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
bulk discounts:
Need more?
Pick up the phone and ask
+48 888 99 98 98
alternatively send us a note by means of
our online form
our website.
Specifications as well as form of a magnet can be verified on our
magnetic calculator.
Order by 14:00 and we’ll ship today!
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 |
Physical analysis of the product - technical parameters
Presented data are the result of a physical analysis. Values were calculated on models for the material Nd2Fe14B. Real-world conditions may differ. Please consider these calculations as a preliminary roadmap when designing systems.
Table 1: Static pull force (pull 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 LBS
400.0 g / 3.9 N
|
weak grip |
| 1 mm |
1129 Gs
112.9 mT
|
0.31 kg / 0.69 LBS
312.8 g / 3.1 N
|
weak grip |
| 2 mm |
905 Gs
90.5 mT
|
0.20 kg / 0.44 LBS
201.0 g / 2.0 N
|
weak grip |
| 3 mm |
683 Gs
68.3 mT
|
0.11 kg / 0.25 LBS
114.5 g / 1.1 N
|
weak grip |
| 5 mm |
366 Gs
36.6 mT
|
0.03 kg / 0.07 LBS
32.9 g / 0.3 N
|
weak grip |
| 10 mm |
92 Gs
9.2 mT
|
0.00 kg / 0.00 LBS
2.1 g / 0.0 N
|
weak grip |
| 15 mm |
33 Gs
3.3 mT
|
0.00 kg / 0.00 LBS
0.3 g / 0.0 N
|
weak grip |
| 20 mm |
15 Gs
1.5 mT
|
0.00 kg / 0.00 LBS
0.1 g / 0.0 N
|
weak grip |
| 30 mm |
5 Gs
0.5 mT
|
0.00 kg / 0.00 LBS
0.0 g / 0.0 N
|
weak grip |
| 50 mm |
1 Gs
0.1 mT
|
0.00 kg / 0.00 LBS
0.0 g / 0.0 N
|
weak grip |
Table 2: Vertical capacity (vertical surface)
MW 9.5x1 / N38
| Distance (mm) | Friction coefficient | Pull Force (kg/lbs/g/N) |
|---|---|---|
| 0 mm | Stal (~0.2) |
0.08 kg / 0.18 LBS
80.0 g / 0.8 N
|
| 1 mm | Stal (~0.2) |
0.06 kg / 0.14 LBS
62.0 g / 0.6 N
|
| 2 mm | Stal (~0.2) |
0.04 kg / 0.09 LBS
40.0 g / 0.4 N
|
| 3 mm | Stal (~0.2) |
0.02 kg / 0.05 LBS
22.0 g / 0.2 N
|
| 5 mm | Stal (~0.2) |
0.01 kg / 0.01 LBS
6.0 g / 0.1 N
|
| 10 mm | Stal (~0.2) |
0.00 kg / 0.00 LBS
0.0 g / 0.0 N
|
| 15 mm | Stal (~0.2) |
0.00 kg / 0.00 LBS
0.0 g / 0.0 N
|
| 20 mm | Stal (~0.2) |
0.00 kg / 0.00 LBS
0.0 g / 0.0 N
|
| 30 mm | Stal (~0.2) |
0.00 kg / 0.00 LBS
0.0 g / 0.0 N
|
| 50 mm | Stal (~0.2) |
0.00 kg / 0.00 LBS
0.0 g / 0.0 N
|
Table 3: Vertical assembly (sliding) - behavior on slippery surfaces
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 LBS
120.0 g / 1.2 N
|
| Painted steel (standard) |
µ = 0.2
20% Nominalnej Siły
|
0.08 kg / 0.18 LBS
80.0 g / 0.8 N
|
| Oily/slippery steel |
µ = 0.1
10% Nominalnej Siły
|
0.04 kg / 0.09 LBS
40.0 g / 0.4 N
|
| Magnet with anti-slip rubber |
µ = 0.5
50% Nominalnej Siły
|
0.20 kg / 0.44 LBS
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 LBS
40.0 g / 0.4 N
|
| 1 mm |
|
0.10 kg / 0.22 LBS
