Figure 3-11 UNITS Function..........................................3-12
Figure 3-12 RANGE Function....................................... 3-14
Figure 3-13 HOLD Function.......................................... 3-16
Figure 3-14 Automatic ZERO Function......................... 3-19
Figure 3-15 Manual ZERO Function..............................3-21
Figure 3-16 Probe Output versus Flux Angle................ 3-23
Figure 3-17 Probe Output versus Distance................... 3-23
Figure 3-18 Flux Density Variations in a Magnet...........3-24
Figure 3-19 Low AC Signal Indication........................... 3-25
ii
Section 1
Introduction
UNDERSTANDING FLUX DENSITY
Magnetic fields surrounding permanent magnets or electrical
conductors can be visualized as a collection of magnetic flux
lines; lines of force existing in the material that is being subjected
to a magnetizing influence. Unlike light, which travels away from
its source indefinitely, magnetic flux lines must eventually return
to the source. Thus all magnetic sources are said to have two
poles. Flux lines are said to emanate from the “north” pole and
return to the “south” pole, as depicted in Figure 1-1.
Figure 1-1
Flux Lines of a Permanent Magnet
One line of flux in the CGS measurement system is called a
maxwell (M
commonly used.
Flux density, also called magnetic induction, is the number of flux
lines passing through a given area. It is commonly assigned the
symbol “B” in scientific documents. In the CGS system a gauss
(G) is one line of flux passing through a 1 cm
), but the weber (Wb), which is 108 lines, is more
x
2
area. The more
1-1
INTRODUCTION
commonly used term is the tesla (T), which is 10,000 lines per
2
. Thus
cm
1 tesla = 10,000 gauss
1 gauss = 0.0001 tesla
Magnetic field strength is a measure of force produced by an
electric current or a permanent magnet. It is the ability to induce
a magnetic field “B”. It is commonly assigned the symbol “H” in
scientific documents. The unit of “H” in the CGS system is an
oersted (Oe), but the ampere/meter (A/m) is more commonly
used. The relationship is
1 oersted = 79.6 ampere/meter
1 ampere/meter = 0.01256 oersted
It is important to know that magnetic field strength and magnetic
flux density are not
the same. The only time the two are
considered equal is in free space (air). Only in free space is the
following relationship true:
1 G = 1 Oe = 0.0001 T = 79.6 A/m
MEASUREMENT OF FLUX DENSITY
A device commonly used to measure flux density is the Hall
generator. A Hall generator is a thin slice of a semiconductor
material to which four leads are attached at the midpoint of each
edge, as shown in Figure 1-2.
1-2
INTRODUCTION
Figure 1-2
Hall Generator
A constant current (Ic) is forced through the material. In a zero
magnetic field there is no voltage difference between the other
two edges. When flux lines pass through the material the path of
the current bends closer to one edge, creating a voltage
difference known as the Hall voltage (Vh). In an ideal Hall
generator there is a linear relationship between the number of
flux lines passing through the material (flux density) and the Hall
voltage.
The Hall voltage is also a function of the direction in which the
flux lines pass through the material, producing a positive voltage
in one direction and a negative voltage in the other. If the same
number of flux lines pass through the material in either direction,
the net result is zero volts. This sensitivity to flux direction makes
it possible to measure both static (dc) and alternating (ac)
magnetic fields.
The Hall voltage is also a function of the angle at which the flux
lines pass through the material. The greatest Hall voltage occurs
when the flux lines pass perpendicularly through the material.
Otherwise the output is related to the cosine of the difference
between 90° and the actual angle.
1-3
INTRODUCTION
The sensitive area of the Hall generator is generally defined as
the largest circular area within the actual slice of the material.
