MPL 15x15x5 / N38 - lamellar magnet
lamellar magnet
Catalog no 020120
GTIN/EAN: 5906301811268
- length
- 15 mm [±0,1 mm]
- Width
- 15 mm [±0,1 mm]
- Height
- 5 mm [±0,1 mm]
- Weight
- 8.44 g
- Magnetization Direction
- ↑ axial
- Coating
- [NiCuNi] Nickel
How we measure these parameters — certificates and measurements
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Need more?Frequently asked questions
What pull rating should I choose for a workshop block magnet?
Are block neodymium magnets available in more durable versions?
How should I choose block magnets for mounting a structure?
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 details - MPL 15x15x5 / N38 - lamellar magnet
Specification / characteristics - MPL 15x15x5 / N38 - lamellar magnet
| properties | values |
|---|---|
| Cat. no. | 020120 |
| GTIN/EAN | 5906301811268 |
| Production/Distribution | Dhit sp. z o.o. |
| Country of origin | Poland / China / Germany |
| Customs code | 85059029 |
| length | 15 mm [±0,1 mm] |
| Width | 15 mm [±0,1 mm] |
| Height | 5 mm [±0,1 mm] |
| Weight | 8.44 g |
| Magnetization Direction | ↑ axial |
| Load capacity ~ ? | 5.87 kg / 57.62 N |
| Magnetic Induction ~ ? | 318.00 mT / 3180 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 |
Physical simulation of the assembly - technical parameters
These values are the direct effect of a engineering analysis. Results rely on algorithms for the class Nd2Fe14B. Actual parameters may differ. Treat these calculations as a supplementary guide for designers.
Table 1: Static pull force (force vs gap) - characteristics
MPL 15x15x5 / N38
| Distance (mm) | Induction (Gauss) / mT | Pull Force (kg/lbs/g/N) | Risk Status |
|---|---|---|---|
| 0 mm |
3179 Gs
317.9 mT
|
5.87 kg / 12.94 lbs
5870.0 g / 57.6 N
|
strong |
| 1 mm |
2873 Gs
287.3 mT
|
4.79 kg / 10.57 lbs
4794.1 g / 47.0 N
|
strong |
| 2 mm |
2528 Gs
252.8 mT
|
3.71 kg / 8.18 lbs
3712.5 g / 36.4 N
|
strong |
| 3 mm |
2181 Gs
218.1 mT
|
2.76 kg / 6.09 lbs
2763.0 g / 27.1 N
|
strong |
| 5 mm |
1565 Gs
156.5 mT
|
1.42 kg / 3.14 lbs
1422.0 g / 13.9 N
|
weak grip |
| 10 mm |
659 Gs
65.9 mT
|
0.25 kg / 0.56 lbs
252.1 g / 2.5 N
|
weak grip |
| 15 mm |
307 Gs
30.7 mT
|
0.05 kg / 0.12 lbs
54.7 g / 0.5 N
|
weak grip |
| 20 mm |
162 Gs
16.2 mT
|
0.02 kg / 0.03 lbs
15.2 g / 0.1 N
|
weak grip |
| 30 mm |
59 Gs
5.9 mT
|
0.00 kg / 0.00 lbs
2.0 g / 0.0 N
|
weak grip |
| 50 mm |
15 Gs
1.5 mT
|
0.00 kg / 0.00 lbs
0.1 g / 0.0 N
|
weak grip |
Table 2: Slippage force (wall)
MPL 15x15x5 / N38
| Distance (mm) | Friction coefficient | Pull Force (kg/lbs/g/N) |
