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MW 12x1 zestaw 1400 szt. / N38 - cylindrical magnet

cylindrical magnet

Catalog no 010560

GTIN/EAN: 5906301815525

Load capacity 0.42 kg / 4.15 N Magnetic Induction 101.90 mT / 1019 Gs
Diameter Ø
12 mm [±0,1 mm]
Height
1 mm [±0,1 mm]
Weight
1190 g
Magnetization Direction
↑ axial
Coating
[NiCuNi] Nickel

How we measure these parameters — certificates and measurements

technical details »

591.87 zł net / pcs

728.00 zł with VAT (23% VAT) / pcs

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Frequently asked questions

Where can I buy strong cylindrical neodymium magnets?
See the available cylinders in the DHIT catalogue. Compare dimensions, grade and the pull-force value on each product card; grade alone does not determine the pull force of a finished magnet.
Can a small cylindrical magnet provide a strong grip for precise workshop work?
Yes, but size alone is not enough to predict the result. Geometry, the steel surface and the direction of load affect the grip. Compare the specifications of the selected dimensions on their product cards.
Which cylindrical magnet can work at a higher temperature?
Check the operating-temperature limit of the particular model rather than assuming one limit for all N grades. The offered N52 models are rated up to 60°C. For hotter applications, ask for a product with a confirmed specification for the actual working temperature.

Guides from the knowledge base

Engineering report for this magnet

Full PDF analysis: pull and shear force, effect of distance, temperature and plate thickness, safety distances and the demagnetization curve.

PDF report Calculator
Want to talk magnets?

Call us now +48 888 99 98 98 alternatively let us know using contact form the contact section.
Specifications and structure of a neodymium magnet can be estimated using our power calculator.

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Detailed specification - MW 12x1 zestaw 1400 szt. / N38 - cylindrical magnet

Specification / characteristics - MW 12x1 zestaw 1400 szt. / N38 - cylindrical magnet

properties
properties values
Cat. no. 010560
GTIN/EAN 5906301815525
Distributor Dhit sp. z o.o.
Country of origin Poland / China / Germany
Customs code 85059029
Diameter Ø 12 mm [±0,1 mm]
Height 1 mm [±0,1 mm]
Weight 1190 g
Magnetization Direction ↑ axial
Load capacity ~ ? 0.42 kg / 4.15 N
Magnetic Induction ~ ? 101.90 mT / 1019 Gs
Coating [NiCuNi] Nickel
Manufacturing Tolerance ±0.1 mm

Magnetic properties of material N38

Specification / characteristics MW 12x1 zestaw 1400 szt. / N38 - cylindrical magnet
properties values units
Remanence Br ? 12.2-12.6 kGs
Remanence Br ? 1220-1260 mT
Coercivity bHc ? 10.8-11.5 kOe
Coercivity bHc ? 860-915 kA/m
Intrinsic coercivity iHc ≥ 12 kOe
Intrinsic coercivity iHc ≥ 955 kA/m
Energy product BHmax ? 36-38 BH max MGOe
Energy product BHmax ? 287-303 BH max KJ/m
Maximum working temperature ? ≤ 80 °C

Physical properties of sintered neodymium magnets Nd2Fe14B at 20°C

Physical properties of sintered neodymium magnets Nd2Fe14B at 20°C
properties values units
Vickers hardness ≥550 Hv
Density ≥7.4 g/cm3
Curie Temperature TC 310 °C
Curie Temperature TF 590 °F
Specific resistance 150 μΩ⋅cm
Bending strength 250 MPa
Compressive strength 1000~1100 MPa
Thermal expansion parallel (∥) to orientation (M) (3-4) x 10-6 °C-1
Thermal expansion perpendicular (⊥) to orientation (M) -(1-3) x 10-6 °C-1
Young's modulus 1.7 x 104 kg/mm²

Physical simulation of the magnet - data

These values are the result of a mathematical simulation. Results are based on models for the material Nd2Fe14B. Real-world performance may deviate from the simulation results. Please consider these data as a preliminary roadmap for designers.

