MW 21.9x10 / N38 - cylindrical magnet
cylindrical magnet
Catalog no 010045
GTIN/EAN: 5906301810445
- Diameter Ø
- 21.9 mm [±0,1 mm]
- Height
- 10 mm [±0,1 mm]
- Weight
- 28.25 g
- Magnetization Direction
- → diametrical
- Coating
- [NiCuNi] Nickel
15.50 zł with VAT / pcs + price for transport
12.60 zł net + 23% VAT / pcs
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Technical - MW 21.9x10 / N38 - cylindrical magnet
Specification / characteristics - MW 21.9x10 / N38 - cylindrical magnet
| properties | values |
|---|---|
| Cat. no. | 010045 |
| GTIN/EAN | 5906301810445 |
| Production/Distribution | Dhit sp. z o.o. |
| Country of origin | Poland / China / Germany |
| Customs code | 85059029 |
| Diameter Ø | 21.9 mm [±0,1 mm] |
| Height | 10 mm [±0,1 mm] |
| Weight | 28.25 g |
| Magnetization Direction | → diametrical |
| Load capacity ~ ? | 14.65 kg / 143.71 N |
| Magnetic Induction ~ ? | 417.89 mT / 4179 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 |
Physical analysis of the magnet - technical parameters
Presented data are the direct effect of a mathematical calculation. Values were calculated on algorithms for the class Nd2Fe14B. Real-world parameters might slightly differ from theoretical values. Please consider these calculations as a supplementary guide when designing systems.
Table 1: Static force (force vs gap) - characteristics
MW 21.9x10 / N38
| Distance (mm) | Induction (Gauss) / mT | Pull Force (kg/lbs/g/N) | Risk Status |
|---|---|---|---|
| 0 mm |
4178 Gs
417.8 mT
|
14.65 kg / 32.30 pounds
14650.0 g / 143.7 N
|
dangerous! |
| 1 mm |
3830 Gs
383.0 mT
|
12.31 kg / 27.15 pounds
12314.7 g / 120.8 N
|
dangerous! |
| 2 mm |
3466 Gs
346.6 mT
|
10.08 kg / 22.23 pounds
10083.5 g / 98.9 N
|
dangerous! |
| 3 mm |
3104 Gs
310.4 mT
|
8.09 kg / 17.83 pounds
8086.3 g / 79.3 N
|
strong |
| 5 mm |
2432 Gs
243.2 mT
|
4.97 kg / 10.95 pounds
4966.5 g / 48.7 N
|
strong |
| 10 mm |
1257 Gs
125.7 mT
|
1.33 kg / 2.93 pounds
1327.0 g / 13.0 N
|
safe |
| 15 mm |
671 Gs
67.1 mT
|
0.38 kg / 0.83 pounds
378.5 g / 3.7 N
|
safe |
| 20 mm |
386 Gs
38.6 mT
|
0.13 kg / 0.28 pounds
125.0 g / 1.2 N
|
safe |
| 30 mm |
156 Gs
15.6 mT
|
0.02 kg / 0.04 pounds
20.4 g / 0.2 N
|
safe |
| 50 mm |
43 Gs
4.3 mT
|
0.00 kg / 0.00 pounds
1.5 g / 0.0 N
|
safe |
Table 2: Vertical hold (vertical surface)
MW 21.9x10 / N38
| Distance (mm) | Friction coefficient | Pull Force (kg/lbs/g/N) |
|---|---|---|
| 0 mm | Stal (~0.2) |
2.93 kg / 6.46 pounds
2930.0 g / 28.7 N
|
| 1 mm | Stal (~0.2) |
2.46 kg / 5.43 pounds
2462.0 g / 24.2 N
|
| 2 mm | Stal (~0.2) |
2.02 kg / 4.44 pounds
2016.0 g / 19.8 N
|
| 3 mm | Stal (~0.2) |
1.62 kg / 3.57 pounds
1618.0 g / 15.9 N
|
| 5 mm | Stal (~0.2) |
0.99 kg / 2.19 pounds