|---|---|---|
| 0 mm | Raw steel (µ ≈ 0.2) |
1.17 kg / 2.59 lbs
1174.0 g / 11.5 N
|
| 1 mm | Raw steel (µ ≈ 0.2) |
0.96 kg / 2.11 lbs
958.0 g / 9.4 N
|
| 2 mm | Raw steel (µ ≈ 0.2) |
0.74 kg / 1.64 lbs
742.0 g / 7.3 N
|
| 3 mm | Raw steel (µ ≈ 0.2) |
0.55 kg / 1.22 lbs
552.0 g / 5.4 N
|
| 5 mm | Raw steel (µ ≈ 0.2) |
0.28 kg / 0.63 lbs
284.0 g / 2.8 N
|
| 10 mm | Raw steel (µ ≈ 0.2) |
0.05 kg / 0.11 lbs
50.0 g / 0.5 N
|
| 15 mm | Raw steel (µ ≈ 0.2) |
0.01 kg / 0.02 lbs
10.0 g / 0.1 N
|
| 20 mm | Raw steel (µ ≈ 0.2) |
0.00 kg / 0.01 lbs
4.0 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: Wall mounting (shearing) - behavior on slippery surfaces
MPL 15x15x5 / N38
| Surface type | Friction coefficient / % | Max load (kg/lbs/g/N) |
|---|---|---|
| Raw steel |
µ = 0.3
30% of nominal force
|
1.76 kg / 3.88 lbs
1761.0 g / 17.3 N
|
| Painted steel (standard) |
µ = 0.2
20% of nominal force
|
1.17 kg / 2.59 lbs
1174.0 g / 11.5 N
|
| Oily/slippery steel |
µ = 0.1
10% of nominal force
|
0.59 kg / 1.29 lbs
587.0 g / 5.8 N
|
| Magnet with anti-slip rubber |
µ = 0.5
50% of nominal force
|
2.94 kg / 6.47 lbs
2935.0 g / 28.8 N
|
Table 4: Steel thickness (substrate influence) - power losses
MPL 15x15x5 / N38
| Steel thickness (mm) | % power | Real pull force (kg/lbs/g/N) |
|---|---|---|
| 0.5 mm |
|
0.59 kg / 1.29 lbs
587.0 g / 5.8 N
|
| 1 mm |
|
1.47 kg / 3.24 lbs
1467.5 g / 14.4 N
|
| 2 mm |
|
2.94 kg / 6.47 lbs
2935.0 g / 28.8 N
|
| 3 mm |
|
4.40 kg / 9.71 lbs
4402.5 g / 43.2 N
|
| 5 mm |
|
5.87 kg / 12.94 lbs
5870.0 g / 57.6 N
|
| 10 mm |
|
5.87 kg / 12.94 lbs
5870.0 g / 57.6 N
|
| 11 mm |
|
5.87 kg / 12.94 lbs
5870.0 g / 57.6 N
|
| 12 mm |
|
5.87 kg / 12.94 lbs
5870.0 g / 57.6 N
|
Table 5: Working in heat (stability) - resistance threshold
MPL 15x15x5 / N38
| Magnet temperature (°C) | Force change relative to 20°C | Remaining pull (kg/lbs/g/N) | Status |
|---|---|---|---|
| 20 °C | 0.0% |
5.87 kg / 12.94 lbs
5870.0 g / 57.6 N
|
Estimate |
| 40 °C | -4.4% |
5.61 kg / 12.38 lbs
5614.6 g / 55.1 N
|
Estimate |
| 60 °C | -8.6% |
5.36 kg / 11.83 lbs
5364.8 g / 52.6 N
|
Estimate |
| 80 °C | -12.8% |
5.12 kg / 11.29 lbs
5120.7 g / 50.2 N
|
Material limit |
| 100 °C | — | — | Out of range — no model |
Table 6: Magnet-Magnet interaction (attraction) - forces in the system
MPL 15x15x5 / N38
| Gap (mm) | Attraction (kg/lbs) (N-S) | Sliding Force (kg/lbs/g/N) | Repulsion (kg/lbs) (N-N) |
|---|---|---|---|
| 0 mm |
14.02 kg / 30.90 lbs
4 741 Gs
|
2.10 kg / 4.64 lbs
2103 g / 20.6 N
|
N/A |
| 1 mm |
12.77 kg / 28.15 lbs
6 068 Gs
|
1.92 kg / 4.22 lbs
1916 g / 18.8 N