Table 1: Static pull force (force vs gap) - power drop
MW 12x1 zestaw 1400 szt. / N38

Distance (mm) Induction (Gauss) / mT Pull Force (kg/lbs/g/N) Risk Status
0 mm 1019 Gs
101.9 mT
 0.42 kg / 0.93 pounds
420.0 g / 4.1 N
 low risk
1 mm 941 Gs
94.1 mT
 0.36 kg / 0.79 pounds
358.5 g / 3.5 N
 low risk
2 mm 812 Gs
81.2 mT
 0.27 kg / 0.59 pounds
266.8 g / 2.6 N
 low risk
3 mm 666 Gs
66.6 mT
 0.18 kg / 0.40 pounds
179.7 g / 1.8 N
 low risk
5 mm 415 Gs
41.5 mT
 0.07 kg / 0.15 pounds
69.7 g / 0.7 N
 low risk
10 mm 126 Gs
12.6 mT
 0.01 kg / 0.01 pounds
6.5 g / 0.1 N
 low risk
15 mm 49 Gs
4.9 mT
 0.00 kg / 0.00 pounds
1.0 g / 0.0 N
 low risk
20 mm 23 Gs
2.3 mT
 0.00 kg / 0.00 pounds
0.2 g / 0.0 N
 low risk
30 mm 7 Gs
0.7 mT
 0.00 kg / 0.00 pounds
0.0 g / 0.0 N
 low risk
50 mm 2 Gs
0.2 mT
 0.00 kg / 0.00 pounds
0.0 g / 0.0 N
 low risk
Magnetic force weakens sharply with every subsequent millimeter of spacing. Keep in mind that every additional insulation layer (e.g., contamination, varnish, dust) strongly reduces the pull force. Neodymiums hold most effectively in perfect adhesion; distance weakens the force. Notice how quickly the load capacity plummet, when the magnet does not touch flatly to the steel surface. When designing the mounting, avoid unnecessary gaps.

Table 2: Slippage force (wall)
MW 12x1 zestaw 1400 szt. / N38

Distance (mm) Friction coefficient Pull Force (kg/lbs/g/N)
0 mm Raw steel (µ ≈ 0.2) 0.08 kg / 0.19 pounds
84.0 g / 0.8 N
1 mm Raw steel (µ ≈ 0.2) 0.07 kg / 0.16 pounds
72.0 g / 0.7 N
2 mm Raw steel (µ ≈ 0.2) 0.05 kg / 0.12 pounds
54.0 g / 0.5 N
3 mm Raw steel (µ ≈ 0.2) 0.04 kg / 0.08 pounds
36.0 g / 0.4 N
5 mm Raw steel (µ ≈ 0.2) 0.01 kg / 0.03 pounds
14.0 g / 0.1 N
10 mm Raw steel (µ ≈ 0.2) 0.00 kg / 0.00 pounds
2.0 g / 0.0 N
15 mm Raw steel (µ ≈ 0.2) 0.00 kg / 0.00 pounds
0.0 g / 0.0 N
20 mm Raw steel (µ ≈ 0.2) 0.00 kg / 0.00 pounds
0.0 g / 0.0 N
30 mm Raw steel (µ ≈ 0.2) 0.00 kg / 0.00 pounds
0.0 g / 0.0 N
50 mm Raw steel (µ ≈ 0.2) 0.00 kg / 0.00 pounds
0.0 g / 0.0 N
The table below presents the estimated weight limit needed to cause the slippage of the magnet vertically against a upright metal surface (considering standard friction). This parameter is relative to the air gap between the magnet and the surface.

Table 3: Wall mounting (sliding) - behavior on slippery surfaces
MW 12x1 zestaw 1400 szt. / N38

Surface type Friction coefficient / % Max load (kg/lbs/g/N)
Raw steel
µ = 0.3 30% of nominal force
0.13 kg / 0.28 pounds
126.0 g / 1.2 N
Painted steel (standard)
µ = 0.2 20% of nominal force
0.08 kg / 0.19 pounds
84.0 g / 0.8 N
Oily/slippery steel
µ = 0.1 10% of nominal force
0.04 kg / 0.09 pounds
42.0 g / 0.4 N
Magnet with anti-slip rubber
µ = 0.5 50% of nominal force
0.21 kg / 0.46 pounds
210.0 g / 2.1 N
When hanging a element on a upright plane (e.g., a board), it will maintain just about 20%-30% of nominal attraction strength. Gravitational force and a low friction coefficient cause that products move down faster than they pop off the substrate. Designing a wall mount? Consider that the shear force is much weaker than the perpendicular breakaway force. On a smooth steel, the element will slide down under a significantly smaller cargo. Utilizing a rubberized layer can effectively improve the result.

