MPL 40x20x6 / N38 - lamellar magnet
lamellar magnet
Catalog no 020589
GTIN/EAN: 5906301815822
- length
- 40 mm [±0,1 mm]
- Width
- 20 mm [±0,1 mm]
- Height
- 6 mm [±0,1 mm]
- Weight
- 36 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 parameters of the product - MPL 40x20x6 / N38 - lamellar magnet
Specification / characteristics - MPL 40x20x6 / N38 - lamellar magnet
| properties | values |
|---|---|
| Cat. no. | 020589 |
| GTIN/EAN | 5906301815822 |
| Distributor | Dhit sp. z o.o. |
| Country of origin | Poland / China / Germany |
| Customs code | 85059029 |
| length | 40 mm [±0,1 mm] |
| Width | 20 mm [±0,1 mm] |
| Height | 6 mm [±0,1 mm] |
| Weight | 36 g |
| Magnetization Direction | ↑ axial |
| Load capacity ~ ? | 13.76 kg / 134.94 N |
| Magnetic Induction ~ ? | 239.54 mT / 2395 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 analysis of the magnet - data
These data represent the result of a engineering simulation. Results were calculated on algorithms for the material Nd2Fe14B. Operational performance may differ from theoretical values. Please consider these calculations as a reference point during assembly planning.
Table 1: Static force (pull vs gap) - power drop
MPL 40x20x6 / N38
| Distance (mm) | Induction (Gauss) / mT | Pull Force (kg/lbs/g/N) | Risk Status |
|---|---|---|---|
| 0 mm |
2395 Gs
239.5 mT
|
13.76 kg / 30.34 LBS
13760.0 g / 135.0 N
|
dangerous! |
| 1 mm |
2271 Gs
227.1 mT
|
12.37 kg / 27.28 LBS
12374.3 g / 121.4 N
|
dangerous! |
| 2 mm |
2127 Gs
212.7 mT
|
10.85 kg / 23.93 LBS
10853.7 g / 106.5 N
|
dangerous! |
| 3 mm |
1972 Gs
197.2 mT
|
9.33 kg / 20.57 LBS
9331.3 g / 91.5 N
|
strong |
| 5 mm |
1659 Gs
165.9 mT
|
6.60 kg / 14.55 LBS
6601.4 g / 64.8 N
|
strong |
| 10 mm |
1018 Gs
101.8 mT
|
2.49 kg / 5.49 LBS
2488.3 g / 24.4 N
|
strong |
| 15 mm |
627 Gs
62.7 mT
|
0.94 kg / 2.08 LBS
942.0 g / 9.2 N
|
low risk |
| 20 mm |
399 Gs
39.9 mT
|
0.38 kg / 0.84 LBS
381.9 g / 3.7 N
|
low risk |
| 30 mm |
181 Gs
18.1 mT
|
0.08 kg / 0.17 LBS
79.0 g / 0.8 N
|
low risk |
| 50 mm |
54 Gs
5.4 mT
|
0.01 kg / 0.02 LBS
7.1 g / 0.1 N
|
low risk |
Table 2: Vertical capacity (vertical surface)
MPL 40x20x6 / N38
| Distance (mm) | Friction coefficient | Pull Force (kg/lbs/g/N) |
|---|---|---|
| 0 mm | Raw steel (µ ≈ 0.2) |
2.75 kg / 6.07 LBS
2752.0 g / 27.0 N
|
| 1 mm | Raw steel (µ ≈ 0.2) |
2.47 kg / 5.45 LBS
2474.0 g / 24.3 N
|
| 2 mm | Raw steel (µ ≈ 0.2) |
2.17 kg / 4.78 LBS
2170.0 g / 21.3 N
|
| 3 mm | Raw steel (µ ≈ 0.2) |
1.87 kg / 4.11 LBS
1866.0 g / 18.3 N
|
| 5 mm | Raw steel (µ ≈ 0.2) |