|
11.49 kg / 25.34 lbs
~0 Gs
|
| 2 mm |
11.45 kg / 25.24 lbs
5 746 Gs
|
1.72 kg / 3.79 lbs
1717 g / 16.8 N
|
10.30 kg / 22.72 lbs
~0 Gs
|
| 3 mm |
10.13 kg / 22.34 lbs
5 405 Gs
|
1.52 kg / 3.35 lbs
1520 g / 14.9 N
|
9.12 kg / 20.10 lbs
~0 Gs
|
| 5 mm |
7.68 kg / 16.93 lbs
4 706 Gs
|
1.15 kg / 2.54 lbs
1152 g / 11.3 N
|
6.91 kg / 15.24 lbs
~0 Gs
|
| 10 mm |
3.40 kg / 7.49 lbs
3 129 Gs
|
0.51 kg / 1.12 lbs
509 g / 5.0 N
|
3.06 kg / 6.74 lbs
~0 Gs
|
| 20 mm |
0.60 kg / 1.33 lbs
1 318 Gs
|
0.09 kg / 0.20 lbs
90 g / 0.9 N
|
0.54 kg / 1.19 lbs
~0 Gs
|
| 50 mm |
0.01 kg / 0.03 lbs
188 Gs
|
0.00 kg / 0.00 lbs
2 g / 0.0 N
|
0.01 kg / 0.02 lbs
~0 Gs
|
| 60 mm |
0.00 kg / 0.01 lbs
118 Gs
|
0.00 kg / 0.00 lbs
1 g / 0.0 N
|
0.00 kg / 0.00 lbs
~0 Gs
|
| 70 mm |
0.00 kg / 0.00 lbs
79 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
55 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
40 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
30 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
MPL 15x15x5 / N38
| Field level (Gs) | mT | Model distance (cm) |
|---|---|---|
| < 5 Gs | < 0.5 mT | 7.5 cm |
| < 10 Gs | < 1.0 mT | 6.0 cm |
| < 20 Gs | < 2.0 mT | 4.5 cm |
| < 40 Gs | < 4.0 mT | 3.5 cm |
| < 50 Gs | < 5.0 mT | 3.5 cm |
| < 400 Gs | < 40.0 mT | 1.5 cm |
| < 600 Gs | < 60.0 mT | 1.5 cm |
Table 8: Impact energy (kinetic energy) - collision effects
MPL 15x15x5 / N38
| Start from (mm) | Speed (km/h) | Energy (J) | Predicted outcome |
|---|---|---|---|
| 10 mm |
24.70 km/h
(6.86 m/s)
|
0.20 J | |
| 30 mm |
25.21 km/h
(7.00 m/s)
|
0.21 J | |
| 50 mm |
25.22 km/h
(7.00 m/s)
|
0.21 J | |
| 100 mm |
25.22 km/h
(7.01 m/s)
|
0.21 J |
Table 9: Surface protection spec
MPL 15x15x5 / 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)
MPL 15x15x5 / N38
| Parameter | Value | SI Unit / Description |
|---|---|---|
| Magnetic Flux | 7 651 Mx | 76.5 µWb |
| Pc Coefficient | 0.40 | Low (Flat) |
Table 11: Submerged application
MPL 15x15x5 / N38
| Environment | Effective steel pull | Effect |
|---|---|---|
| Air (land) | 5.87 kg | Standard |
| Water (riverbed) |
6.72 kg
(+0.85 kg buoyancy gain)
|
+14.5% |
1. Wall mount (shear)
*Warning: On a vertical surface, the magnet retains just ~20% of its perpendicular strength.
2. Plate thickness effect
*Thin metal sheet (e.g. computer case) drastically limits the holding force.
3. Thermal stability
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) = 0.40
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.
Chemical composition
| 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 Nd2Fe14B magnets.