Table 4: Material efficiency (saturation) - power losses
MW 12x1 zestaw 1400 szt. / N38

Steel thickness (mm) % power Real pull force (kg/lbs/g/N)
0.5 mm
10%
 0.04 kg / 0.09 pounds
42.0 g / 0.4 N
1 mm
25%
 0.11 kg / 0.23 pounds
105.0 g / 1.0 N
2 mm
50%
 0.21 kg / 0.46 pounds
210.0 g / 2.1 N
3 mm
75%
 0.32 kg / 0.69 pounds
315.0 g / 3.1 N
5 mm
100%
 0.42 kg / 0.93 pounds
420.0 g / 4.1 N
10 mm
100%
 0.42 kg / 0.93 pounds
420.0 g / 4.1 N
11 mm
100%
 0.42 kg / 0.93 pounds
420.0 g / 4.1 N
12 mm
100%
 0.42 kg / 0.93 pounds
420.0 g / 4.1 N
A too thin steel is incapable of absorb the entire magnetic field, which weakens actual performance of the holder. If you attach a powerful product to a thin surface, the magnetism will pass right through and the pull force will drop sharply. To squeeze the maximum of this neodymium's potential, you require a sufficiently solid element of steel. The saturation phenomenon means that on sheet metal structures (e.g., thin profiles), the holder shows lower pull force. We suggest choosing the steel cross-section according to the table below.

Table 5: Thermal resistance (stability) - thermal limit
MW 12x1 zestaw 1400 szt. / N38

Magnet temperature (°C) Force change relative to 20°C Remaining pull (kg/lbs/g/N) Status
20 °C 0.0% 0.42 kg / 0.93 pounds
420.0 g / 4.1 N
 Estimate
40 °C -4.4% 0.40 kg / 0.89 pounds
401.7 g / 3.9 N
 Estimate
60 °C -8.6% 0.38 kg / 0.85 pounds
383.9 g / 3.8 N
 Estimate
80 °C -12.8% 0.37 kg / 0.81 pounds
366.4 g / 3.6 N
 Material limit
100 °C — — Out of range — no model
The table estimates the reversible force change relative to 20°C, assuming a Br coefficient of -0.11%/°C and force proportional to Br². This is a simplified model with unchanged contact and geometry, not a measurement. Above the material limit, neither force nor irreversible magnetization loss is predicted.
The temperature limit comes from this product’s material data. Permissible conditions also depend on geometry and the magnetic circuit. Without B-H curves for the specific grade and temperature, Pc alone does not determine irreversible demagnetization. Values within the material range do not guarantee the allowable temperature of the complete assembly.

Table 6: Magnet-Magnet interaction (attraction) - forces in the system
MW 12x1 zestaw 1400 szt. / N38

Gap (mm) Attraction (kg/lbs) (N-S) Lateral Force (kg/lbs/g/N) Repulsion (kg/lbs) (N-N)
0 mm 0.72 kg / 1.60 pounds
1 959 Gs
0.11 kg / 0.24 pounds
109 g / 1.1 N
 N/A
1 mm 0.68 kg / 1.50 pounds
1 978 Gs
0.10 kg / 0.23 pounds
102 g / 1.0 N
 0.61 kg / 1.35 pounds
~0 Gs
2 mm 0.62 kg / 1.36 pounds
1 883 Gs
0.09 kg / 0.20 pounds
93 g / 0.9 N
 0.56 kg / 1.23 pounds
~0 Gs
3 mm 0.54 kg / 1.19 pounds
1 762 Gs
0.08 kg / 0.18 pounds
81 g / 0.8 N
 0.49 kg / 1.07 pounds
~0 Gs
5 mm 0.38 kg / 0.84 pounds
1 479 Gs
0.06 kg / 0.13 pounds
57 g / 0.6 N
 0.34 kg / 0.76 pounds
~0 Gs
10 mm 0.12 kg / 0.26 pounds
830 Gs
0.02 kg / 0.04 pounds
18 g / 0.2 N
 0.11 kg / 0.24 pounds
~0 Gs
20 mm 0.01 kg / 0.02 pounds
253 Gs
0.00 kg / 0.00 pounds
2 g / 0.0 N
 0.01 kg / 0.02 pounds
~0 Gs
50 mm 0.00 kg / 0.00 pounds
25 Gs
0.00 kg / 0.00 pounds
0 g / 0.0 N
 0.00 kg / 0.00 pounds
~0 Gs
60 mm 0.00 kg / 0.00 pounds
15 Gs
0.00 kg / 0.00 pounds
0 g / 0.0 N
 0.00 kg / 0.00 pounds
~0 Gs
70 mm 0.00 kg / 0.00 pounds
10 Gs
0.00 kg / 0.00 pounds
0 g / 0.0 N
 0.00 kg / 0.00 pounds
~0 Gs
80 mm 0.00 kg / 0.00 pounds
7 Gs
0.00 kg / 0.00 pounds
0 g / 0.0 N
 0.00 kg / 0.00 pounds
~0 Gs
90 mm 0.00 kg / 0.00 pounds
5 Gs
0.00 kg / 0.00 pounds
0 g / 0.0 N
 0.00 kg / 0.00 pounds
~0 Gs
100 mm 0.00 kg / 0.00 pounds
3 Gs
0.00 kg / 0.00 pounds
0 g / 0.0 N
 0.00 kg / 0.00 pounds
~0 Gs
Two magnets interact from a significantly greater distance than a neodymium and metal combination. The setup of magnet-to-magnet produces a massive flux and a larger range of operation. Planning to create a strong closure? Apply two magnets instead of a neodymium and a striker plate. Be careful that when connecting a pair of magnets, the pinch force is extreme. The repulsion force is slightly lower than the connection force, but still large.
*The magnetic induction in repulsion mode drops to ~0 Gs at the geometric center of the gap (caused by magnetic field nullification).
Attention: Calculations refer to shear force of two same magnets (friction coefficient ~0.15 for Ni-Ni plating).