994.0 g / 9.8 N
|
| 10 mm | Stal (~0.2) |
0.27 kg / 0.59 pounds
266.0 g / 2.6 N
|
| 15 mm | Stal (~0.2) |
0.08 kg / 0.17 pounds
76.0 g / 0.7 N
|
| 20 mm | Stal (~0.2) |
0.03 kg / 0.06 pounds
26.0 g / 0.3 N
|
| 30 mm | Stal (~0.2) |
0.00 kg / 0.01 pounds
4.0 g / 0.0 N
|
| 50 mm | Stal (~0.2) |
0.00 kg / 0.00 pounds
0.0 g / 0.0 N
|
Table 3: Vertical assembly (sliding) - vertical pull
MW 21.9x10 / N38
| Surface type | Friction coefficient / % Mocy | Max load (kg/lbs/g/N) |
|---|---|---|
| Raw steel |
µ = 0.3
30% Nominalnej Siły
|
4.40 kg / 9.69 pounds
4395.0 g / 43.1 N
|
| Painted steel (standard) |
µ = 0.2
20% Nominalnej Siły
|
2.93 kg / 6.46 pounds
2930.0 g / 28.7 N
|
| Oily/slippery steel |
µ = 0.1
10% Nominalnej Siły
|
1.47 kg / 3.23 pounds
1465.0 g / 14.4 N
|
| Magnet with anti-slip rubber |
µ = 0.5
50% Nominalnej Siły
|
7.33 kg / 16.15 pounds
7325.0 g / 71.9 N
|
Table 4: Material efficiency (saturation) - power losses
MW 21.9x10 / N38
| Steel thickness (mm) | % power | Real pull force (kg/lbs/g/N) |
|---|---|---|
| 0.5 mm |
|
0.73 kg / 1.61 pounds
732.5 g / 7.2 N
|
| 1 mm |
|
1.83 kg / 4.04 pounds
1831.3 g / 18.0 N
|
| 2 mm |
|
3.66 kg / 8.07 pounds
3662.5 g / 35.9 N
|
| 3 mm |
|
5.49 kg / 12.11 pounds
5493.8 g / 53.9 N
|
| 5 mm |
|
9.16 kg / 20.19 pounds
9156.3 g / 89.8 N
|
| 10 mm |
|
14.65 kg / 32.30 pounds
14650.0 g / 143.7 N
|
| 11 mm |
|
14.65 kg / 32.30 pounds
14650.0 g / 143.7 N
|
| 12 mm |
|
14.65 kg / 32.30 pounds
14650.0 g / 143.7 N
|
Table 5: Thermal stability (material behavior) - resistance threshold
MW 21.9x10 / N38
| Ambient temp. (°C) | Power loss | Remaining pull (kg/lbs/g/N) | Status |
|---|---|---|---|
| 20 °C | 0.0% |
14.65 kg / 32.30 pounds
14650.0 g / 143.7 N
|
OK |
| 40 °C | -2.2% |
14.33 kg / 31.59 pounds
14327.7 g / 140.6 N
|
OK |
| 60 °C | -4.4% |
14.01 kg / 30.88 pounds
14005.4 g / 137.4 N
|
|
| 80 °C | -6.6% |
13.68 kg / 30.17 pounds
13683.1 g / 134.2 N
|
|
| 100 °C | -28.8% |
10.43 kg / 23.00 pounds
10430.8 g / 102.3 N
|
Table 6: Magnet-Magnet interaction (attraction) - forces in the system
MW 21.9x10 / N38
| Gap (mm) | Attraction (kg/lbs) (N-S) | Sliding Force (kg/lbs/g/N) | Repulsion (kg/lbs) (N-N) |
|---|---|---|---|
| 0 mm |
40.53 kg / 89.35 pounds
5 433 Gs
|
6.08 kg / 13.40 pounds
6079 g / 59.6 N
|
N/A |
| 1 mm |
37.31 kg / 82.26 pounds
8 017 Gs
|
5.60 kg / 12.34 pounds
5597 g / 54.9 N
|
33.58 kg / 74.03 pounds
~0 Gs
|
| 2 mm |
34.07 kg / 75.11 pounds
7 660 Gs
|
5.11 kg / 11.27 pounds
5110 g / 50.1 N
|
30.66 kg / 67.60 pounds
~0 Gs
|
| 3 mm |
30.92 kg / 68.16 pounds
7 297 Gs
|
4.64 kg / 10.22 pounds
4637 g / 45.5 N
|
27.82 kg / 61.34 pounds
~0 Gs
|
| 5 mm |
25.04 kg / 55.20 pounds
6 567 Gs
|
3.76 kg / 8.28 pounds
