MW 9.5x1 / N38 - cylindrical magnet
cylindrical magnet
Catalog no 010107
GTIN/EAN: 5906301811060
Diameter Ø
9.5 mm [±0,1 mm]
Height
1 mm [±0,1 mm]
Weight
0.53 g
Magnetization Direction
↑ axial
Load capacity
0.40 kg / 3.96 N
Magnetic Induction
127.68 mT / 1277 Gs
Coating
[NiCuNi] Nickel
0.295 ZŁ with VAT / pcs + price for transport
0.240 ZŁ net + 23% VAT / pcs
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Technical - MW 9.5x1 / N38 - cylindrical magnet
Specification / characteristics - MW 9.5x1 / N38 - cylindrical magnet
| properties | values |
|---|---|
| Cat. no. | 010107 |
| GTIN/EAN | 5906301811060 |
| Production/Distribution | Dhit sp. z o.o. |
| Country of origin | Poland / China / Germany |
| Customs code | 85059029 |
| Diameter Ø | 9.5 mm [±0,1 mm] |
| Height | 1 mm [±0,1 mm] |
| Weight | 0.53 g |
| Magnetization Direction | ↑ axial |
| Load capacity ~ ? | 0.40 kg / 3.96 N |
| Magnetic Induction ~ ? | 127.68 mT / 1277 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 |
Engineering analysis of the magnet - data
These data constitute the direct effect of a physical calculation. Values rely on models for the class Nd2Fe14B. Operational parameters may deviate from the simulation results. Use these calculations as a reference point during assembly planning.
Table 1: Static force (force vs distance) - interaction chart
MW 9.5x1 / N38
| Distance (mm) | Induction (Gauss) / mT | Pull Force (kg/lbs/g/N) | Risk Status |
|---|---|---|---|
| 0 mm |
1276 Gs
127.6 mT
|
0.40 kg / 0.88 pounds
400.0 g / 3.9 N
|
weak grip |
| 1 mm |
1129 Gs
112.9 mT
|
0.31 kg / 0.69 pounds
312.8 g / 3.1 N
|
weak grip |
| 2 mm |
905 Gs
90.5 mT
|
0.20 kg / 0.44 pounds
201.0 g / 2.0 N
|
weak grip |
| 3 mm |
683 Gs
68.3 mT
|
0.11 kg / 0.25 pounds
114.5 g / 1.1 N
|
weak grip |
| 5 mm |
366 Gs
36.6 mT
|
0.03 kg / 0.07 pounds
32.9 g / 0.3 N
|
weak grip |
| 10 mm |
92 Gs
9.2 mT
|
0.00 kg / 0.00 pounds
2.1 g / 0.0 N
|
weak grip |
| 15 mm |
33 Gs
3.3 mT
|
0.00 kg / 0.00 pounds
0.3 g / 0.0 N
|
weak grip |
| 20 mm |
15 Gs
1.5 mT
|
0.00 kg / 0.00 pounds
0.1 g / 0.0 N
|
weak grip |
| 30 mm |
5 Gs
0.5 mT
|
0.00 kg / 0.00 pounds
0.0 g / 0.0 N
|
weak grip |
| 50 mm |
1 Gs
0.1 mT
|
0.00 kg / 0.00 pounds
0.0 g / 0.0 N
|
weak grip |
Table 2: Vertical load (wall)
MW 9.5x1 / N38
| Distance (mm) | Friction coefficient | Pull Force (kg/lbs/g/N) |
|---|---|---|
| 0 mm | Stal (~0.2) |
0.08 kg / 0.18 pounds
80.0 g / 0.8 N
|
| 1 mm | Stal (~0.2) |
0.06 kg / 0.14 pounds
62.0 g / 0.6 N
|
| 2 mm | Stal (~0.2) |
0.04 kg / 0.09 pounds
40.0 g / 0.4 N
|
| 3 mm | Stal (~0.2) |
0.02 kg / 0.05 pounds
22.0 g / 0.2 N
|
| 5 mm | Stal (~0.2) |
0.01 kg / 0.01 pounds
6.0 g / 0.1 N
|
| 10 mm | Stal (~0.2) |
0.00 kg / 0.00 pounds
0.0 g / 0.0 N
|