Table 7: Axial field levels — not safety zones
MW 12x1 zestaw 1400 szt. / N38

Field level (Gs) mT Model distance (cm)
< 5 Gs < 0.5 mT 3.5 cm
< 10 Gs < 1.0 mT 3.0 cm
< 20 Gs < 2.0 mT 2.5 cm
< 40 Gs < 4.0 mT 2.0 cm
< 50 Gs < 5.0 mT 1.5 cm
< 400 Gs < 40.0 mT 1.0 cm
< 600 Gs < 60.0 mT 0.5 cm
Reference field levels for a model of one magnet, on its axis in air, with a 5 mm distance step. These are not device immunity limits or safe distances for implants. Do not use this table to assess the safety of a pacemaker, defibrillator or other implant; follow the device manufacturer’s and your clinician’s guidance. Steel and other magnets change the field distribution.

Table 8: Collisions (kinetic energy) - warning
MW 12x1 zestaw 1400 szt. / N38

Start from (mm) Speed (km/h) Energy (J) Predicted outcome
10 mm 0.53 km/h
(0.15 m/s)
 0.01 J
30 mm 0.53 km/h
(0.15 m/s)
 0.01 J
50 mm 0.53 km/h
(0.15 m/s)
 0.01 J
100 mm 0.53 km/h
(0.15 m/s)
 0.01 J
NdFeB products are prone to chipping – a strong collision with metal causes immediate chipping. Control the attraction moment – a neodymium left loose becomes dangerous. Impact energy can trigger coating fragments or injury to skin. Be sure to control the product during bringing near metal so it doesn't hit with great force against the metal. A contact at a velocity of dozens of km/h ends with a crack of the magnet. Use safety goggles when handling with large magnets.

Table 9: Surface protection spec
MW 12x1 zestaw 1400 szt. / N38

Technical parameter Value / Description
Coating type [NiCuNi] Nickel
Layer structure Nickel - Copper - Nickel
Layer thickness 10-20 µm
Salt spray test (SST) ? 24 h
Recommended environment Indoors only (dry)
Neodymium magnets are highly susceptible to corrosion without proper protection. The silver nickel coating also serves an aesthetic function but is not fully waterproof.

Table 10: Electrical data (Pc)
MW 12x1 zestaw 1400 szt. / N38

Parameter Value SI Unit / Description
Magnetic Flux 1 564 Mx 15.6 µWb
Pc Coefficient 0.13 Low (Flat)
Flux value emitted by the magnet pole. Key data for generator designers and motors. Pc value determines the working geometry.

Table 11: Submerged application
MW 12x1 zestaw 1400 szt. / N38

Environment Effective steel pull Effect
Air (land) 0.42 kg Standard
Water (riverbed) 0.48 kg
(+0.06 kg buoyancy gain)
+14.5%
Corrosion warning: Standard nickel requires drying after every contact with moisture; lack of maintenance will lead to rust spots.
The magnetic field penetrates through water without any losses. Buoyancy helps in lifting finds.