1.32 kg / 2.91 LBS
1320.0 g / 12.9 N
|
| 10 mm | Raw steel (µ ≈ 0.2) |
0.50 kg / 1.10 LBS
498.0 g / 4.9 N
|
| 15 mm | Raw steel (µ ≈ 0.2) |
0.19 kg / 0.41 LBS
188.0 g / 1.8 N
|
| 20 mm | Raw steel (µ ≈ 0.2) |
0.08 kg / 0.17 LBS
76.0 g / 0.7 N
|
| 30 mm | Raw steel (µ ≈ 0.2) |
0.02 kg / 0.04 LBS
16.0 g / 0.2 N
|
| 50 mm | Raw steel (µ ≈ 0.2) |
0.00 kg / 0.00 LBS
2.0 g / 0.0 N
|
Table 3: Vertical assembly (shearing) - behavior on slippery surfaces
MPL 40x20x6 / N38
| Surface type | Friction coefficient / % | Max load (kg/lbs/g/N) |
|---|---|---|
| Raw steel |
µ = 0.3
30% of nominal force
|
4.13 kg / 9.10 LBS
4128.0 g / 40.5 N
|
| Painted steel (standard) |
µ = 0.2
20% of nominal force
|
2.75 kg / 6.07 LBS
2752.0 g / 27.0 N
|
| Oily/slippery steel |
µ = 0.1
10% of nominal force
|
1.38 kg / 3.03 LBS
1376.0 g / 13.5 N
|
| Magnet with anti-slip rubber |
µ = 0.5
50% of nominal force
|
6.88 kg / 15.17 LBS
6880.0 g / 67.5 N
|
Table 4: Steel thickness (saturation) - sheet metal selection
MPL 40x20x6 / N38
| Steel thickness (mm) | % power | Real pull force (kg/lbs/g/N) |
|---|---|---|
| 0.5 mm |
|
0.69 kg / 1.52 LBS
688.0 g / 6.7 N
|
| 1 mm |
|
1.72 kg / 3.79 LBS
1720.0 g / 16.9 N
|
| 2 mm |
|
3.44 kg / 7.58 LBS
3440.0 g / 33.7 N
|
| 3 mm |
|
5.16 kg / 11.38 LBS
5160.0 g / 50.6 N
|
| 5 mm |
|
8.60 kg / 18.96 LBS
8600.0 g / 84.4 N
|
| 10 mm |
|
13.76 kg / 30.34 LBS
13760.0 g / 135.0 N
|
| 11 mm |
|
13.76 kg / 30.34 LBS
13760.0 g / 135.0 N
|
| 12 mm |
|
13.76 kg / 30.34 LBS
13760.0 g / 135.0 N
|
Table 5: Thermal resistance (stability) - thermal limit
MPL 40x20x6 / N38
| Magnet temperature (°C) | Force change relative to 20°C | Remaining pull (kg/lbs/g/N) | Status |
|---|---|---|---|
| 20 °C | 0.0% |
13.76 kg / 30.34 LBS
13760.0 g / 135.0 N
|
Estimate |
| 40 °C | -4.4% |
13.16 kg / 29.02 LBS
13161.2 g / 129.1 N
|
Estimate |
| 60 °C | -8.6% |
12.58 kg / 27.72 LBS
12575.8 g / 123.4 N
|
Estimate |
| 80 °C | -12.8% |
12.00 kg / 26.46 LBS
12003.6 g / 117.8 N
|
Material limit |
| 100 °C | — | — | Out of range — no model |
Table 6: Two magnets (repulsion) - field range
MPL 40x20x6 / N38
| Gap (mm) | Attraction (kg/lbs) (N-S) | Shear Force (kg/lbs/g/N) | Repulsion (kg/lbs) (N-N) |
|---|---|---|---|
| 0 mm |
28.29 kg / 62.37 LBS
3 904 Gs
|
4.24 kg / 9.36 LBS
4243 g / 41.6 N
|
N/A |
| 1 mm |
26.93 kg / 59.36 LBS
4 673 Gs
|
4.04 kg / 8.90 LBS
4039 g / 39.6 N
|
24.23 kg / 53.43 LBS
~0 Gs
|
| 2 mm |
25.44 kg / 56.09 LBS
4 542 Gs
|
3.82 kg / 8.41 LBS
3816 g / 37.4 N
|
22.90 kg / 50.48 LBS
~0 Gs
|
| 3 mm |
23.89 kg / 52.67 LBS
