MW 10x1.5 zestaw 2600 szt. / N38 - cylindrical magnet
cylindrical magnet
Catalog no 010558
GTIN/EAN: 5906301815501
- Diameter Ø
- 10 mm [±0,1 mm]
- Height
- 1.5 mm [±0,1 mm]
- Weight
- 2288 g
- Magnetization Direction
- ↑ axial
- Coating
- [NiCuNi] Nickel
How we measure these parameters — certificates and measurements
731.70 zł net / pcs
899.99 zł with VAT (23% VAT) / pcs
bulk discounts:
Need more?Frequently asked questions
Where can I buy strong cylindrical neodymium magnets?
Can a small cylindrical magnet provide a strong grip for precise workshop work?
Which cylindrical magnet can work at a higher temperature?
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.
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Technical of the product - MW 10x1.5 zestaw 2600 szt. / N38 - cylindrical magnet
Specification / characteristics - MW 10x1.5 zestaw 2600 szt. / N38 - cylindrical magnet
| properties | values |
|---|---|
| Cat. no. | 010558 |
| GTIN/EAN | 5906301815501 |
| Distributor | Dhit sp. z o.o. |
| Country of origin | Poland / China / Germany |
| Customs code | 85059029 |
| Diameter Ø | 10 mm [±0,1 mm] |
| Height | 1.5 mm [±0,1 mm] |
| Weight | 2288 g |
| Magnetization Direction | ↑ axial |
| Load capacity ~ ? | 0.82 kg / 8.01 N |
| Magnetic Induction ~ ? | 178.06 mT / 1781 Gs |
| Coating | [NiCuNi] Nickel |
| Manufacturing Tolerance | ±0.1 mm |
Magnetic properties of material N38
| 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
| 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 |
Engineering simulation of the magnet - technical parameters
The following data represent the outcome of a mathematical simulation. Values were calculated on algorithms for the material Nd2Fe14B. Operational parameters may differ from theoretical values. Treat these calculations as a preliminary roadmap for designers.
Table 1: Static force (pull vs distance) - interaction chart
MW 10x1.5 zestaw 2600 szt. / N38
| Distance (mm) | Induction (Gauss) / mT | Pull Force (kg/lbs/g/N) | Risk Status |
|---|---|---|---|
| 0 mm |
1780 Gs
178.0 mT
|
0.82 kg / 1.81 LBS
820.0 g / 8.0 N
|
safe |
| 1 mm |
1557 Gs
155.7 mT
|
0.63 kg / 1.38 LBS
627.2 g / 6.2 N
|
safe |
| 2 mm |
1253 Gs
125.3 mT
|
0.41 kg / 0.90 LBS
406.2 g / 4.0 N
|
safe |
| 3 mm |
958 Gs
95.8 mT
|
0.24 kg / 0.52 LBS
237.4 g / 2.3 N
|
safe |
| 5 mm |
530 Gs
53.0 mT
|
0.07 kg / 0.16 LBS
72.8 g / 0.7 N
|
safe |
| 10 mm |
140 Gs
14.0 mT
|
0.01 kg / 0.01 LBS
5.1 g / 0.1 N
|
safe |
| 15 mm |
52 Gs
5.2 mT
|
0.00 kg / 0.00 LBS
0.7 g / 0.0 N
|
safe |
| 20 mm |
24 Gs
2.4 mT
|
0.00 kg / 0.00 LBS
0.1 g / 0.0 N
|
safe |
| 30 mm |
8 Gs
0.8 mT
|
0.00 kg / 0.00 LBS