Advantages
- Their strength remains stable, and after approximately 10 years it drops only by ~1% (according to research),
- Magnets perfectly resist against demagnetization caused by external fields,
- The use of an refined finish of noble metals (nickel, gold, silver) causes the element to have aesthetics,
- Neodymium magnets achieve maximum magnetic induction on a contact point, which ensures high operational effectiveness,
- Made from properly selected components, these magnets show impressive resistance to high heat, enabling them to function (depending on their shape) at temperatures up to 230°C and above...
- Thanks to freedom in designing and the capacity to modify to individual projects,
- Huge importance in modern industrial fields – they are utilized in computer drives, motor assemblies, medical devices, also multitasking production systems.
- Thanks to their power density, small magnets offer high operating force, occupying minimum space,
Limitations
- At very strong impacts they can break, therefore we recommend placing them in steel cases. A metal housing provides additional protection against damage, as well as increases the magnet's durability.
- Do not exceed this material temperature limit: 80°C. Overheating may permanently weaken the magnet.
- Due to the susceptibility of magnets to corrosion in a humid environment, we suggest using waterproof magnets made of rubber, plastic or other material immune to moisture, when using outdoors
- Limited possibility of producing nuts in the magnet and complex forms - recommended is a housing - mounting mechanism.
- Health risk related to microscopic parts of magnets are risky, if swallowed, which is particularly important in the aspect of protecting the youngest. Furthermore, small components of these devices are able to be problematic in diagnostics 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
Detachment force of the magnet in optimal conditions – what it depends on?
- on a base made of mild steel, perfectly concentrating the magnetic flux
- with a thickness minimum 10 mm
- with a plane perfectly flat
- with total lack of distance (no impurities)
- under vertical force direction (90-degree angle)
- at conditions approx. 20°C
Determinants of lifting force in real conditions
- Air gap (betwixt the magnet and the plate), since even a tiny distance (e.g. 0.5 mm) results in a reduction in lifting capacity by up to 50% (this also applies to varnish, rust or dirt).
- Pull-off angle – note that the magnet holds strongest perpendicularly. Under shear forces, the holding force drops drastically, often to levels of 20-30% of the maximum value.
- Element thickness – to utilize 100% power, the steel must be adequately massive. Thin sheet restricts the attraction force (the magnet "punches through" it).
- Material composition – not every steel attracts identically. High carbon content weaken the interaction with the magnet.
- Plate texture – smooth surfaces guarantee perfect abutment, which improves field saturation. Rough surfaces reduce efficiency.
- Thermal environment – heating the magnet causes a temporary drop of force. It is worth remembering the maximum operating temperature for a given model.
Lifting capacity testing was carried out on plates with a smooth surface of optimal thickness, under perpendicular forces, however under shearing force the holding force is lower. Additionally, even a minimal clearance between the magnet’s surface and the plate decreases the lifting capacity.
Safety rules for work with neodymium magnets
Magnet fragility
Despite metallic appearance, neodymium is delicate and cannot withstand shocks. Do not hit, as the magnet may shatter into sharp, dangerous pieces.
Adults only
Absolutely store magnets out of reach of children. Ingestion danger is significant, and the effects of magnets clamping inside the body are fatal.
Electronic devices
Very strong magnetic fields can corrupt files on payment cards, HDDs, and other magnetic media. Stay away of at least 10 cm.
Nickel coating and allergies
A percentage of the population suffer from a contact allergy to Ni, which is the common plating for neodymium magnets. Frequent touching might lead to a rash. We recommend wear safety gloves.
Phone sensors
Navigation devices and mobile phones are highly sensitive to magnetism. Direct contact with a powerful NdFeB magnet can decalibrate the sensors in your phone.
Pinching danger
Danger of trauma: The pulling power is so great that it can result in blood blisters, crushing, and broken bones. Protective gloves are recommended.
Danger to pacemakers
Warning for patients: Powerful magnets disrupt medical devices. Maintain minimum 30 cm distance or ask another person to handle the magnets.
Caution required
Before starting, read the rules. Sudden snapping can break the magnet or injure your hand. Think ahead.
Flammability
Fire hazard: Neodymium dust is explosive. Do not process magnets without safety gear as this risks ignition.
Do not overheat magnets
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.
