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MW 12x1.5 zestaw 1820 szt. / N38 - cylindrical magnet

cylindrical magnet

Catalog no 010561

GTIN/EAN: 5906301815532

Load capacity 0.87 kg / 8.51 N Magnetic Induction 150.32 mT / 1503 Gs
Diameter Ø
12 mm [±0,1 mm]
Height
1.5 mm [±0,1 mm]
Weight
2311.4 g
Magnetization Direction
↑ axial
Coating
[NiCuNi] Nickel

How we measure these parameters — certificates and measurements

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599.27 zł net / pcs

737.10 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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Technical details - MW 12x1.5 zestaw 1820 szt. / N38 - cylindrical magnet

Specification / characteristics - MW 12x1.5 zestaw 1820 szt. / N38 - cylindrical magnet

properties
properties values
Cat. no. 010561
GTIN/EAN 5906301815532
Distributor Dhit sp. z o.o.
Country of origin Poland / China / Germany
Customs code 85059029
Diameter Ø 12 mm [±0,1 mm]
Height 1.5 mm [±0,1 mm]
Weight 2311.4 g
Magnetization Direction ↑ axial
Load capacity ~ ? 0.87 kg / 8.51 N
Magnetic Induction ~ ? 150.32 mT / 1503 Gs
Coating [NiCuNi] Nickel
Manufacturing Tolerance ±0.1 mm

Magnetic properties of material N38

Specification / characteristics MW 12x1.5 zestaw 1820 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 modeling of the product - technical parameters

These information constitute the direct effect of a mathematical analysis. Values rely on algorithms for the material Nd2Fe14B. Real-world conditions may deviate from the simulation results. Please consider these calculations as a reference point during assembly planning.

Table 1: Static pull force (force vs gap) - characteristics
MW 12x1.5 zestaw 1820 szt. / N38

Distance (mm) Induction (Gauss) / mT Pull Force (kg/lbs/g/N) Risk Status
0 mm 1503 Gs
150.3 mT
 0.87 kg / 1.92 pounds
870.0 g / 8.5 N
 low risk
1 mm 1365 Gs
136.5 mT
 0.72 kg / 1.58 pounds
718.1 g / 7.0 N
 low risk
2 mm 1163 Gs
116.3 mT
 0.52 kg / 1.15 pounds
521.4 g / 5.1 N
 low risk
3 mm 947 Gs
94.7 mT
 0.35 kg / 0.76 pounds
345.7 g / 3.4 N
 low risk
5 mm 587 Gs
58.7 mT
 0.13 kg / 0.29 pounds
132.6 g / 1.3 N
 low risk
10 mm 180 Gs
18.0 mT
 0.01 kg / 0.03 pounds
12.5 g / 0.1 N
 low risk
15 mm 70 Gs
7.0 mT
 0.00 kg / 0.00 pounds
1.9 g / 0.0 N
 low risk
20 mm 33 Gs
3.3 mT
 0.00 kg / 0.00 pounds
0.4 g / 0.0 N
 low risk
30 mm 11 Gs
1.1 mT
 0.00 kg / 0.00 pounds
0.0 g / 0.0 N
 low risk
50 mm 3 Gs
0.3 mT
 0.00 kg / 0.00 pounds
0.0 g / 0.0 N
 low risk
Grip strength weakens sharply with every subsequent millimeter of gap. Remember that even a very thin break (e.g., contamination, paint, rust) significantly weakens the grip. Magnets hold strongest in perfect adhesion; gap nullifies the force. Notice how quickly the load capacity drop, when the product does not adhere flatly to the steel surface. When designing the mounting, discard additional spacers.

Table 2: Slippage force (vertical surface)
MW 12x1.5 zestaw 1820 szt. / N38

Distance (mm) Friction coefficient Pull Force (kg/lbs/g/N)
0 mm Raw steel (µ ≈ 0.2) 0.17 kg / 0.38 pounds
174.0 g / 1.7 N
1 mm Raw steel (µ ≈ 0.2) 0.14 kg / 0.32 pounds
144.0 g / 1.4 N
2 mm Raw steel (µ ≈ 0.2) 0.10 kg / 0.23 pounds
104.0 g / 1.0 N
3 mm Raw steel (µ ≈ 0.2) 0.07 kg / 0.15 pounds
70.0 g / 0.7 N
5 mm Raw steel (µ ≈ 0.2) 0.03 kg / 0.06 pounds
26.0 g / 0.3 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
This section presents the approximate weight limit required to cause the downward movement of the magnet downwards along a vertical metal surface (considering typical friction coefficient). The holding force is relative to the air gap between the magnet and the metal.