100.0 g / 1.0 N
|
| 2 mm |
|
0.20 kg / 0.44 LBS
200.0 g / 2.0 N
|
| 3 mm |
|
0.30 kg / 0.66 LBS
300.0 g / 2.9 N
|
| 5 mm |
|
0.40 kg / 0.88 LBS
400.0 g / 3.9 N
|
| 10 mm |
|
0.40 kg / 0.88 LBS
400.0 g / 3.9 N
|
| 11 mm |
|
0.40 kg / 0.88 LBS
400.0 g / 3.9 N
|
| 12 mm |
|
0.40 kg / 0.88 LBS
400.0 g / 3.9 N
|
Table 5: Thermal resistance (material behavior) - thermal limit
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 LBS
400.0 g / 3.9 N
|
OK |
| 40 °C | -2.2% |
0.39 kg / 0.86 LBS
391.2 g / 3.8 N
|
OK |
| 60 °C | -4.4% |
0.38 kg / 0.84 LBS
382.4 g / 3.8 N
|
|
| 80 °C | -6.6% |
0.37 kg / 0.82 LBS
373.6 g / 3.7 N
|
|
| 100 °C | -28.8% |
0.28 kg / 0.63 LBS
284.8 g / 2.8 N
|
Table 6: Two magnets (repulsion) - forces in the system
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 LBS
2 403 Gs
|
0.11 kg / 0.24 LBS
107 g / 1.0 N
|
N/A |
| 1 mm |
0.65 kg / 1.43 LBS
2 436 Gs
|
0.10 kg / 0.21 LBS
97 g / 1.0 N
|
0.58 kg / 1.29 LBS
~0 Gs
|
| 2 mm |
0.56 kg / 1.23 LBS
2 257 Gs
|
0.08 kg / 0.18 LBS
84 g / 0.8 N
|
0.50 kg / 1.10 LBS
~0 Gs
|
| 3 mm |
0.46 kg / 1.00 LBS
2 041 Gs
|
0.07 kg / 0.15 LBS
68 g / 0.7 N
|
0.41 kg / 0.90 LBS
~0 Gs
|
| 5 mm |
0.27 kg / 0.60 LBS
1 580 Gs
|
0.04 kg / 0.09 LBS
41 g / 0.4 N
|
0.25 kg / 0.54 LBS
~0 Gs
|
| 10 mm |
0.06 kg / 0.13 LBS
732 Gs
|
0.01 kg / 0.02 LBS
9 g / 0.1 N
|
0.05 kg / 0.12 LBS
~0 Gs
|
| 20 mm |
0.00 kg / 0.01 LBS
183 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
16 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
10 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
6 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
4 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
3 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
2 Gs
|
0.00 kg / 0.00 LBS
0 g / 0.0 N
|
0.00 kg / 0.00 LBS
~0 Gs
|
Table 7: Hazards (implants) - 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 |
| Mechanical watch | 20 Gs (2.0 mT) | 2.0 cm |
| Phone / Smartphone | 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: Dynamics (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: Coating parameters (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
*Warning: On a vertical wall, the magnet retains merely approx. 20-30% of its max power.
2. Efficiency vs thickness
*Thin steel (e.g. computer case) significantly limits the holding force.
3. Thermal stability
*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) = 0.16
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% |
Sustainability
| recyclability (EoL) | 100% |
| recycled raw materials | ~10% (pre-cons) |
| carbon footprint | low / zredukowany |
| waste code (EWC) | 16 02 16 |
See more offers
Pros as well as cons of Nd2Fe14B magnets.
