MW 8x5 / N38 - cylindrical magnet
cylindrical magnet
Catalog no 010105
GTIN/EAN: 5906301811046
Diameter Ø
8 mm [±0,1 mm]
Height
5 mm [±0,1 mm]
Weight
1.88 g
Magnetization Direction
↑ axial
Load capacity
2.17 kg / 21.31 N
Magnetic Induction
483.41 mT / 4834 Gs
Coating
[NiCuNi] Nickel
0.836 ZŁ with VAT / pcs + price for transport
0.680 ZŁ net + 23% VAT / pcs
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MW 8x5 / N38 - cylindrical magnet
Specification / characteristics MW 8x5 / N38 - cylindrical magnet
| properties | values |
|---|---|
| Cat. no. | 010105 |
| GTIN/EAN | 5906301811046 |
| Production/Distribution | Dhit sp. z o.o. |
| Country of origin | Poland / China / Germany |
| Customs code | 85059029 |
| Diameter Ø | 8 mm [±0,1 mm] |
| Height | 5 mm [±0,1 mm] |
| Weight | 1.88 g |
| Magnetization Direction | ↑ axial |
| Load capacity ~ ? | 2.17 kg / 21.31 N |
| Magnetic Induction ~ ? | 483.41 mT / 4834 Gs |
| Coating | [NiCuNi] Nickel |
| Manufacturing Tolerance | ±0.1 mm |
Magnetic properties of material N38
| properties | values | units |
|---|---|---|
| remenance Br [min. - max.] ? | 12.2-12.6 | kGs |
| remenance Br [min. - max.] ? | 1220-1260 | mT |
| coercivity bHc ? | 10.8-11.5 | kOe |
| coercivity bHc ? | 860-915 | kA/m |
| actual internal force iHc | ≥ 12 | kOe |
| actual internal force iHc | ≥ 955 | kA/m |
| energy density [min. - max.] ? | 36-38 | BH max MGOe |
| energy density [min. - max.] ? | 287-303 | BH max KJ/m |
| max. temperature ? | ≤ 80 | °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 | 312 - 380 | °C |
| Curie Temperature TF | 593 - 716 | °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 |
Technical modeling of the magnet - data
These data represent the outcome of a physical calculation. Values rely on models for the material Nd2Fe14B. Real-world parameters might slightly differ from theoretical values. Use these data as a reference point during assembly planning.
MW 8x5 / N38
| Distance (mm) | Induction (Gauss) / mT | Pull Force (kg) | Risk Status |
|---|---|---|---|
| 0 mm |
4830 Gs
483.0 mT
|
2.17 kg / 2170.0 g
21.3 N
|
medium risk |
| 1 mm |
3655 Gs
365.5 mT
|
1.24 kg / 1242.8 g
12.2 N
|
safe |
| 2 mm |
2610 Gs
261.0 mT
|
0.63 kg / 633.9 g
6.2 N
|
safe |
| 3 mm |
1825 Gs
182.5 mT
|
0.31 kg / 310.0 g
3.0 N
|
safe |
| 5 mm |
915 Gs
91.5 mT
|
0.08 kg / 77.9 g
0.8 N
|
safe |
| 10 mm |
234 Gs
23.4 mT
|
0.01 kg / 5.1 g
0.1 N
|
safe |
| 15 mm |
89 Gs
8.9 mT
|
0.00 kg / 0.7 g
0.0 N
|
safe |
| 20 mm |
43 Gs
4.3 mT
|
0.00 kg / 0.2 g
0.0 N
|
safe |
| 30 mm |
14 Gs
1.4 mT
|
0.00 kg / 0.0 g
0.0 N
|
safe |
| 50 mm |
3 Gs
0.3 mT
|
0.00 kg / 0.0 g
0.0 N
|
safe |
MW 8x5 / N38
| Distance (mm) | Friction coefficient | Pull Force (kg) |
|---|---|---|
| 0 mm | Stal (~0.2) |
0.43 kg / 434.0 g
4.3 N
|
| 1 mm | Stal (~0.2) |
0.25 kg / 248.0 g
2.4 N
|
| 2 mm | Stal (~0.2) |
0.13 kg / 126.0 g
1.2 N
|
| 3 mm | Stal (~0.2) |
0.06 kg / 62.0 g
0.6 N
|
| 5 mm | Stal (~0.2) |
0.02 kg / 16.0 g
0.2 N
|
| 10 mm | Stal (~0.2) |
0.00 kg / 2.0 g
0.0 N
|
| 15 mm | Stal (~0.2) |