3756 g / 36.8 N
|
22.54 kg / 49.68 pounds
~0 Gs
|
| 10 mm |
13.74 kg / 30.29 pounds
4 865 Gs
|
2.06 kg / 4.54 pounds
2061 g / 20.2 N
|
12.37 kg / 27.26 pounds
~0 Gs
|
| 20 mm |
3.67 kg / 8.09 pounds
2 515 Gs
|
0.55 kg / 1.21 pounds
551 g / 5.4 N
|
3.30 kg / 7.28 pounds
~0 Gs
|
| 50 mm |
0.13 kg / 0.29 pounds
476 Gs
|
0.02 kg / 0.04 pounds
20 g / 0.2 N
|
0.12 kg / 0.26 pounds
~0 Gs
|
| 60 mm |
0.06 kg / 0.12 pounds
312 Gs
|
0.01 kg / 0.02 pounds
8 g / 0.1 N
|
0.05 kg / 0.11 pounds
~0 Gs
|
| 70 mm |
0.03 kg / 0.06 pounds
214 Gs
|
0.00 kg / 0.01 pounds
4 g / 0.0 N
|
0.02 kg / 0.05 pounds
~0 Gs
|
| 80 mm |
0.01 kg / 0.03 pounds
153 Gs
|
0.00 kg / 0.00 pounds
2 g / 0.0 N
|
0.01 kg / 0.03 pounds
~0 Gs
|
| 90 mm |
0.01 kg / 0.02 pounds
113 Gs
|
0.00 kg / 0.00 pounds
1 g / 0.0 N
|
0.00 kg / 0.00 pounds
~0 Gs
|
| 100 mm |
0.00 kg / 0.01 pounds
86 Gs
|
0.00 kg / 0.00 pounds
1 g / 0.0 N
|
0.00 kg / 0.00 pounds
~0 Gs
|
Table 7: Hazards (implants) - precautionary measures
MW 21.9x10 / N38
| Object / Device | Limit (Gauss) / mT | Safe distance |
|---|---|---|
| Pacemaker | 5 Gs (0.5 mT) | 11.0 cm |
| Hearing aid | 10 Gs (1.0 mT) | 9.0 cm |
| Timepiece | 20 Gs (2.0 mT) | 7.0 cm |
| Phone / Smartphone | 40 Gs (4.0 mT) | 5.5 cm |
| Remote | 50 Gs (5.0 mT) | 5.0 cm |
| Payment card | 400 Gs (40.0 mT) | 2.0 cm |
| HDD hard drive | 600 Gs (60.0 mT) | 2.0 cm |
Table 8: Dynamics (cracking risk) - warning
MW 21.9x10 / N38
| Start from (mm) | Speed (km/h) | Energy (J) | Predicted outcome |
|---|---|---|---|
| 10 mm |
23.32 km/h
(6.48 m/s)
|
0.59 J | |
| 30 mm |
24.35 km/h
(6.76 m/s)
|
0.65 J | |
| 50 mm |
24.37 km/h
(6.77 m/s)
|
0.65 J | |
| 100 mm |
24.37 km/h
(6.77 m/s)
|
0.65 J |
Table 9: Corrosion resistance
MW 21.9x10 / 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 (Pc)
MW 21.9x10 / N38
| Parameter | Value | SI Unit / Description |
|---|---|---|
| Magnetic Flux | 16 059 Mx | 160.6 µWb |
| Pc Coefficient | 0.55 | Low (Flat) |
Table 11: Submerged application
MW 21.9x10 / N38
| Environment | Effective steel pull | Effect |
|---|---|---|
| Air (land) | 14.65 kg | Standard |
| Water (riverbed) |
16.77 kg
(+2.12 kg buoyancy gain)
|
+14.5% |
1. Sliding resistance
*Warning: On a vertical wall, the magnet holds only ~20% of its nominal pull.
2. Plate thickness effect
*Thin metal sheet (e.g. computer case) severely weakens the holding force.
3. Power loss vs temp
*For standard magnets, the max working temp is 80°C.
4. Demagnetization curve and operating point (B-H)
chart generated for the permeance coefficient Pc (Permeance Coefficient) = 0.55
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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Pros as well as cons of rare earth magnets.