Table 3: Wall mounting (sliding) - behavior on slippery surfaces
MW 12x1.5 zestaw 1820 szt. / N38

Surface type Friction coefficient / % Max load (kg/lbs/g/N)
Raw steel
µ = 0.3 30% of nominal force
0.26 kg / 0.58 pounds
261.0 g / 2.6 N
Painted steel (standard)
µ = 0.2 20% of nominal force
0.17 kg / 0.38 pounds
174.0 g / 1.7 N
Oily/slippery steel
µ = 0.1 10% of nominal force
0.09 kg / 0.19 pounds
87.0 g / 0.9 N
Magnet with anti-slip rubber
µ = 0.5 50% of nominal force
0.44 kg / 0.96 pounds
435.0 g / 4.3 N
When mounting a element on a vertical plane (e.g., a car body), it will maintain only approx. 20%-30% of nominal attraction strength. Gravitational force as well as a low friction coefficient influence the fact that magnets slide down easier than they pull off. Designing a hanger? Remember that the shear force is much weaker than the maximum static pull force. On a slippery surface, the magnet will slide down under a significantly smaller weight. Application of an anti-slip layer can significantly raise the stability.

Table 4: Steel thickness (substrate influence) - power losses
MW 12x1.5 zestaw 1820 szt. / N38

Steel thickness (mm) % power Real pull force (kg/lbs/g/N)
0.5 mm
10%
 0.09 kg / 0.19 pounds
87.0 g / 0.9 N
1 mm
25%
 0.22 kg / 0.48 pounds
217.5 g / 2.1 N
2 mm
50%
 0.44 kg / 0.96 pounds
435.0 g / 4.3 N
3 mm
75%
 0.65 kg / 1.44 pounds
652.5 g / 6.4 N
5 mm
100%
 0.87 kg / 1.92 pounds
870.0 g / 8.5 N
10 mm
100%
 0.87 kg / 1.92 pounds
870.0 g / 8.5 N
11 mm
100%
 0.87 kg / 1.92 pounds
870.0 g / 8.5 N
12 mm
100%
 0.87 kg / 1.92 pounds
870.0 g / 8.5 N
A thin metal plate cannot conduct the entire magnetic field, which wastes potential of the holder. Should you attach a powerful product to a weak sheet, the field will pass right through and the attraction force will be weaker. To utilize full efficiency of this neodymium's potential, you require a sufficiently solid piece of metal. The material oversaturation causes that on delicate walls (e.g., appliance housings), the holder holds weaker. We recommend selecting the steel dimension according to the table below.

Table 5: Thermal stability (material behavior) - power drop
MW 12x1.5 zestaw 1820 szt. / N38

Magnet temperature (°C) Force change relative to 20°C Remaining pull (kg/lbs/g/N) Status
20 °C 0.0% 0.87 kg / 1.92 pounds
870.0 g / 8.5 N
 Estimate
40 °C -4.4% 0.83 kg / 1.83 pounds
832.1 g / 8.2 N
 Estimate
60 °C -8.6% 0.80 kg / 1.75 pounds
795.1 g / 7.8 N
 Estimate
80 °C -12.8% 0.76 kg / 1.67 pounds
758.9 g / 7.4 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 (repulsion) - field range
MW 12x1.5 zestaw 1820 szt. / N38

Gap (mm) Attraction (kg/lbs) (N-S) Shear Strength (kg/lbs/g/N) Repulsion (kg/lbs) (N-N)
0 mm 1.57 kg / 3.47 pounds
2 770 Gs
0.24 kg / 0.52 pounds
236 g / 2.3 N
 N/A
1 mm 1.46 kg / 3.21 pounds
2 891 Gs
0.22 kg / 0.48 pounds
219 g / 2.1 N
 1.31 kg / 2.89 pounds
~0 Gs
2 mm 1.30 kg / 2.87 pounds
2 731 Gs
0.19 kg / 0.43 pounds
195 g / 1.9 N
 1.17 kg / 2.58 pounds
~0 Gs
3 mm 1.12 kg / 2.48 pounds
2 538 Gs
0.17 kg / 0.37 pounds
168 g / 1.7 N
 1.01 kg / 2.23 pounds
~0 Gs
5 mm 0.78 kg / 1.71 pounds
2 109 Gs
0.12 kg / 0.26 pounds
116 g / 1.1 N
 0.70 kg / 1.54 pounds
~0 Gs
10 mm 0.24 kg / 0.53 pounds
1 173 Gs
0.04 kg / 0.08 pounds
36 g / 0.4 N
 0.22 kg / 0.48 pounds
~0 Gs
20 mm 0.02 kg / 0.05 pounds
361 Gs
0.00 kg / 0.01 pounds
3 g / 0.0 N
 0.02 kg / 0.05 pounds
~0 Gs
50 mm 0.00 kg / 0.00 pounds
36 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
22 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
14 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
10 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
7 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
5 Gs
0.00 kg / 0.00 pounds
0 g / 0.0 N
 0.00 kg / 0.00 pounds
~0 Gs
Two strong neodymiums attract each other from a much further distance than a neodymium and metal combination. The setup of two magnets creates a more powerful interaction and a wider radius of action. Want to build a strong closure? Apply two magnets instead of one magnet and a striker plate. Exercise caution that when attracting two neodymiums, the collision energy is huge. The repulsion force is marginally weaker than the attraction, but still large.
*Field value between like poles reaches ~0 Gs in the exact middle between the magnets (due to field cancellation).
* Figures refer to friction force of two identical neodymium magnets (friction coefficient ~0.15 for Ni-Ni layer).