0.00 kg / 0.0 g
0.0 N
|
| 20 mm | Stal (~0.2) |
0.00 kg / 0.0 g
0.0 N
|
| 30 mm | Stal (~0.2) |
0.00 kg / 0.0 g
0.0 N
|
| 50 mm | Stal (~0.2) |
0.00 kg / 0.0 g
0.0 N
|
MW 8x5 / N38
| Surface type | Friction coefficient / % Mocy | Max load (kg) |
|---|---|---|
| Raw steel |
µ = 0.3
30% Nominalnej Siły
|
0.65 kg / 651.0 g
6.4 N
|
| Painted steel (standard) |
µ = 0.2
20% Nominalnej Siły
|
0.43 kg / 434.0 g
4.3 N
|
| Oily/slippery steel |
µ = 0.1
10% Nominalnej Siły
|
0.22 kg / 217.0 g
2.1 N
|
| Magnet with anti-slip rubber |
µ = 0.5
50% Nominalnej Siły
|
1.09 kg / 1085.0 g
10.6 N
|
MW 8x5 / N38
| Steel thickness (mm) | % power | Real pull force (kg) |
|---|---|---|
| 0.5 mm |
|
0.22 kg / 217.0 g
2.1 N
|
| 1 mm |
|
0.54 kg / 542.5 g
5.3 N
|
| 2 mm |
|
1.09 kg / 1085.0 g
10.6 N
|
| 5 mm |
|
2.17 kg / 2170.0 g
21.3 N
|
| 10 mm |
|
2.17 kg / 2170.0 g
21.3 N
|
MW 8x5 / N38
| Ambient temp. (°C) | Power loss | Remaining pull | Status |
|---|---|---|---|
| 20 °C | 0.0% |
2.17 kg / 2170.0 g
21.3 N
|
OK |
| 40 °C | -2.2% |
2.12 kg / 2122.3 g
20.8 N
|
OK |
| 60 °C | -4.4% |
2.07 kg / 2074.5 g
20.4 N
|
OK |
| 80 °C | -6.6% |
2.03 kg / 2026.8 g
19.9 N
|
|
| 100 °C | -28.8% |
1.55 kg / 1545.0 g
15.2 N
|
MW 8x5 / N38
| Gap (mm) | Attraction (kg) (N-S) | Repulsion (kg) (N-N) |
|---|---|---|
| 0 mm |
7.23 kg / 7228 g
70.9 N
5 742 Gs
|
N/A |
| 1 mm |
5.58 kg / 5585 g
54.8 N
8 490 Gs
|
5.03 kg / 5026 g
49.3 N
~0 Gs
|
| 2 mm |
4.14 kg / 4140 g
40.6 N
7 310 Gs
|
3.73 kg / 3726 g
36.6 N
~0 Gs
|
| 3 mm |
2.98 kg / 2984 g
29.3 N
6 207 Gs
|
2.69 kg / 2686 g
26.3 N
~0 Gs
|
| 5 mm |
1.48 kg / 1479 g
14.5 N
4 369 Gs
|
1.33 kg / 1331 g
13.1 N
~0 Gs
|
| 10 mm |
0.26 kg / 260 g
2.5 N
1 830 Gs
|
0.23 kg / 234 g
2.3 N
~0 Gs
|
| 20 mm |
0.02 kg / 17 g
0.2 N
468 Gs
|
0.02 kg / 15 g
0.1 N
~0 Gs
|
| 50 mm |
0.00 kg / 0 g
0.0 N
47 Gs
|
0.00 kg / 0 g
0.0 N
~0 Gs
|
MW 8x5 / N38
| Object / Device | Limit (Gauss) / mT | Safe distance |
|---|---|---|
| Pacemaker | 5 Gs (0.5 mT) | 4.5 cm |
| Hearing aid | 10 Gs (1.0 mT) | 3.5 cm |
| Mechanical watch | 20 Gs (2.0 mT) | 3.0 cm |
| Mobile device | 40 Gs (4.0 mT) | 2.5 cm |
| Car key | 50 Gs (5.0 mT) | 2.0 cm |
| Payment card | 400 Gs (40.0 mT) | 1.0 cm |
| HDD hard drive | 600 Gs (60.0 mT) | 1.0 cm |
MW 8x5 / N38
| Start from (mm) | Speed (km/h) | Energy (J) | Predicted outcome |
|---|---|---|---|
| 10 mm |
34.31 km/h
(9.53 m/s)
|
0.09 J | |
| 30 mm |
59.35 km/h
(16.49 m/s)
|
0.26 J | |
| 50 mm |
76.62 km/h
(21.28 m/s)
|
0.43 J | |
| 100 mm |
108.35 km/h
(30.10 m/s)
|
0.85 J |
MW 8x5 / 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) |
MW 8x5 / N38
| Parameter | Value | SI Unit / Description |
|---|---|---|
| Magnetic Flux | 2 450 Mx | 24.5 µWb |
| Pc Coefficient | 0.68 | High (Stable) |
MW 8x5 / N38
| Environment | Effective steel pull | Effect |
|---|---|---|
| Air (land) | 2.17 kg | Standard |
| Water (riverbed) |
2.48 kg
(+0.31 kg Buoyancy gain)
|
+14.5% |
1. Sliding resistance
*Warning: On a vertical surface, the magnet retains just ~20% of its max power.