Strengths
- Their magnetic field is maintained, and after around 10 years it drops only by ~1% (theoretically),
- Magnets very well defend themselves against demagnetization caused by external fields,
- In other words, due to the glossy layer of silver, the element is aesthetically pleasing,
- Neodymium magnets ensure maximum magnetic induction on a small area, which allows for strong attraction,
- Through (appropriate) combination of ingredients, they can achieve high thermal strength, enabling action at temperatures approaching 230°C and above...
- Due to the potential of precise forming and adaptation to unique requirements, NdFeB magnets can be created in a broad palette of shapes and sizes, which amplifies use scope,
- Fundamental importance in modern technologies – they are used in magnetic memories, drive modules, advanced medical instruments, also complex engineering applications.
- Thanks to concentrated force, small magnets offer high operating force, occupying minimum space,
Limitations
- They are fragile upon heavy impacts. To avoid cracks, it is worth securing magnets using a steel holder. Such protection not only protects the magnet but also increases its resistance to damage
- We warn that neodymium magnets can lose their strength at high temperatures. To prevent this, we advise our specialized [AH] magnets, which work effectively even at 230°C.
- Due to the susceptibility of magnets to corrosion in a humid environment, we suggest using waterproof magnets made of rubber, plastic or other material stable to moisture, when using outdoors
- Limited possibility of creating threads in the magnet and complicated shapes - recommended is casing - mounting mechanism.
- Potential hazard related to microscopic parts of magnets pose a threat, when accidentally swallowed, which is particularly important in the context of child safety. Additionally, small elements of these devices can complicate diagnosis medical after entering the body.
- Higher cost of purchase is a significant factor to consider compared to ceramic magnets, especially in budget applications
Pull force analysis
Maximum lifting capacity of the magnet – what it depends on?
- using a base made of high-permeability steel, acting as a magnetic yoke
- with a thickness of at least 10 mm
- characterized by even structure
- without any air gap between the magnet and steel
- during detachment in a direction vertical to the mounting surface
- at conditions approx. 20°C
Determinants of practical lifting force of a magnet
- Distance (between the magnet and the metal), because even a microscopic clearance (e.g. 0.5 mm) leads to a drastic drop in lifting capacity by up to 50% (this also applies to paint, rust or debris).
- Angle of force application – highest force is available only during perpendicular pulling. The shear force of the magnet along the plate is usually many times lower (approx. 1/5 of the lifting capacity).
- 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 – not every steel attracts identically. High carbon content worsen the interaction with the magnet.
- Surface structure – the more even the surface, the better the adhesion and stronger the hold. Roughness creates an air distance.
- Thermal environment – temperature increase causes a temporary drop of force. It is worth remembering the maximum operating temperature for a given model.
Lifting capacity was measured by applying a polished steel plate of suitable thickness (min. 20 mm), under vertically applied force, whereas under attempts to slide the magnet the load capacity is reduced by as much as fivefold. Moreover, even a small distance between the magnet’s surface and the plate reduces the lifting capacity.
Safety rules for work with neodymium magnets
Risk of cracking
Despite metallic appearance, neodymium is delicate and cannot withstand shocks. Do not hit, as the magnet may crumble into sharp, dangerous pieces.
Product not for children
Absolutely keep magnets away from children. Ingestion danger is high, and the consequences of magnets clamping inside the body are tragic.
Serious injuries
Danger of trauma: The pulling power is so great that it can result in blood blisters, pinching, and broken bones. Protective gloves are recommended.
Demagnetization risk
Avoid heat. Neodymium magnets are susceptible to heat. If you need operation above 80°C, inquire about special high-temperature series (H, SH, UH).
Do not underestimate power
Before starting, read the rules. Uncontrolled attraction can destroy the magnet or hurt your hand. Be predictive.
Warning for heart patients
For implant holders: Strong magnetic fields affect electronics. Maintain at least 30 cm distance or ask another person to handle the magnets.
Warning for allergy sufferers
Some people experience a hypersensitivity to nickel, which is the standard coating for neodymium magnets. Prolonged contact might lead to a rash. It is best to use safety gloves.
Cards and drives
Powerful magnetic fields can destroy records on payment cards, HDDs, and storage devices. Stay away of at least 10 cm.
Combustion hazard
Mechanical processing of neodymium magnets carries a risk of fire risk. Magnetic powder oxidizes rapidly with oxygen and is difficult to extinguish.
Magnetic interference
Note: rare earth magnets generate a field that confuses sensitive sensors. Maintain a safe distance from your phone, tablet, and GPS.