1. Sliding resistance

*Note: On a vertical wall, the magnet holds only approx. 20-30% of its nominal pull.

2. Efficiency vs thickness

*Thin steel (e.g. 0.5mm PC case) drastically limits the holding force.

3. Heat tolerance

N38: the maximum material working temperature is 80°C. Permitted conditions also depend on the shape and magnetic circuit.

4. Demagnetization curve and operating point (B-H)

chart generated for the permeance coefficient Pc (Permeance Coefficient) = 0.13

The chart above illustrates the magnetic characteristics of the material within the second quadrant of the hysteresis loop. The solid red line represents the demagnetization curve (material potential), while the dashed blue line is the load line based on the magnet's geometry. The Pc (Permeance Coefficient), also known as the load line slope, is a dimensionless value that describes the relationship between the magnet's shape and its magnetic stability. The intersection of these two lines (the black dot) is the operating point — it determines the actual magnetic flux density generated by the magnet in this specific configuration. A higher Pc value means the magnet is more 'slender' (tall relative to its area), resulting in a higher operating point and better resistance to irreversible demagnetization caused by external fields or temperature. A value of 0.42 is relatively low (typical for flat magnets), meaning the operating point is closer to the 'knee' of the curve — caution is advised when operating at temperatures near the maximum limit to avoid strength loss.

Technical specification and ecology

Material specification

iron (Fe) 64% – 68%
neodymium (Nd) 29% – 32%
boron (B) 1.1% – 1.2%
dysprosium (Dy) 0.5% – 2.0%
coating (Ni-Cu-Ni) < 0.05%

Sustainability

recyclability (EoL) 100%
recycled raw materials ~10% (pre-cons)
carbon footprint low / zredukowany
waste code (EWC) 16 02 16
Safety card (GPSR)
responsible entity
Dhit sp. z o.o.
ul. Kościuszki 6A, 05-850 Ożarów Mazowiecki
tel: +48 22 499 98 98 | e-mail: bok@dhit.pl
batch number/type
id: 010560-2026
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The presented product is a very strong rod magnet, made from durable NdFeB material, which, at dimensions of Ø12x1 mm, guarantees maximum efficiency. This specific item boasts a tolerance of ±0.1mm and professional build quality, making it an ideal solution for professional engineers and designers. As a magnetic rod with significant force (approx. 0.42 kg), this product is in stock from our warehouse in Poland, ensuring lightning-fast order fulfillment. Furthermore, its triple-layer Ni-Cu-Ni coating effectively protects it against corrosion in standard operating conditions, guaranteeing an aesthetic appearance and durability for years.
This model is perfect for building electric motors, advanced Hall effect sensors, and efficient filters, where field concentration on a small surface counts. Thanks to the pull force of 4.15 N with a weight of only 1190 g, this cylindrical magnet is indispensable in miniature devices and wherever every gram matters.
Since our magnets have a very precise dimensions, the recommended way is to glue them into holes with a slightly larger diameter (e.g., 12.1 mm) using epoxy glues. To ensure stability in industry, anaerobic resins are used, which do not react with the nickel coating and fill the gap, guaranteeing durability of the connection.
Choose the material grade together with the dimensions and working conditions. A grade designation alone does not determine the pull force of the finished magnet. Check the properties and working temperature of this specific model on its product card; contact us before ordering for an unusual application.
The presented product is a neodymium magnet with precisely defined parameters: diameter 12 mm and height 1 mm. The key parameter here is the lifting capacity amounting to approximately 0.42 kg (force ~4.15 N), which, with such defined dimensions, proves the high power of the NdFeB material. The product has a [NiCuNi] coating, which protects the surface against external factors, giving it an aesthetic, silvery shine.
Standardly, the magnetic axis runs through the center of the cylinder, causing the greatest attraction force to occur on the bases with a diameter of 12 mm. Thanks to this, the magnet can be easily glued into a hole and achieve a strong field on the front surface. On request, we can also produce versions magnetized through the diameter if your project requires it.

Strengths as well as weaknesses of rare earth magnets.