2. Steel saturation
*Thin steel (e.g. 0.5mm PC case) drastically reduces the holding force.
3. Power loss vs temp
*For standard magnets, the safety limit is 80°C.
4. Demagnetization curve and operating point (B-H)
chart generated for the permeance coefficient Pc (Permeance Coefficient) = 0.68
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.
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% |
Sustainability
| recyclability (EoL) | 100% |
| recycled raw materials | ~10% (pre-cons) |
| carbon footprint | low / zredukowany |
| waste code (EWC) | 16 02 16 |
Other offers
Advantages and disadvantages of rare earth magnets.
Pros
- Their power is maintained, and after approximately 10 years it drops only by ~1% (according to research),
- They feature excellent resistance to magnetic field loss when exposed to external magnetic sources,
- Thanks to the glossy finish, the layer of Ni-Cu-Ni, gold, or silver gives an aesthetic appearance,
- The surface of neodymium magnets generates a strong 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 shape) at temperatures up to 230°C and above...
- Possibility of precise shaping and adjusting to concrete requirements,
- Fundamental importance in future technologies – they are used in mass storage devices, electric motors, medical equipment, also multitasking production systems.
- Relatively small size with high pulling force – neodymium magnets offer high power in compact dimensions, which makes them useful in miniature devices
Cons
- At very strong impacts they can break, therefore we recommend placing them in special holders. A metal housing provides additional protection against damage, as well as increases the magnet's durability.
- Neodymium magnets lose strength when exposed to high temperatures. After reaching 80°C, many of them experience permanent drop of power (a factor is the shape as well as dimensions of the magnet). We offer magnets specially adapted to work at temperatures up to 230°C marked [AH], which are very resistant to heat
- They rust in a humid environment - during use outdoors we suggest using waterproof magnets e.g. in rubber, plastic
- We recommend cover - magnetic mount, due to difficulties in creating nuts inside the magnet and complex shapes.
- Potential hazard to health – tiny shards of magnets can be dangerous, when accidentally swallowed, which gains importance in the context of child health protection. It is also worth noting that tiny parts of these products are able to be problematic in diagnostics medical after entering the body.
- Due to expensive raw materials, their price is relatively high,
Lifting parameters
Optimal lifting capacity of a neodymium magnet – what contributes to it?
- on a base made of mild steel, perfectly concentrating the magnetic field
- whose thickness equals approx. 10 mm
- characterized by lack of roughness
- without the slightest air gap between the magnet and steel
- for force applied at a right angle (pull-off, not shear)
- in neutral thermal conditions
Practical aspects of lifting capacity – factors
- Gap between surfaces – even a fraction of a millimeter of distance (caused e.g. by varnish or unevenness) significantly weakens the pulling force, often by half at just 0.5 mm.
- Force direction – remember that the magnet holds strongest perpendicularly. Under shear forces, the capacity drops significantly, often to levels of 20-30% of the nominal value.
- Wall thickness – the thinner the sheet, the weaker the hold. Part of the magnetic field passes through the material instead of generating force.
- Metal type – different alloys reacts the same. Alloy additives weaken the interaction with the magnet.
- Surface quality – the smoother and more polished the surface, the larger the contact zone and higher the lifting capacity. Roughness creates an air distance.
- Operating temperature – NdFeB sinters have a sensitivity to temperature. When it is hot they are weaker, and at low temperatures they can be stronger (up to a certain limit).
Holding force was checked on a smooth steel plate of 20 mm thickness, when a perpendicular force was applied, whereas under attempts to slide the magnet the load capacity is reduced by as much as fivefold. In addition, even a slight gap between the magnet and the plate lowers the lifting capacity.
Medical implants
Patients with a pacemaker have to maintain an absolute distance from magnets. The magnetic field can interfere with the operation of the life-saving device.
Crushing risk
Big blocks can crush fingers instantly. Under no circumstances put your hand betwixt two strong magnets.
Machining danger
Fire hazard: Neodymium dust is explosive. Avoid machining magnets without safety gear as this risks ignition.
Conscious usage
Handle with care. Rare earth magnets attract from a distance and snap with massive power, often quicker than you can react.
GPS and phone interference
GPS units and smartphones are extremely sensitive to magnetism. Close proximity with a strong magnet can permanently damage the internal compass in your phone.
Electronic devices
Avoid bringing magnets close to a purse, laptop, or TV. The magnetic field can irreversibly ruin these devices and wipe information from cards.
Danger to the youngest
Neodymium magnets are not suitable for play. Swallowing multiple magnets can lead to them connecting inside the digestive tract, which constitutes a critical condition and requires immediate surgery.
Material brittleness
Protect your eyes. Magnets can fracture upon violent connection, launching shards into the air. We recommend safety glasses.
Demagnetization risk
Control the heat. Exposing the magnet to high heat will ruin its properties and pulling force.
Skin irritation risks
Warning for allergy sufferers: The nickel-copper-nickel coating contains nickel. If skin irritation appears, cease working with magnets and wear gloves.
