MW 3x1 zestaw 100 szt. / N38 - cylindrical magnet
cylindrical magnet
Catalog no 010548
GTIN/EAN: 5906301815396
- Diameter Ø
- 3 mm [±0,1 mm]
- Height
- 1 mm [±0,1 mm]
- Weight
- 5 g
- Magnetization Direction
- ↑ axial
- Coating
- [NiCuNi] Nickel
How we measure these parameters — certificates and measurements
10.56 zł net / pcs
12.99 zł with VAT (23% VAT) / pcs
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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 3x1 zestaw 100 szt. / N38 - cylindrical magnet
Specification / characteristics - MW 3x1 zestaw 100 szt. / N38 - cylindrical magnet
| properties | values |
|---|---|
| Cat. no. | 010548 |
| GTIN/EAN | 5906301815396 |
| Distributor | Dhit sp. z o.o. |
| Country of origin | Poland / China / Germany |
| Customs code | 85059029 |
| Diameter Ø | 3 mm [±0,1 mm] |
| Height | 1 mm [±0,1 mm] |
| Weight | 5 g |
| Magnetization Direction | ↑ axial |
| Load capacity ~ ? | 0.21 kg / 2.10 N |
| Magnetic Induction ~ ? | 342.82 mT / 3428 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 |
Technical modeling of the assembly - data
Presented data represent the direct effect of a mathematical calculation. Values are based on algorithms for the material Nd2Fe14B. Real-world conditions may differ. Use these calculations as a supplementary guide for designers.
Table 1: Static force (pull vs gap) - interaction chart
MW 3x1 zestaw 100 szt. / N38
| Distance (mm) | Induction (Gauss) / mT | Pull Force (kg/lbs/g/N) | Risk Status |
|---|---|---|---|
| 0 mm |
3422 Gs
342.2 mT
|
0.21 kg / 0.46 lbs
210.0 g / 2.1 N
|
low risk |
| 1 mm |
1521 Gs
152.1 mT
|
0.04 kg / 0.09 lbs
41.5 g / 0.4 N
|
low risk |
| 2 mm |
585 Gs
58.5 mT
|
0.01 kg / 0.01 lbs
6.1 g / 0.1 N
|
low risk |
| 3 mm |
260 Gs
26.0 mT
|
0.00 kg / 0.00 lbs
1.2 g / 0.0 N
|
low risk |
| 5 mm |
76 Gs
7.6 mT
|
0.00 kg / 0.00 lbs
0.1 g / 0.0 N
|
low risk |
| 10 mm |
12 Gs
1.2 mT
|
0.00 kg / 0.00 lbs
0.0 g / 0.0 N
|
low risk |
| 15 mm |
4 Gs
0.4 mT
|
0.00 kg / 0.00 lbs
0.0 g / 0.0 N
|
low risk |
| 20 mm |
2 Gs
0.2 mT
|
0.00 kg / 0.00 lbs
0.0 g / 0.0 N
|
low risk |
| 30 mm |
0 Gs
0.0 mT
|
0.00 kg / 0.00 lbs
0.0 g / 0.0 N
|
low risk |
| 50 mm |
0 Gs
0.0 mT
|
0.00 kg / 0.00 lbs
0.0 g / 0.0 N
|
low risk |
Table 2: Sliding capacity (vertical surface)
MW 3x1 zestaw 100 szt. / N38
| Distance (mm) | Friction coefficient | Pull Force (kg/lbs/g/N) |
|---|---|---|
| 0 mm | Raw steel (µ ≈ 0.2) |
0.04 kg / 0.09 lbs
42.0 g / 0.4 N
|
| 1 mm | Raw steel (µ ≈ 0.2) |
0.01 kg / 0.02 lbs
8.0 g / 0.1 N
|
| 2 mm | Raw steel (µ ≈ 0.2) |
0.00 kg / 0.00 lbs
2.0 g / 0.0 N
|
| 3 mm | Raw steel (µ ≈ 0.2) |
0.00 kg / 0.00 lbs
0.0 g / 0.0 N
|
| 5 mm | Raw steel (µ ≈ 0.2) |
0.00 kg / 0.00 lbs
0.0 g / 0.0 N
|
| 10 mm | Raw steel (µ ≈ 0.2) |
0.00 kg / 0.00 lbs
0.0 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 (sliding) - vertical pull
MW 3x1 zestaw 100 szt. / N38
| Surface type | Friction coefficient / % | Max load (kg/lbs/g/N) |
|---|---|---|
| Raw steel |
µ = 0.3
30% of nominal force
|
0.06 kg / 0.14 lbs
63.0 g / 0.6 N
|
| Painted steel (standard) |
µ = 0.2
20% of nominal force
|
0.04 kg / 0.09 lbs
42.0 g / 0.4 N
|
| Oily/slippery steel |
µ = 0.1
10% of nominal force
|
0.02 kg / 0.05 lbs
21.0 g / 0.2 N
|
| Magnet with anti-slip rubber |
µ = 0.5
50% of nominal force
|
0.11 kg / 0.23 lbs
105.0 g / 1.0 N
|
Table 4: Material efficiency (saturation) - power losses
MW 3x1 zestaw 100 szt. / N38
| Steel thickness (mm) | % power | Real pull force (kg/lbs/g/N) |