0.0 g / 0.0 N
|
safe |
| 50 mm |
2 Gs
0.2 mT
|
0.00 kg / 0.00 LBS
0.0 g / 0.0 N
|
safe |
Table 2: Vertical capacity (wall)
MW 10x1.5 zestaw 2600 szt. / N38
| Distance (mm) | Friction coefficient | Pull Force (kg/lbs/g/N) |
|---|---|---|
| 0 mm | Raw steel (µ ≈ 0.2) |
0.16 kg / 0.36 LBS
164.0 g / 1.6 N
|
| 1 mm | Raw steel (µ ≈ 0.2) |
0.13 kg / 0.28 LBS
126.0 g / 1.2 N
|
| 2 mm | Raw steel (µ ≈ 0.2) |
0.08 kg / 0.18 LBS
82.0 g / 0.8 N
|
| 3 mm | Raw steel (µ ≈ 0.2) |
0.05 kg / 0.11 LBS
48.0 g / 0.5 N
|
| 5 mm | Raw steel (µ ≈ 0.2) |
0.01 kg / 0.03 LBS
14.0 g / 0.1 N
|
| 10 mm | Raw steel (µ ≈ 0.2) |
0.00 kg / 0.00 LBS
2.0 g / 0.0 N
|
| 15 mm | Raw steel (µ ≈ 0.2) |
0.00 kg / 0.00 LBS
0.0 g / 0.0 N
|
| 20 mm | Raw steel (µ ≈ 0.2) |
0.00 kg / 0.00 LBS
0.0 g / 0.0 N
|
| 30 mm | Raw steel (µ ≈ 0.2) |
0.00 kg / 0.00 LBS
0.0 g / 0.0 N
|
| 50 mm | Raw steel (µ ≈ 0.2) |
0.00 kg / 0.00 LBS
0.0 g / 0.0 N
|
Table 3: Vertical assembly (shearing) - vertical pull
MW 10x1.5 zestaw 2600 szt. / N38
| Surface type | Friction coefficient / % | Max load (kg/lbs/g/N) |
|---|---|---|
| Raw steel |
µ = 0.3
30% of nominal force
|
0.25 kg / 0.54 LBS
246.0 g / 2.4 N
|
| Painted steel (standard) |
µ = 0.2
20% of nominal force
|
0.16 kg / 0.36 LBS
164.0 g / 1.6 N
|
| Oily/slippery steel |
µ = 0.1
10% of nominal force
|
0.08 kg / 0.18 LBS
82.0 g / 0.8 N
|
| Magnet with anti-slip rubber |
µ = 0.5
50% of nominal force
|
0.41 kg / 0.90 LBS
410.0 g / 4.0 N
|
Table 4: Material efficiency (substrate influence) - power losses
MW 10x1.5 zestaw 2600 szt. / N38
| Steel thickness (mm) | % power | Real pull force (kg/lbs/g/N) |
|---|---|---|
| 0.5 mm |
|
0.08 kg / 0.18 LBS
82.0 g / 0.8 N
|
| 1 mm |
|
0.21 kg / 0.45 LBS
205.0 g / 2.0 N
|
| 2 mm |
|
0.41 kg / 0.90 LBS
410.0 g / 4.0 N
|
| 3 mm |
|
0.62 kg / 1.36 LBS
615.0 g / 6.0 N
|
| 5 mm |
|
0.82 kg / 1.81 LBS
820.0 g / 8.0 N
|
| 10 mm |
|
0.82 kg / 1.81 LBS
820.0 g / 8.0 N
|
| 11 mm |
|
0.82 kg / 1.81 LBS
820.0 g / 8.0 N
|
| 12 mm |
|
0.82 kg / 1.81 LBS
820.0 g / 8.0 N
|
Table 5: Thermal stability (material behavior) - resistance threshold
MW 10x1.5 zestaw 2600 szt. / N38
| Magnet temperature (°C) | Force change relative to 20°C | Remaining pull (kg/lbs/g/N) | Status |
|---|---|---|---|
| 20 °C | 0.0% |
0.82 kg / 1.81 LBS
820.0 g / 8.0 N
|
Estimate |
| 40 °C | -4.4% |
0.78 kg / 1.73 LBS
784.3 g / 7.7 N
|
Estimate |
| 60 °C | -8.6% |
0.75 kg / 1.65 LBS
749.4 g / 7.4 N
|
Estimate |
| 80 °C | -12.8% |
0.72 kg / 1.58 LBS
715.3 g / 7.0 N
|
Material limit |
| 100 °C | — | — | Out of range — no model |
Table 6: Magnet-Magnet interaction (attraction) - forces in the system