| 15 mm | Stal (~0.2) |
0.00 kg / 0.00 pounds
0.0 g / 0.0 N
|
| 20 mm | Stal (~0.2) |
0.00 kg / 0.00 pounds
0.0 g / 0.0 N
|
| 30 mm | Stal (~0.2) |
0.00 kg / 0.00 pounds
0.0 g / 0.0 N
|
| 50 mm | Stal (~0.2) |
0.00 kg / 0.00 pounds
0.0 g / 0.0 N
|
Table 3: Wall mounting (shearing) - vertical pull
MW 9.5x1 / N38
| Surface type | Friction coefficient / % Mocy | Max load (kg/lbs/g/N) |
|---|---|---|
| Raw steel |
µ = 0.3
30% Nominalnej Siły
|
0.12 kg / 0.26 pounds
120.0 g / 1.2 N
|
| Painted steel (standard) |
µ = 0.2
20% Nominalnej Siły
|
0.08 kg / 0.18 pounds
80.0 g / 0.8 N
|
| Oily/slippery steel |
µ = 0.1
10% Nominalnej Siły
|
0.04 kg / 0.09 pounds
40.0 g / 0.4 N
|
| Magnet with anti-slip rubber |
µ = 0.5
50% Nominalnej Siły
|
0.20 kg / 0.44 pounds
200.0 g / 2.0 N
|
Table 4: Material efficiency (saturation) - power losses
MW 9.5x1 / N38
| Steel thickness (mm) | % power | Real pull force (kg/lbs/g/N) |
|---|---|---|
| 0.5 mm |
|
0.04 kg / 0.09 pounds
40.0 g / 0.4 N
|
| 1 mm |
|
0.10 kg / 0.22 pounds
100.0 g / 1.0 N
|
| 2 mm |
|
0.20 kg / 0.44 pounds
200.0 g / 2.0 N
|
| 3 mm |
|
0.30 kg / 0.66 pounds
300.0 g / 2.9 N
|
| 5 mm |
|
0.40 kg / 0.88 pounds
400.0 g / 3.9 N
|
| 10 mm |
|
0.40 kg / 0.88 pounds
400.0 g / 3.9 N
|
| 11 mm |
|
0.40 kg / 0.88 pounds
400.0 g / 3.9 N
|
| 12 mm |
|
0.40 kg / 0.88 pounds
400.0 g / 3.9 N
|
Table 5: Thermal resistance (material behavior) - resistance threshold
MW 9.5x1 / N38
| Ambient temp. (°C) | Power loss | Remaining pull (kg/lbs/g/N) | Status |
|---|---|---|---|
| 20 °C | 0.0% |
0.40 kg / 0.88 pounds
400.0 g / 3.9 N
|
OK |
| 40 °C | -2.2% |
0.39 kg / 0.86 pounds
391.2 g / 3.8 N
|
OK |
| 60 °C | -4.4% |
0.38 kg / 0.84 pounds
382.4 g / 3.8 N
|
|
| 80 °C | -6.6% |
0.37 kg / 0.82 pounds
373.6 g / 3.7 N
|
|
| 100 °C | -28.8% |
0.28 kg / 0.63 pounds
284.8 g / 2.8 N
|
Table 6: Two magnets (attraction) - field collision
MW 9.5x1 / N38
| Gap (mm) | Attraction (kg/lbs) (N-S) | Shear Strength (kg/lbs/g/N) | Repulsion (kg/lbs) (N-N) |
|---|---|---|---|
| 0 mm |
0.71 kg / 1.57 pounds
2 403 Gs
|
0.11 kg / 0.24 pounds
107 g / 1.0 N
|
N/A |
| 1 mm |
0.65 kg / 1.43 pounds
2 436 Gs
|
0.10 kg / 0.21 pounds
97 g / 1.0 N
|
0.58 kg / 1.29 pounds
~0 Gs
|
| 2 mm |
0.56 kg / 1.23 pounds
2 257 Gs
|
0.08 kg / 0.18 pounds
84 g / 0.8 N
|
0.50 kg / 1.10 pounds
~0 Gs
|
| 3 mm |
0.46 kg / 1.00 pounds
2 041 Gs
|
0.07 kg / 0.15 pounds
68 g / 0.7 N
|
0.41 kg / 0.90 pounds
~0 Gs
|
| 5 mm |
0.27 kg / 0.60 pounds
1 580 Gs
|
0.04 kg / 0.09 pounds
41 g / 0.4 N
|
0.25 kg / 0.54 pounds
~0 Gs
|
| 10 mm |
0.06 kg / 0.13 pounds
732 Gs
|
0.01 kg / 0.02 pounds
9 g / 0.1 N
|
0.05 kg / 0.12 pounds
~0 Gs
|
| 20 mm |
0.00 kg / 0.01 pounds
183 Gs
|
0.00 kg / 0.00 pounds
1 g / 0.0 N
|
0.00 kg / 0.00 pounds
~0 Gs
|