Advantages

Besides their tremendous magnetic power, neodymium magnets offer the following advantages:
  • They retain attractive force for almost 10 years – the loss is just ~1% (in theory),
  • They show high resistance to demagnetization induced by external disturbances,
  • The use of an shiny finish of noble metals (nickel, gold, silver) causes the element to present itself better,
  • The surface of neodymium magnets generates a unique magnetic field – this is a key feature,
  • Made from properly selected components, these magnets show impressive resistance to high heat, enabling them to function (depending on their form) at temperatures up to 230°C and above...
  • Thanks to flexibility in forming and the ability to customize to unusual requirements,
  • Key role in advanced technology sectors – they are commonly used in data components, brushless drives, precision medical tools, and other advanced devices.
  • Relatively small size with high pulling force – neodymium magnets offer impressive pulling force in compact dimensions, which allows their use in compact constructions

Weaknesses

Disadvantages of NdFeB magnets:
  • To avoid cracks under impact, we suggest using special steel holders. Such a solution protects the magnet and simultaneously improves its durability.
  • Do not exceed this material temperature limit: 80°C. Overheating may permanently weaken the magnet.
  • Magnets exposed to a humid environment can rust. Therefore while using outdoors, we advise using waterproof magnets made of rubber, plastic or other material resistant to moisture
  • We recommend a housing - magnetic mechanism, due to difficulties in producing nuts inside the magnet and complicated forms.
  • Health risk related to microscopic parts of magnets pose a threat, if swallowed, which is particularly important in the context of child health protection. Additionally, small elements of these products can complicate diagnosis medical after entering the body.
  • Due to expensive raw materials, their price exceeds standard values,

Pull force analysis

Maximum lifting capacity of the magnet – what affects it?

Holding force of 0.42 kg is a measurement result executed under specific, ideal conditions:
  • using a plate made of low-carbon steel, serving as a ideal flux conductor
  • possessing a thickness of min. 10 mm to avoid saturation
  • characterized by lack of roughness
  • under conditions of ideal adhesion (metal-to-metal)
  • during pulling in a direction vertical to the plane
  • at standard ambient temperature

Impact of factors on magnetic holding capacity in practice

In real-world applications, the actual lifting capacity results from several key aspects, presented from the most important:
  • Space between magnet and steel – even a fraction of a millimeter of distance (caused e.g. by varnish or dirt) drastically reduces the pulling force, often by half at just 0.5 mm.
  • Force direction – note that the magnet holds strongest perpendicularly. Under shear forces, the holding force drops drastically, often to levels of 20-30% of the nominal value.
  • Base massiveness – too thin steel does not close the flux, causing part of the flux to be wasted into the air.
  • Material composition – not every steel attracts identically. Alloy additives worsen the interaction with the magnet.
  • Surface finish – full contact is possible only on polished steel. Rough texture reduce the real contact area, weakening the magnet.
  • Thermal environment – heating the magnet causes a temporary drop of induction. It is worth remembering the thermal limit for a given model.

Lifting capacity testing was performed on a smooth plate of suitable thickness, under a perpendicular pulling force, whereas under shearing force the load capacity is reduced by as much as 5 times. Moreover, even a small distance between the magnet and the plate lowers the lifting capacity.

Safety rules for work with neodymium magnets
Phone sensors

A strong magnetic field disrupts the operation of magnetometers in phones and GPS navigation. Keep magnets close to a device to avoid breaking the sensors.

Bodily injuries

Protect your hands. Two powerful magnets will snap together immediately with a force of several hundred kilograms, destroying everything in their path. Exercise extreme caution!

Do not overheat magnets

Do not exceed the maximum operating temperature stated in the specifications of the particular product. The limit depends on the material, geometry and operating arrangement; there is no single threshold for all neodymium magnets. Overheating can permanently weaken a magnet.

Nickel allergy

Medical facts indicate that nickel (standard magnet coating) is a strong allergen. If your skin reacts to metals, prevent direct skin contact or select encased magnets.

Respect the power

Before use, read the rules. Sudden snapping can destroy the magnet or hurt your hand. Think ahead.

Dust is flammable

Drilling and cutting of neodymium magnets poses a fire risk. Magnetic powder oxidizes rapidly with oxygen and is hard to extinguish.

Magnetic media

Do not bring magnets near a wallet, laptop, or TV. The magnetism can destroy these devices and wipe information from cards.

Shattering risk

Neodymium magnets are ceramic materials, which means they are prone to chipping. Impact of two magnets will cause them shattering into shards.

ICD Warning

Individuals with a ICD should keep an large gap from magnets. The magnetism can interfere with the functioning of the implant.

Swallowing risk

Always keep magnets out of reach of children. Ingestion danger is significant, and the effects of magnets connecting inside the body are life-threatening.

Important! Details about risks in the article: Magnet Safety Guide.