|---|---|---|
| 0.5 mm |
|
0.02 kg / 0.05 lbs
21.0 g / 0.2 N
|
| 1 mm |
|
0.05 kg / 0.12 lbs
52.5 g / 0.5 N
|
| 2 mm |
|
0.11 kg / 0.23 lbs
105.0 g / 1.0 N
|
| 3 mm |
|
0.16 kg / 0.35 lbs
157.5 g / 1.5 N
|
| 5 mm |
|
0.21 kg / 0.46 lbs
210.0 g / 2.1 N
|
| 10 mm |
|
0.21 kg / 0.46 lbs
210.0 g / 2.1 N
|
| 11 mm |
|
0.21 kg / 0.46 lbs
210.0 g / 2.1 N
|
| 12 mm |
|
0.21 kg / 0.46 lbs
210.0 g / 2.1 N
|
Table 5: Working in heat (stability) - power drop
MW 3x1 zestaw 100 szt. / N38
| Magnet temperature (°C) | Force change relative to 20°C | Remaining pull (kg/lbs/g/N) | Status |
|---|---|---|---|
| 20 °C | 0.0% |
0.21 kg / 0.46 lbs
210.0 g / 2.1 N
|
Estimate |
| 40 °C | -4.4% |
0.20 kg / 0.44 lbs
200.9 g / 2.0 N
|
Estimate |
| 60 °C | -8.6% |
0.19 kg / 0.42 lbs
191.9 g / 1.9 N
|
Estimate |
| 80 °C | -12.8% |
0.18 kg / 0.40 lbs
183.2 g / 1.8 N
|
Material limit |
| 100 °C | — | — | Out of range — no model |
Table 6: Magnet-Magnet interaction (repulsion) - forces in the system
MW 3x1 zestaw 100 szt. / N38
| Gap (mm) | Attraction (kg/lbs) (N-S) | Sliding Force (kg/lbs/g/N) | Repulsion (kg/lbs) (N-N) |
|---|---|---|---|
| 0 mm |
0.51 kg / 1.12 lbs
4 928 Gs
|
0.08 kg / 0.17 lbs
77 g / 0.8 N
|
N/A |
| 1 mm |
0.26 kg / 0.56 lbs
4 847 Gs
|
0.04 kg / 0.08 lbs
38 g / 0.4 N
|
0.23 kg / 0.51 lbs
~0 Gs
|
| 2 mm |
0.10 kg / 0.22 lbs
3 042 Gs
|
0.02 kg / 0.03 lbs
15 g / 0.1 N
|
0.09 kg / 0.20 lbs
~0 Gs
|
| 3 mm |
0.04 kg / 0.08 lbs
1 865 Gs
|
0.01 kg / 0.01 lbs
6 g / 0.1 N
|
0.03 kg / 0.08 lbs
~0 Gs
|
| 5 mm |
0.01 kg / 0.01 lbs
764 Gs
|
0.00 kg / 0.00 lbs
1 g / 0.0 N
|
0.00 kg / 0.00 lbs
~0 Gs
|
| 10 mm |
0.00 kg / 0.00 lbs
153 Gs
|
0.00 kg / 0.00 lbs
0 g / 0.0 N
|
0.00 kg / 0.00 lbs
~0 Gs
|
| 20 mm |
0.00 kg / 0.00 lbs
23 Gs
|
0.00 kg / 0.00 lbs
0 g / 0.0 N
|
0.00 kg / 0.00 lbs
~0 Gs
|
| 50 mm |
0.00 kg / 0.00 lbs
2 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
1 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
1 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
0 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
0 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
0 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 3x1 zestaw 100 szt. / N38
| Field level (Gs) | mT | Model distance (cm) |
|---|---|---|
| < 5 Gs | < 0.5 mT | 1.5 cm |
| < 10 Gs | < 1.0 mT | 1.5 cm |
| < 20 Gs | < 2.0 mT | 1.0 cm |
| < 40 Gs | < 4.0 mT | 1.0 cm |
| < 50 Gs | < 5.0 mT | 1.0 cm |
| < 400 Gs | < 40.0 mT | 0.5 cm |
| < 600 Gs | < 60.0 mT | 0.5 cm |
Table 8: Dynamics (cracking risk) - warning
MW 3x1 zestaw 100 szt. / N38
| Start from (mm) | Speed (km/h) | Energy (J) | Predicted outcome |
|---|---|---|---|
| 10 mm |
2.62 km/h
(0.73 m/s)
|
0.00 J | |
| 30 mm |
2.62 km/h
(0.73 m/s)
|
0.00 J | |
| 50 mm |
2.62 km/h
(0.73 m/s)
|
0.00 J | |
| 100 mm |
2.62 km/h
(0.73 m/s)
|
0.00 J |
Table 9: Corrosion resistance
MW 3x1 zestaw 100 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: Construction data (Pc)
MW 3x1 zestaw 100 szt. / N38
| Parameter | Value | SI Unit / Description |
|---|---|---|
| Magnetic Flux | 257 Mx | 2.6 µWb |
| Pc Coefficient | 0.44 | Low (Flat) |
Table 11: Hydrostatics and buoyancy
MW 3x1 zestaw 100 szt. / N38
| Environment | Effective steel pull | Effect |
|---|---|---|
| Air (land) | 0.21 kg | Standard |
| Water (riverbed) |
0.24 kg
(+0.03 kg buoyancy gain)
|
+14.5% |
1. Sliding resistance
*Warning: On a vertical wall, the magnet holds just a fraction of its nominal pull.