Table 7: Axial field levels — not safety zones
MW 12x1.5 zestaw 1820 szt. / N38

Field level (Gs) mT Model distance (cm)
< 5 Gs < 0.5 mT 4.0 cm
< 10 Gs < 1.0 mT 3.5 cm
< 20 Gs < 2.0 mT 2.5 cm
< 40 Gs < 4.0 mT 2.0 cm
< 50 Gs < 5.0 mT 2.0 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 12x1.5 zestaw 1820 szt. / N38

Start from (mm) Speed (km/h) Energy (J) Predicted outcome
10 mm 0.53 km/h
(0.15 m/s)
 0.02 J
30 mm 0.53 km/h
(0.15 m/s)
 0.03 J
50 mm 0.53 km/h
(0.15 m/s)
 0.03 J
100 mm 0.53 km/h
(0.15 m/s)
 0.03 J
NdFeB products are very brittle – a strong collision with metal can result in shattering. Watch the impact speed – a neodymium left loose speeds with massive force. Striking energy can trigger coating fragments or painful pinches to skin. Always hold the magnet during installation so it doesn't hit with great force against the metal. A collision at high speed almost guarantees destruction of the neodymium. Wear safety glasses when playing with powerful specimens.

Table 9: Corrosion resistance
MW 12x1.5 zestaw 1820 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)
For outdoor applications, an epoxy coating is required; standard nickel is intended for indoor use. The silver nickel coating also serves an aesthetic function but is not fully waterproof.

Table 10: Construction data (Pc)
MW 12x1.5 zestaw 1820 szt. / N38

Parameter Value SI Unit / Description
Magnetic Flux 2 159 Mx 21.6 µWb
Pc Coefficient 0.19 Low (Flat)
Total magnetic flux emitted by the pole surface. Key data for generator designers and motors. Pc value defines the working geometry.

Table 11: Hydrostatics and buoyancy
MW 12x1.5 zestaw 1820 szt. / N38

Environment Effective steel pull Effect
Air (land) 0.87 kg Standard
Water (riverbed) 1.00 kg
(+0.13 kg buoyancy gain)
+14.5%
Corrosion warning: Remember to wipe the magnet thoroughly after removing it from water and apply a protective layer (e.g., oil) to avoid corrosion.
Contrary to myths, water does not block the magnetic field. However, remember the water resistance when pulling the rope quickly.

1. Sliding resistance

*Warning: On a vertical surface, the magnet holds merely approx. 20-30% of its perpendicular strength.

2. Efficiency vs thickness

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

3. Temperature resistance

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) = 0.19

This simulation demonstrates the magnetic stability of the selected magnet under specific geometric conditions. 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

Elemental analysis

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%

Ecology and recycling (GPSR)

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: 010561-2026
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The presented product is an exceptionally strong cylindrical magnet, made from advanced NdFeB material, which, with dimensions of Ø12x1.5 mm, guarantees maximum efficiency. The MW 12x1.5 zestaw 1820 szt. / N38 component boasts an accuracy of ±0.1mm and industrial build quality, making it an excellent solution for professional engineers and designers. As a magnetic rod with impressive force (approx. 0.87 kg), this product is in stock from our European logistics center, ensuring rapid order fulfillment. Additionally, its Ni-Cu-Ni coating secures it against corrosion in standard operating conditions, guaranteeing an aesthetic appearance and durability for years.
This model is created for building electric motors, advanced Hall effect sensors, and efficient filters, where maximum induction on a small surface counts. Thanks to the pull force of 8.51 N with a weight of only 2311.4 g, this rod is indispensable in miniature devices and wherever every gram matters.
Since our magnets have a tolerance of ±0.1mm, 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 are safe for nickel 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 1.5 mm. The key parameter here is the lifting capacity amounting to approximately 0.87 kg (force ~8.51 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.
This rod magnet is magnetized axially (along the height of 1.5 mm), which means that the N and S poles are located on the flat, circular surfaces. Such an arrangement is standard when connecting magnets in stacks (e.g., in filters) or when mounting in sockets at the bottom of a hole. On request, we can also produce versions magnetized through the diameter if your project requires it.