| 50 mm |
0.00 kg / 0.00 pounds
16 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
10 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
6 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
4 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
3 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
2 Gs
|
0.00 kg / 0.00 pounds
0 g / 0.0 N
|
0.00 kg / 0.00 pounds
~0 Gs
|
Table 7: Safety (HSE) (electronics) - precautionary measures
MW 9.5x1 / N38
| Object / Device | Limit (Gauss) / mT | Safe distance |
|---|---|---|
| Pacemaker | 5 Gs (0.5 mT) | 3.0 cm |
| Hearing aid | 10 Gs (1.0 mT) | 2.5 cm |
| Timepiece | 20 Gs (2.0 mT) | 2.0 cm |
| Mobile device | 40 Gs (4.0 mT) | 1.5 cm |
| Remote | 50 Gs (5.0 mT) | 1.5 cm |
| Payment card | 400 Gs (40.0 mT) | 0.5 cm |
| HDD hard drive | 600 Gs (60.0 mT) | 0.5 cm |
Table 8: Impact energy (cracking risk) - collision effects
MW 9.5x1 / N38
| Start from (mm) | Speed (km/h) | Energy (J) | Predicted outcome |
|---|---|---|---|
| 10 mm |
27.80 km/h
(7.72 m/s)
|
0.02 J | |
| 30 mm |
47.99 km/h
(13.33 m/s)
|
0.05 J | |
| 50 mm |
61.95 km/h
(17.21 m/s)
|
0.08 J | |
| 100 mm |
87.61 km/h
(24.34 m/s)
|
0.16 J |
Table 9: Anti-corrosion coating durability
MW 9.5x1 / 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 (Flux)
MW 9.5x1 / N38
| Parameter | Value | SI Unit / Description |
|---|---|---|
| Magnetic Flux | 1 184 Mx | 11.8 µWb |
| Pc Coefficient | 0.16 | Low (Flat) |
Table 11: Physics of underwater searching
MW 9.5x1 / N38
| Environment | Effective steel pull | Effect |
|---|---|---|
| Air (land) | 0.40 kg | Standard |
| Water (riverbed) |
0.46 kg
(+0.06 kg buoyancy gain)
|
+14.5% |
1. Sliding resistance
*Caution: On a vertical wall, the magnet holds merely a fraction of its max power.
2. Plate thickness effect
*Thin steel (e.g. 0.5mm PC case) significantly reduces the holding force.
3. Thermal stability
*For N38 grade, the critical limit is 80°C.
4. Demagnetization curve and operating point (B-H)
chart generated for the permeance coefficient Pc (Permeance Coefficient) = 0.16
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 Nd2Fe14B magnets.
Pros
- They have unchanged lifting capacity, and over around 10 years their performance decreases symbolically – ~1% (according to theory),
- Magnets very well resist against loss of magnetization caused by external fields,
- Thanks to the shimmering finish, the layer of Ni-Cu-Ni, gold, or silver-plated gives an modern appearance,
- The surface of neodymium magnets generates a unique magnetic field – this is a distinguishing feature,
- Due to their durability and thermal resistance, neodymium magnets are capable of operate (depending on the shape) even at high temperatures reaching 230°C or more...