MW 10x1.5 zestaw 2600 szt. / N38
| Gap (mm) | Attraction (kg/lbs) (N-S) | Sliding Force (kg/lbs/g/N) | Repulsion (kg/lbs) (N-N) |
|---|---|---|---|
| 0 mm |
1.53 kg / 3.38 LBS
3 185 Gs
|
0.23 kg / 0.51 LBS
230 g / 2.3 N
|
N/A |
| 1 mm |
1.38 kg / 3.03 LBS
3 371 Gs
|
0.21 kg / 0.45 LBS
206 g / 2.0 N
|
1.24 kg / 2.73 LBS
~0 Gs
|
| 2 mm |
1.17 kg / 2.59 LBS
3 114 Gs
|
0.18 kg / 0.39 LBS
176 g / 1.7 N
|
1.06 kg / 2.33 LBS
~0 Gs
|
| 3 mm |
0.96 kg / 2.12 LBS
2 817 Gs
|
0.14 kg / 0.32 LBS
144 g / 1.4 N
|
0.86 kg / 1.91 LBS
~0 Gs
|
| 5 mm |
0.59 kg / 1.29 LBS
2 201 Gs
|
0.09 kg / 0.19 LBS
88 g / 0.9 N
|
0.53 kg / 1.16 LBS
~0 Gs
|
| 10 mm |
0.14 kg / 0.30 LBS
1 060 Gs
|
0.02 kg / 0.05 LBS
20 g / 0.2 N
|
0.12 kg / 0.27 LBS
~0 Gs
|
| 20 mm |
0.01 kg / 0.02 LBS
281 Gs
|
0.00 kg / 0.00 LBS
1 g / 0.0 N
|
0.00 kg / 0.00 LBS
~0 Gs
|
| 50 mm |
0.00 kg / 0.00 LBS
26 Gs
|
0.00 kg / 0.00 LBS
0 g / 0.0 N
|
0.00 kg / 0.00 LBS
~0 Gs
|
| 60 mm |
0.00 kg / 0.00 LBS
15 Gs
|
0.00 kg / 0.00 LBS
0 g / 0.0 N
|
0.00 kg / 0.00 LBS
~0 Gs
|
| 70 mm |
0.00 kg / 0.00 LBS
10 Gs
|
0.00 kg / 0.00 LBS
0 g / 0.0 N
|
0.00 kg / 0.00 LBS
~0 Gs
|
| 80 mm |
0.00 kg / 0.00 LBS
7 Gs
|
0.00 kg / 0.00 LBS
0 g / 0.0 N
|
0.00 kg / 0.00 LBS
~0 Gs
|
| 90 mm |
0.00 kg / 0.00 LBS
5 Gs
|
0.00 kg / 0.00 LBS
0 g / 0.0 N
|
0.00 kg / 0.00 LBS
~0 Gs
|
| 100 mm |
0.00 kg / 0.00 LBS
4 Gs
|
0.00 kg / 0.00 LBS
0 g / 0.0 N
|
0.00 kg / 0.00 LBS
~0 Gs
|
Table 7: Axial field levels — not safety zones
MW 10x1.5 zestaw 2600 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 | 2.0 cm |
| < 400 Gs | < 40.0 mT | 1.0 cm |
| < 600 Gs | < 60.0 mT | 0.5 cm |
Table 8: Impact energy (cracking risk) - warning
MW 10x1.5 zestaw 2600 szt. / N38
| Start from (mm) | Speed (km/h) | Energy (J) | Predicted outcome |
|---|---|---|---|
| 10 mm |
0.47 km/h
(0.13 m/s)
|
0.02 J | |
| 30 mm |
0.47 km/h
(0.13 m/s)
|
0.02 J | |
| 50 mm |
0.47 km/h
(0.13 m/s)
|
0.02 J | |
| 100 mm |
0.47 km/h
(0.13 m/s)
|
0.02 J |
Table 9: Anti-corrosion coating durability
MW 10x1.5 zestaw 2600 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) |
Table 10: Electrical data (Flux)
MW 10x1.5 zestaw 2600 szt. / N38
| Parameter | Value | SI Unit / Description |
|---|---|---|
| Magnetic Flux | 1 717 Mx | 17.2 µWb |
| Pc Coefficient | 0.22 | Low (Flat) |
Table 11: Physics of underwater searching
MW 10x1.5 zestaw 2600 szt. / N38
| Environment | Effective steel pull | Effect |
|---|---|---|
| Air (land) | 0.82 kg | Standard |
| Water (riverbed) |
0.94 kg
(+0.12 kg buoyancy gain)
|
+14.5% |
1. Shear force
*Warning: On a vertical surface, the magnet holds merely ~20% of its perpendicular strength.