This active area can range in size from 0.2 mm (0.008”) to 19
mm (0.75”) in diameter. Often the Hall generator assembly is too
fragile to use by itself so it is often mounted in a protective tube
and terminated with a flexible cable and a connector. This
assembly, known as a Hall probe, is generally provided in two
configurations:
Figure 1-3
Hall Probe Configurations
In “transverse” probes the Hall generator is mounted in a thin, flat
stem whereas in “axial” probes the Hall generator is mounted in a
cylindrical stem. The axis of sensitivity is the primary difference,
as shown by “B” in Figure 1-3. Generally transverse probes are
used to make measurements between two magnetic poles such
as those in audio speakers, electric motors and imaging
machines. Axial probes are often used to measure the magnetic
field along the axis of a coil, solenoid or traveling wave tube.
Either probe can be used where there are few physical space
limitations, such as in geomagnetic or electromagnetic
interference surveys.
1-4
INTRODUCTION
1-5
INTRODUCTION
Handle the Hall probe with care. Do not bend the stem or
apply pressure to the probe tip as damage may result. Use
the protective cover when the probe is not in use.
PRODUCT DESCRIPTION
The MODEL HHG-22 GAUSS / TESLAMETER is a portable
instrument that utilizes a Hall probe to measure magnetic flux
density in terms of gauss, tesla or ampere/meter. The
measurement range is from 0.01 mT (0.1 G or 0.01 kA/m) to
1.999T (19.99 kG or 1591 kA/m). The instrument is capable of
measuring static (dc) magnetic fields and alternating (ac) fields.
The MODEL HHG-22 consists of a palm-sized meter and various
detachable Hall probes. The meter operates on standard 9 volt
alkaline batteries or can be operated with an external ac-to-dc
power supply. A retractable bail allows the meter to stand upright
on a flat surface. A notch in the bail allows the meter to be wall
mounted when bench space is at a premium. The large display is
visible at considerable distances. The instrument is easily
configured using a single rotary selector and two pushbuttons.
Three measurement ranges can be selected or the meter can
automatically select the best range based on the present flux
density being measured. A “zero” function allows the user to
remove undesirable readings from nearby magnetic fields
(including earth’s) or false readings caused by initial electrical
offsets in the probe and meter. Included is a “zero flux chamber”
which allows the probe to be shielded from external magnetic
fields during this operation. The “zero” adjustment can be made
manually or automatically.
1-6
INTRODUCTION
Other features include two “hold” modes, allowing either the
arithmetic maximum or minimum values to be held indefinitely
until reset by the user.
The meter, probes and accessories are protected when not in
use by a sturdy carrying case.
APPLICATIONS
•Sorting or performing incoming inspection on permanent
magnets, particularly multi-pole magnets.
•
Testing audio speaker magnet assemblies, electric motor
armatures and stators, transformer lamination stacks,
cut toroidal cores, coils and solenoids.
•
Determining the location of stray fields around medical
diagnostic equipment.
•
Determining sources of electromagnetic interference.
•
Locating flaws in welded joints.
•
Inspection of ferrous materials.
•
3-dimensional field mapping.
•
Inspection of magnetic recording heads.
1-7
Section 2
Specifications
INSTRUMENT
RANGE RESOLUTION
gauss tesla A/m Gauss tesla A/m
200 G 20 mT 16 kA/m0.1 G0.01 mT0.01 kA/m
2 kG 200 mT 159 kA/m1 G0.1 mT0.1 kA/m
20 kG 2 T 1591 kA/m10 G1 mT1 kA/m
ACCURACY (including probe):
dc mode: ± 2 % of reading, ± 3 counts
ac mode:
20 - 10,000 Hz: ± 3.5 % of reading, ± 5 counts
ACCURACY CHANGE WITH
TEMPERATURE
(not including probe): ± 0.02 % / ºC typical
WARMUP TIME TO RATED
ACCURACY: 15 minutes
MIN / MAX HOLD ACQUISITION TIME:
dc mode:180 ms typical
ac mode: 300 ms typical
BATTERY TYPE: 9 Vdc alkaline (NEDA 1640A)
BATTERY LIFE: 8 hours typical (two batteries)
AUXILIARY POWER: 9 Vdc, 300 mA
2-1
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