- Thanks to versatility in designing and the capacity to adapt to individual projects,
- Fundamental importance in innovative solutions – they serve a role in magnetic memories, brushless drives, advanced medical instruments, also technologically advanced constructions.
- Thanks to their power density, small magnets offer high operating force, with minimal size,
Limitations
- To avoid cracks under impact, we recommend using special steel holders. Such a solution protects the magnet and simultaneously increases its durability.
- Neodymium magnets decrease their strength under the influence of heating. As soon as 80°C is exceeded, many of them start losing their force. Therefore, we recommend our special magnets marked [AH], which maintain stability even at temperatures up to 230°C
- Due to the susceptibility of magnets to corrosion in a humid environment, we recommend using waterproof magnets made of rubber, plastic or other material immune to moisture, in case of application outdoors
- Due to limitations in creating threads and complex forms in magnets, we propose using cover - magnetic holder.
- Health risk resulting from small fragments of magnets pose a threat, in case of ingestion, which becomes key in the context of child health protection. It is also worth noting that small elements of these devices are able to disrupt the diagnostic process medical in case of swallowing.
- With mass production the cost of neodymium magnets is economically unviable,
Holding force characteristics
Optimal lifting capacity of a neodymium magnet – what contributes to it?
- on a plate made of mild steel, perfectly concentrating the magnetic flux
- with a cross-section no less than 10 mm
- characterized by smoothness
- under conditions of ideal adhesion (metal-to-metal)
- under vertical application of breakaway force (90-degree angle)
- in stable room temperature
Lifting capacity in practice – influencing factors
- Air gap (between the magnet and the plate), since 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 paint, rust or debris).
- Pull-off angle – remember that the magnet holds strongest perpendicularly. Under shear forces, the holding force drops significantly, often to levels of 20-30% of the maximum value.
- Steel thickness – insufficiently thick steel causes magnetic saturation, causing part of the power to be lost into the air.
- Chemical composition of the base – mild steel gives the best results. Alloy steels lower magnetic permeability and holding force.
- Plate texture – smooth surfaces ensure maximum contact, which improves field saturation. Rough surfaces weaken the grip.
- Thermal conditions – NdFeB sinters have a sensitivity to temperature. When it is hot they are weaker, and at low temperatures gain strength (up to a certain limit).
Lifting capacity testing was conducted on a smooth plate of optimal thickness, under perpendicular forces, in contrast under parallel forces the lifting capacity is smaller. Moreover, even a slight gap between the magnet and the plate reduces the holding force.
Precautions when working with neodymium magnets
Threat to navigation
Remember: rare earth magnets produce a field that confuses precision electronics. Keep a separation from your mobile, tablet, and GPS.
Operating temperature
Control the heat. Exposing the magnet to high heat will destroy its properties and strength.
Skin irritation risks
Some people suffer from a contact allergy to nickel, which is the common plating for neodymium magnets. Prolonged contact may cause an allergic reaction. We suggest wear protective gloves.
Do not underestimate power
Handle magnets consciously. Their powerful strength can surprise even professionals. Be vigilant and do not underestimate their force.
Keep away from computers
Equipment safety: Neodymium magnets can damage data carriers and sensitive devices (heart implants, hearing aids, timepieces).
This is not a toy
Neodymium magnets are not suitable for play. Accidental ingestion of several magnets can lead to them connecting inside the digestive tract, which poses a direct threat to life and necessitates immediate surgery.
Dust explosion hazard
Machining of NdFeB material poses a fire risk. Magnetic powder reacts violently with oxygen and is hard to extinguish.
Finger safety
Large magnets can break fingers in a fraction of a second. Never place your hand between two strong magnets.
Medical interference
Individuals with a heart stimulator should maintain an safe separation from magnets. The magnetism can interfere with the operation of the life-saving device.
Risk of cracking
Watch out for shards. Magnets can explode upon violent connection, launching shards into the air. Eye protection is mandatory.
