63 dBµA/m
  • Diameter/Side: 0.6 m
  • Resonance Frequency (pair of coils): 700 kHz
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HHS 5204-36

HHS 5204-12 – Circular Helmholtz Coils

  • Number of turns: 12
  • Frequency Range: DC - 500 kHz
  • Coil Shape: Circular
  • Nominal Coil Current (continuous): 30 A
  • Maximum Coil Current (5 min.): 60 A
  • Magnetic Field Strength Nominal (continuos): 1288 A/m
  • Magnetic Field Strength Maximum (5 min.): 2500 A/m
  • Magnetic field strength at 1 A Coil Current: 42.93 A/m; 152.66 dBµA/m
  • Diameter/Side: 0.4 m
  • Resonance Frequency (pair of coils): 1400 kHz
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Schwarzbeck FESP 5133-1330 Circular Radiating Loop

FESP 5133-1330 – Circular Coil

Usable Frequency Range: 0 – 20 (50) kHz

The handheld coil FESP 5133-1330 was designed for immunity testing against magnetic fields up to approx. 20 kHz. The coil has 225 turns of Cu-wire on 15 layers. There are spacers to provide a constant distance of 50 mm between coil center and EuT-surface. The generated magnetic fieldstrength is direct proportional to the coil current. Typical applications are Immunity Tests according to the Measuring Method SF 01 G acc. to VG 95377 standard.

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FESP 5132 - Magnetic Handheld Coil

FESP 5132 – Radiating Loop

Usable Frequency Range: 0 – 150 kHz

The magnetic, handheld coil FESP 5132 was designed to generate defined magnetic fieldstrength in the audio frequency range up to 100 kHz. The main application is immunity testing against magnetic fields according to EN 55103 and MIL-STD-461 G. Depending on the current source characteristics magnetic fields up to 1500 A/m can be generated for a short time.

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