2. Steel saturation
*Thin steel (e.g. 0.5mm PC case) severely weakens 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) = 0.44
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% |
Environmental data
| recyclability (EoL) | 100% |
| recycled raw materials | ~10% (pre-cons) |
| carbon footprint | low / zredukowany |
| waste code (EWC) | 16 02 16 |
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Strengths as well as weaknesses of rare earth magnets.
Advantages
- They virtually do not lose power, because even after 10 years the performance loss is only ~1% (in laboratory conditions),
- They possess excellent resistance to magnetic field loss as a result of external magnetic sources,
- The use of an metallic layer of noble metals (nickel, gold, silver) causes the element to look better,
- Magnets are distinguished by huge magnetic induction on the surface,
- Due to their durability and thermal resistance, neodymium magnets can operate (depending on the form) even at high temperatures reaching 230°C or more...
- Thanks to versatility in forming and the ability to adapt to unusual requirements,
- Huge importance in innovative solutions – they are commonly used in computer drives, electric motors, diagnostic systems, as well as technologically advanced constructions.
- Thanks to their power density, small magnets offer high operating force, occupying minimum space,
Disadvantages
- Brittleness is one of their disadvantages. Upon intense impact they can break. We recommend 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.
- When exposed to humidity, magnets usually rust. For applications outside, it is recommended to use protective magnets, such as magnets in rubber or plastics, which secure oxidation as well as corrosion.
- We recommend cover - magnetic mount, due to difficulties in realizing nuts inside the magnet and complex forms.
- Possible danger resulting from small fragments of magnets pose a threat, in case of ingestion, which gains importance in the context of child safety. It is also worth noting that small components of these magnets can disrupt the diagnostic process medical in case of swallowing.
- Due to complex production process, their price is relatively high,
Holding force characteristics
Highest magnetic holding force – what affects it?
- with the use of a sheet made of low-carbon steel, ensuring maximum field concentration
- with a cross-section no less than 10 mm
- with a plane perfectly flat
- with zero gap (no paint)
- during detachment in a direction perpendicular to the mounting surface
- in temp. approx. 20°C
Determinants of lifting force in real conditions
- Space between surfaces – every millimeter of separation (caused e.g. by varnish or unevenness) drastically reduces the pulling force, often by half at just 0.5 mm.
- Pull-off angle – note that the magnet holds strongest perpendicularly. Under sliding down, the capacity drops significantly, often to levels of 20-30% of the maximum value.
- Plate thickness – too thin plate causes magnetic saturation, causing part of the flux to be lost to the other side.
- Material type – ideal substrate is pure iron steel. Cast iron may have worse magnetic properties.
- Smoothness – full contact is possible only on smooth steel. Rough texture create air cushions, weakening the magnet.
- Thermal environment – heating the magnet results in weakening of force. It is worth remembering the thermal limit for a given model.
Holding force was measured on the plate surface of 20 mm thickness, when a perpendicular force was applied, whereas under parallel forces the load capacity is reduced by as much as 5 times. Moreover, even a minimal clearance between the magnet and the plate decreases the lifting capacity.
Precautions when working with NdFeB magnets
No play value
Absolutely keep magnets away from children. Ingestion danger is significant, and the consequences of magnets connecting inside the body are tragic.
Thermal limits
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.
Handling guide
Be careful. Neodymium magnets act from a distance and snap with massive power, often quicker than you can move away.
Threat to navigation
A strong magnetic field interferes with the operation of compasses in phones and GPS navigation. Do not bring magnets near a smartphone to prevent damaging the sensors.
Hand protection
Danger of trauma: The attraction force is so immense that it can cause blood blisters, pinching, and broken bones. Protective gloves are recommended.
Metal Allergy
A percentage of the population suffer from a hypersensitivity to Ni, which is the common plating for NdFeB magnets. Prolonged contact may cause an allergic reaction. We recommend wear protective gloves.
Magnetic media
Device Safety: Neodymium magnets can ruin payment cards and sensitive devices (pacemakers, medical aids, mechanical watches).
Danger to pacemakers
Patients with a heart stimulator should keep an safe separation from magnets. The magnetism can stop the operation of the life-saving device.
Risk of cracking
Neodymium magnets are ceramic materials, meaning they are prone to chipping. Collision of two magnets leads to them cracking into small pieces.
Dust is flammable
Fire warning: Neodymium dust is explosive. Avoid machining magnets in home conditions as this risks ignition.