4 402 Gs
|
3.58 kg / 7.90 LBS
3584 g / 35.2 N
|
21.50 kg / 47.41 LBS
~0 Gs
|
| 5 mm |
20.74 kg / 45.72 LBS
4 101 Gs
|
3.11 kg / 6.86 LBS
3110 g / 30.5 N
|
18.66 kg / 41.14 LBS
~0 Gs
|
| 10 mm |
13.57 kg / 29.92 LBS
3 318 Gs
|
2.04 kg / 4.49 LBS
2036 g / 20.0 N
|
12.21 kg / 26.93 LBS
~0 Gs
|
| 20 mm |
5.12 kg / 11.28 LBS
2 037 Gs
|
0.77 kg / 1.69 LBS
767 g / 7.5 N
|
4.60 kg / 10.15 LBS
~0 Gs
|
| 50 mm |
0.34 kg / 0.76 LBS
528 Gs
|
0.05 kg / 0.11 LBS
52 g / 0.5 N
|
0.31 kg / 0.68 LBS
~0 Gs
|
| 60 mm |
0.16 kg / 0.36 LBS
363 Gs
|
0.02 kg / 0.05 LBS
24 g / 0.2 N
|
0.15 kg / 0.32 LBS
~0 Gs
|
| 70 mm |
0.08 kg / 0.18 LBS
258 Gs
|
0.01 kg / 0.03 LBS
12 g / 0.1 N
|
0.07 kg / 0.16 LBS
~0 Gs
|
| 80 mm |
0.04 kg / 0.10 LBS
188 Gs
|
0.01 kg / 0.01 LBS
7 g / 0.1 N
|
0.04 kg / 0.09 LBS
~0 Gs
|
| 90 mm |
0.02 kg / 0.05 LBS
141 Gs
|
0.00 kg / 0.01 LBS
4 g / 0.0 N
|
0.02 kg / 0.05 LBS
~0 Gs
|
| 100 mm |
0.01 kg / 0.03 LBS
108 Gs
|
0.00 kg / 0.00 LBS
2 g / 0.0 N
|
0.01 kg / 0.03 LBS
~0 Gs
|
Table 7: Axial field levels — not safety zones
MPL 40x20x6 / N38
| Field level (Gs) | mT | Model distance (cm) |
|---|---|---|
| < 5 Gs | < 0.5 mT | 12.0 cm |
| < 10 Gs | < 1.0 mT | 9.5 cm |
| < 20 Gs | < 2.0 mT | 7.5 cm |
| < 40 Gs | < 4.0 mT | 6.0 cm |
| < 50 Gs | < 5.0 mT | 5.5 cm |
| < 400 Gs | < 40.0 mT | 2.0 cm |
| < 600 Gs | < 60.0 mT | 2.0 cm |
Table 8: Impact energy (kinetic energy) - collision effects
MPL 40x20x6 / N38
| Start from (mm) | Speed (km/h) | Energy (J) | Predicted outcome |
|---|---|---|---|
| 10 mm |
22.54 km/h
(6.26 m/s)
|
0.71 J | |
| 30 mm |
24.48 km/h
(6.80 m/s)
|
0.83 J | |
| 50 mm |
24.55 km/h
(6.82 m/s)
|
0.84 J | |
| 100 mm |
24.57 km/h
(6.82 m/s)
|
0.84 J |
Table 9: Anti-corrosion coating durability
MPL 40x20x6 / 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)
MPL 40x20x6 / N38
| Parameter | Value | SI Unit / Description |
|---|---|---|
| Magnetic Flux | 20 490 Mx | 204.9 µWb |
| Pc Coefficient | 0.27 | Low (Flat) |
Table 11: Physics of underwater searching
MPL 40x20x6 / N38
| Environment | Effective steel pull | Effect |
|---|---|---|
| Air (land) | 13.76 kg | Standard |
| Water (riverbed) |
15.76 kg
(+2.00 kg buoyancy gain)
|
+14.5% |
1. Wall mount (shear)
*Note: On a vertical wall, the magnet retains merely approx. 20-30% of its nominal pull.
2. Plate thickness effect
*Thin metal sheet (e.g. computer case) drastically limits the holding force.
3. Temperature resistance
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) = 0.27
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.