Advantages
- They have stable power, and over around ten years their performance decreases symbolically – ~1% (according to theory),
- Neodymium magnets are distinguished by remarkably resistant to demagnetization caused by external magnetic fields,
- In other words, due to the smooth surface of silver, the element gains visual value,
- Magnetic induction on the working part of the magnet turns out to be extremely intense,
- Made from properly selected components, these magnets show impressive resistance to high heat, enabling them to function (depending on their form) at temperatures up to 230°C and above...
- Thanks to modularity in constructing and the ability to modify to individual projects,
- Significant place in innovative solutions – they are commonly used in HDD drives, drive modules, advanced medical instruments, as well as technologically advanced constructions.
- Compactness – despite small sizes they offer powerful magnetic field, making them ideal for precision applications
Disadvantages
- At very strong impacts they can break, therefore we advise placing them in special holders. A metal housing provides additional protection against damage and increases the magnet's durability.
- Neodymium magnets lose force when exposed to high temperatures. After reaching 80°C, many of them experience permanent weakening 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
- Due to the susceptibility of magnets to corrosion in a humid environment, we recommend using waterproof magnets made of rubber, plastic or other material resistant to moisture, in case of application outdoors
- Limited possibility of producing threads in the magnet and complex shapes - recommended is cover - 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 components 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,
Lifting parameters
Maximum holding power of the magnet – what contributes to it?
- with the application of a yoke made of special test steel, ensuring maximum field concentration
- whose transverse dimension reaches at least 10 mm
- with a plane perfectly flat
- under conditions of ideal adhesion (metal-to-metal)
- for force applied at a right angle (pull-off, not shear)
- at temperature approx. 20 degrees Celsius
Key elements affecting lifting force
- Clearance – the presence of any layer (rust, dirt, air) acts as an insulator, which reduces capacity steeply (even by 50% at 0.5 mm).
- Angle of force application – maximum parameter is obtained only during pulling at a 90° angle. The force required to slide of the magnet along the surface is typically many times smaller (approx. 1/5 of the lifting capacity).
- Element thickness – to utilize 100% power, the steel must be adequately massive. Paper-thin metal limits the lifting capacity (the magnet "punches through" it).
- Material composition – different alloys attracts identically. High carbon content weaken the attraction effect.
- Base smoothness – the smoother and more polished the plate, the larger the contact zone and higher the lifting capacity. Unevenness acts like micro-gaps.
- Thermal environment – heating the magnet results in weakening of induction. It is worth remembering the thermal limit for a given model.
Lifting capacity testing was carried out on a smooth plate of optimal thickness, under a perpendicular pulling force, however under parallel forces the lifting capacity is smaller. Moreover, even a small distance between the magnet and the plate decreases the holding force.
Precautions when working with neodymium magnets
Nickel allergy
A percentage of the population have a sensitization to nickel, which is the common plating for NdFeB magnets. Extended handling might lead to skin redness. We suggest wear safety gloves.
Warning for heart patients
Health Alert: Strong magnets can deactivate heart devices and defibrillators. Do not approach if you have medical devices.
Combustion hazard
Dust generated during machining of magnets is flammable. Do not drill into magnets without proper cooling and knowledge.
Cards and drives
Powerful magnetic fields can erase data on payment cards, hard drives, and storage devices. Keep a distance of at least 10 cm.
Impact on smartphones
GPS units and smartphones are extremely sensitive to magnetism. Direct contact with a strong magnet can ruin the internal compass in your phone.
Material brittleness
Beware of splinters. Magnets can explode upon uncontrolled impact, launching sharp fragments into the air. We recommend safety glasses.
Adults only
Neodymium magnets are not toys. Swallowing a few magnets can lead to them attracting across intestines, which poses a critical condition and necessitates immediate surgery.
Crushing risk
Pinching hazard: The attraction force is so great that it can result in hematomas, pinching, and broken bones. Use thick gloves.
Caution required
Before starting, read the rules. Uncontrolled attraction can destroy the magnet or hurt your hand. Be predictive.
Do not overheat magnets
Standard neodymium magnets (N-type) lose power when the temperature surpasses 80°C. Damage is permanent.