2. Steel thickness impact
*Thin metal sheet (e.g. computer case) significantly reduces 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) = 0.22
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.
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 |
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Advantages and disadvantages of neodymium magnets.
Strengths
- Their strength is maintained, and after around ten years it drops only by ~1% (theoretically),
- They feature excellent resistance to magnetic field loss due to external magnetic sources,
- By applying a lustrous layer of gold, the element gains an professional look,
- They feature high magnetic induction at the operating surface, which improves attraction properties,
- Thanks to resistance to high temperature, they can operate (depending on the form) even at temperatures up to 230°C and higher...
- Thanks to flexibility in designing and the ability to modify to unusual requirements,
- Fundamental importance in modern industrial fields – they are used in magnetic memories, electromotive mechanisms, medical devices, as well as technologically advanced constructions.
- Thanks to concentrated force, small magnets offer high operating force, with minimal size,
Limitations
- Brittleness is one of their disadvantages. Upon intense impact they can break. We advise keeping them in a strong case, which not only protects them against impacts but also increases their 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 during using outdoors, we suggest using waterproof magnets made of rubber, plastic or other material resistant to moisture
- Due to limitations in producing nuts and complicated forms in magnets, we recommend using casing - magnetic mount.
- Possible danger related to microscopic parts of magnets are risky, when accidentally swallowed, which becomes key in the context of child safety. Additionally, tiny parts of these products can be problematic in diagnostics medical after entering the body.
- Due to complex production process, their price exceeds standard values,
Pull force analysis
Highest magnetic holding force – what it depends on?
- with the application of a sheet made of low-carbon steel, ensuring full magnetic saturation
- whose thickness equals approx. 10 mm
- with an ground touching surface
- with total lack of distance (no paint)
- during pulling in a direction perpendicular to the mounting surface
- in neutral thermal conditions
Key elements affecting lifting force
- Gap between surfaces – even a fraction of a millimeter of separation (caused e.g. by veneer or dirt) diminishes the pulling force, often by half at just 0.5 mm.
- Force direction – note that the magnet has greatest strength perpendicularly. Under sliding down, the holding force drops significantly, often to levels of 20-30% of the nominal value.
- Substrate thickness – for full efficiency, the steel must be sufficiently thick. Paper-thin metal restricts the lifting capacity (the magnet "punches through" it).
- Plate material – mild steel attracts best. Alloy steels decrease magnetic properties and lifting capacity.
- Plate texture – smooth surfaces guarantee perfect abutment, which increases field saturation. Uneven metal weaken the grip.
- Thermal factor – high temperature weakens magnetic field. Too high temperature can permanently damage the magnet.
Lifting capacity testing was performed on a smooth plate of suitable thickness, under a perpendicular pulling force, in contrast under shearing force the lifting capacity is smaller. Moreover, even a slight gap between the magnet’s surface and the plate reduces the lifting capacity.
Precautions when working with neodymium magnets
Magnets are brittle
Neodymium magnets are sintered ceramics, meaning they are fragile like glass. Clashing of two magnets leads to them cracking into small pieces.
Warning for heart patients
Patients with a ICD have to maintain an safe separation from magnets. The magnetism can disrupt the functioning of the implant.
Threat to navigation
A strong magnetic field interferes with the operation of compasses in smartphones and navigation systems. Do not bring magnets close to a smartphone to avoid damaging the sensors.
Operating temperature
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.
Do not give to children
Absolutely store magnets away from children. Ingestion danger is significant, and the consequences of magnets connecting inside the body are fatal.
Physical harm
Protect your hands. Two large magnets will snap together immediately with a force of massive weight, destroying everything in their path. Exercise extreme caution!
Electronic devices
Intense magnetic fields can corrupt files on credit cards, HDDs, and storage devices. Keep a distance of at least 10 cm.
Do not drill into magnets
Machining of neodymium magnets carries a risk of fire hazard. Neodymium dust reacts violently with oxygen and is difficult to extinguish.
Nickel allergy
Warning for allergy sufferers: The nickel-copper-nickel coating consists of nickel. If skin irritation occurs, cease working with magnets and use protective gear.
Powerful field
Handle magnets consciously. Their huge power can shock even experienced users. Be vigilant and do not underestimate their force.
