MPL 30x3x2 / N38 - lamellar magnet
lamellar magnet
Catalog no 020585
GTIN/EAN: 5906301815785
- length
- 30 mm [±0,1 mm]
- Width
- 3 mm [±0,1 mm]
- Height
- 2 mm [±0,1 mm]
- Weight
- 1.35 g
- Magnetization Direction
- ↑ axial
- Coating
- [NiCuNi] Nickel
How we measure these parameters — certificates and measurements
0.780 zł net / pcs
0.959 zł with VAT (23% VAT) / pcs
bulk discounts:
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 - MPL 30x3x2 / N38 - lamellar magnet
Specification / characteristics - MPL 30x3x2 / N38 - lamellar magnet
| properties | values |
|---|---|
| Cat. no. | 020585 |
| GTIN/EAN | 5906301815785 |
| Distributor | Dhit sp. z o.o. |
| Country of origin | Poland / China / Germany |
| Customs code | 85059029 |
| length | 30 mm [±0,1 mm] |
| Width | 3 mm [±0,1 mm] |
| Height | 2 mm [±0,1 mm] |
| Weight | 1.35 g |
| Magnetization Direction | ↑ axial |
| Load capacity ~ ? | 3.14 kg / 30.79 N |
| Magnetic Induction ~ ? | 367.55 mT / 3676 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 |
Engineering analysis of the assembly - report
The following information constitute the result of a physical calculation. Values are based on models for the material Nd2Fe14B. Real-world conditions might slightly differ from theoretical values. Use these data as a supplementary guide when designing systems.
Table 1: Static force (force vs gap) - characteristics
MPL 30x3x2 / N38
| Distance (mm) | Induction (Gauss) / mT | Pull Force (kg/lbs/g/N) | Risk Status |
|---|---|---|---|
| 0 mm |
3669 Gs
366.9 mT
|
3.14 kg / 6.92 lbs
3140.0 g / 30.8 N
|
warning |
| 1 mm |
2074 Gs
207.4 mT
|
1.00 kg / 2.21 lbs
1003.5 g / 9.8 N
|
low risk |
| 2 mm |
1148 Gs
114.8 mT
|
0.31 kg / 0.68 lbs
307.3 g / 3.0 N
|
low risk |
| 3 mm |
702 Gs
70.2 mT
|
0.11 kg / 0.25 lbs
115.0 g / 1.1 N
|
low risk |
| 5 mm |
336 Gs
33.6 mT
|
0.03 kg / 0.06 lbs
26.3 g / 0.3 N
|
low risk |
| 10 mm |
106 Gs
10.6 mT
|
0.00 kg / 0.01 lbs
2.6 g / 0.0 N
|
low risk |
| 15 mm |
48 Gs
4.8 mT
|
0.00 kg / 0.00 lbs
0.5 g / 0.0 N
|
low risk |
| 20 mm |
26 Gs
2.6 mT
|
0.00 kg / 0.00 lbs
0.2 g / 0.0 N
|
low risk |
| 30 mm |
10 Gs
1.0 mT
|
0.00 kg / 0.00 lbs
0.0 g / 0.0 N
|
low risk |
| 50 mm |
2 Gs
0.2 mT
|
0.00 kg / 0.00 lbs
0.0 g / 0.0 N
|
low risk |
Table 2: Sliding load (wall)
MPL 30x3x2 / N38
| Distance (mm) | Friction coefficient | Pull Force (kg/lbs/g/N) |
|---|---|---|
| 0 mm | Raw steel (µ ≈ 0.2) |
0.63 kg / 1.38 lbs