Advantages and disadvantages of rare earth magnets.

Strengths

Besides their stability, neodymium magnets are valued for these benefits:
  • Their magnetic field remains stable, and after around 10 years it decreases only by ~1% (according to research),
  • They maintain their magnetic properties even under strong external field,
  • In other words, due to the glossy finish of silver, the element becomes visually attractive,
  • They feature high magnetic induction at the operating surface, which affects their effectiveness,
  • Through (adequate) combination of ingredients, they can achieve high thermal strength, enabling operation at temperatures approaching 230°C and above...
  • Due to the potential of flexible shaping and adaptation to unique requirements, magnetic components can be created in a variety of geometric configurations, which increases their versatility,
  • Huge importance in future technologies – they find application in computer drives, electric drive systems, medical equipment, and technologically advanced constructions.
  • Compactness – despite small sizes they offer powerful magnetic field, making them ideal for precision applications

Limitations

Disadvantages of NdFeB magnets:
  • To avoid cracks upon strong impacts, we suggest using special steel holders. Such a solution protects the magnet and simultaneously increases its durability.
  • Do not exceed this material temperature limit: 80°C. Overheating may permanently weaken the magnet.
  • They rust in a humid environment - during use outdoors we advise using waterproof magnets e.g. in rubber, plastic
  • Limited possibility of making threads in the magnet and complex shapes - recommended is casing - magnetic holder.
  • Health risk related to microscopic parts of magnets pose a threat, if swallowed, which gains importance in the context of child safety. It is also worth noting that small elements of these magnets can be problematic in diagnostics medical when they are in the body.
  • Higher cost of purchase is a significant factor to consider compared to ceramic magnets, especially in budget applications

Pull force analysis

Detachment force of the magnet in optimal conditions – what affects it?

Breakaway force was defined for ideal contact conditions, taking into account:
  • with the contact of a sheet made of low-carbon steel, ensuring maximum field concentration
  • with a cross-section minimum 10 mm
  • with an ground contact surface
  • with zero gap (no impurities)
  • under perpendicular force vector (90-degree angle)
  • at ambient temperature approx. 20 degrees Celsius

Impact of factors on magnetic holding capacity in practice

In real-world applications, the actual lifting capacity depends on several key aspects, ranked from the most important:
  • Distance (between the magnet and the plate), as even a very small clearance (e.g. 0.5 mm) can cause a drastic drop in force by up to 50% (this also applies to varnish, rust or dirt).
  • Force direction – declared lifting capacity refers to detachment vertically. When attempting to slide, the magnet holds significantly lower power (often approx. 20-30% of nominal force).
  • Base massiveness – insufficiently thick steel does not close the flux, causing part of the flux to be wasted to the other side.
  • Material composition – not every steel reacts the same. High carbon content weaken the attraction effect.
  • Surface quality – the more even the surface, the better the adhesion and higher the lifting capacity. Unevenness acts like micro-gaps.
  • Temperature influence – hot environment weakens magnetic field. Exceeding the limit temperature can permanently damage the magnet.

Lifting capacity was determined using a polished steel plate of optimal thickness (min. 20 mm), under perpendicular detachment force, whereas under parallel forces the holding force is lower. Additionally, even a small distance between the magnet and the plate reduces the holding force.

Safety rules for work with neodymium magnets
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.

Magnetic media

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

Mechanical processing

Machining of neodymium magnets poses a fire hazard. Magnetic powder reacts violently with oxygen and is hard to extinguish.

Conscious usage

Before use, read the rules. Uncontrolled attraction can destroy the magnet or injure your hand. Think ahead.

Physical harm

Mind your fingers. Two large magnets will join immediately with a force of massive weight, destroying everything in their path. Be careful!

Pacemakers

Patients with a pacemaker must maintain an absolute distance from magnets. The magnetism can interfere with the functioning of the implant.

Fragile material

Despite metallic appearance, the material is brittle and cannot withstand shocks. Avoid impacts, as the magnet may crumble into sharp, dangerous pieces.

Phone sensors

An intense magnetic field negatively affects the functioning of magnetometers in smartphones and navigation systems. Maintain magnets close to a device to avoid breaking the sensors.

Swallowing risk

These products are not suitable for play. Swallowing a few magnets can lead to them connecting inside the digestive tract, which poses a severe health hazard and requires urgent medical intervention.

Sensitization to coating

Medical facts indicate that the nickel plating (the usual finish) is a common allergen. If you have an allergy, avoid direct skin contact or opt for coated magnets.

Danger! Need more info? Check our post: Are neodymium magnets dangerous?