Material specification
| 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 |
Other deals
Advantages and disadvantages of neodymium magnets.
Strengths
- They have stable power, and over nearly 10 years their performance decreases symbolically – ~1% (according to theory),
- They are extremely resistant to demagnetization induced by external field influence,
- The use of an shiny layer of noble metals (nickel, gold, silver) causes the element to look better,
- Magnetic induction on the working layer of the magnet remains very high,
- Due to their durability and thermal resistance, neodymium magnets are capable of operate (depending on the form) even at high temperatures reaching 230°C or more...
- Thanks to freedom in forming and the capacity to customize to complex applications,
- Significant place in modern industrial fields – they find application in magnetic memories, brushless drives, medical devices, and technologically advanced constructions.
- Relatively small size with high pulling force – neodymium magnets offer strong magnetic field in compact dimensions, which allows their use in compact constructions
Disadvantages
- 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 improves its resistance to damage
- Do not exceed this material temperature limit: 80°C. Overheating may permanently weaken the magnet.
- They oxidize in a humid environment - during use outdoors we advise using waterproof magnets e.g. in rubber, plastic
- We recommend a housing - magnetic mechanism, due to difficulties in producing threads inside the magnet and complex shapes.
- Health risk to health – tiny shards of magnets can be dangerous, in case of ingestion, which is particularly important in the aspect of protecting the youngest. Additionally, tiny parts of these magnets are able to disrupt the diagnostic process medical in case of swallowing.
- Higher cost of purchase is one of the disadvantages compared to ceramic magnets, especially in budget applications
Lifting parameters
Detachment force of the magnet in optimal conditions – what it depends on?
- with the application of a sheet made of low-carbon steel, guaranteeing maximum field concentration
- with a thickness no less than 10 mm
- with a plane free of scratches
- with direct contact (no coatings)
- during detachment in a direction perpendicular to the mounting surface
- at standard ambient temperature
Determinants of practical lifting force of a magnet
- Distance – existence of any layer (paint, tape, air) interrupts the magnetic circuit, which reduces capacity steeply (even by 50% at 0.5 mm).
- Load vector – highest force is obtained only during perpendicular pulling. The resistance to sliding of the magnet along the surface is standardly several times lower (approx. 1/5 of the lifting capacity).
- Plate thickness – too thin steel does not accept the full field, causing part of the flux to be escaped to the other side.
- Material type – the best choice is high-permeability steel. Cast iron may have worse magnetic properties.
- Surface structure – the more even the surface, the larger the contact zone and higher the lifting capacity. Roughness acts like micro-gaps.
- Thermal conditions – neodymium magnets have a negative temperature coefficient. When it is hot they lose power, and in frost they can be stronger (up to a certain limit).
Lifting capacity was assessed with the use of a steel plate with a smooth surface of suitable thickness (min. 20 mm), under perpendicular pulling force, whereas under parallel forces the lifting capacity is smaller. In addition, even a small distance between the magnet and the plate decreases the lifting capacity.
Precautions when working with NdFeB magnets
GPS and phone interference
Note: rare earth magnets generate a field that confuses precision electronics. Maintain a safe distance from your phone, tablet, and GPS.
Product not for children
Only for adults. Tiny parts pose a choking risk, leading to severe trauma. Store away from kids and pets.
Sensitization to coating
A percentage of the population have a hypersensitivity to Ni, which is the standard coating for neodymium magnets. Extended handling might lead to a rash. We recommend wear safety gloves.
Machining danger
Dust produced during cutting of magnets is combustible. Avoid drilling into magnets without proper cooling and knowledge.
Demagnetization risk
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.
Magnets are brittle
Watch out for shards. Magnets can fracture upon violent connection, launching shards into the air. Wear goggles.
Handling guide
Before starting, check safety instructions. Uncontrolled attraction can destroy the magnet or injure your hand. Think ahead.
Hand protection
Big blocks can crush fingers instantly. Under no circumstances place your hand betwixt two attracting surfaces.
Health Danger
For implant holders: Strong magnetic fields disrupt medical devices. Keep at least 30 cm distance or request help to work with the magnets.
Keep away from computers
Powerful magnetic fields can erase data on payment cards, hard drives, and other magnetic media. Maintain a gap of at least 10 cm.