628.0 g / 6.2 N
|
| 1 mm | Raw steel (µ ≈ 0.2) |
0.20 kg / 0.44 lbs
200.0 g / 2.0 N
|
| 2 mm | Raw steel (µ ≈ 0.2) |
0.06 kg / 0.14 lbs
62.0 g / 0.6 N
|
| 3 mm | Raw steel (µ ≈ 0.2) |
0.02 kg / 0.05 lbs
22.0 g / 0.2 N
|
| 5 mm | Raw steel (µ ≈ 0.2) |
0.01 kg / 0.01 lbs
6.0 g / 0.1 N
|
| 10 mm | Raw steel (µ ≈ 0.2) |
0.00 kg / 0.00 lbs
0.0 g / 0.0 N
|
| 15 mm | Raw steel (µ ≈ 0.2) |
0.00 kg / 0.00 lbs
0.0 g / 0.0 N
|
| 20 mm | Raw steel (µ ≈ 0.2) |
0.00 kg / 0.00 lbs
0.0 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: Vertical assembly (sliding) - behavior on slippery surfaces
MPL 30x3x2 / N38
| Surface type | Friction coefficient / % | Max load (kg/lbs/g/N) |
|---|---|---|
| Raw steel |
µ = 0.3
30% of nominal force
|
0.94 kg / 2.08 lbs
942.0 g / 9.2 N
|
| Painted steel (standard) |
µ = 0.2
20% of nominal force
|
0.63 kg / 1.38 lbs
628.0 g / 6.2 N
|
| Oily/slippery steel |
µ = 0.1
10% of nominal force
|
0.31 kg / 0.69 lbs
314.0 g / 3.1 N
|
| Magnet with anti-slip rubber |
µ = 0.5
50% of nominal force
|
1.57 kg / 3.46 lbs
1570.0 g / 15.4 N
|
Table 4: Material efficiency (saturation) - sheet metal selection
MPL 30x3x2 / N38
| Steel thickness (mm) | % power | Real pull force (kg/lbs/g/N) |
|---|---|---|
| 0.5 mm |
|
0.31 kg / 0.69 lbs
314.0 g / 3.1 N
|
| 1 mm |
|
0.79 kg / 1.73 lbs
785.0 g / 7.7 N
|
| 2 mm |
|
1.57 kg / 3.46 lbs
1570.0 g / 15.4 N
|
| 3 mm |
|
2.36 kg / 5.19 lbs
2355.0 g / 23.1 N
|
| 5 mm |
|
3.14 kg / 6.92 lbs
3140.0 g / 30.8 N
|
| 10 mm |
|
3.14 kg / 6.92 lbs
3140.0 g / 30.8 N
|
| 11 mm |
|
3.14 kg / 6.92 lbs
3140.0 g / 30.8 N
|
| 12 mm |
|
3.14 kg / 6.92 lbs
3140.0 g / 30.8 N
|
Table 5: Working in heat (stability) - power drop
MPL 30x3x2 / N38
| Magnet temperature (°C) | Force change relative to 20°C | Remaining pull (kg/lbs/g/N) | Status |
|---|---|---|---|
| 20 °C | 0.0% |
3.14 kg / 6.92 lbs
3140.0 g / 30.8 N
|
Estimate |
| 40 °C | -4.4% |
3.00 kg / 6.62 lbs
3003.4 g / 29.5 N
|
Estimate |
| 60 °C | -8.6% |
2.87 kg / 6.33 lbs
2869.8 g / 28.2 N
|
Estimate |
| 80 °C | -12.8% |
2.74 kg / 6.04 lbs
2739.2 g / 26.9 N
|
Material limit |
| 100 °C | — | — | Out of range — no model |
Table 6: Two magnets (attraction) - field collision
MPL 30x3x2 / N38
| Gap (mm) | Attraction (kg/lbs) (N-S) | Sliding Force (kg/lbs/g/N) | Repulsion (kg/lbs) (N-N) |
|---|---|---|---|
| 0 mm |
7.47 kg / 16.47 lbs
4 811 Gs
|
1.12 kg / 2.47 lbs
1120 g / 11.0 N
|
N/A |
| 1 mm |
4.42 kg / 9.75 lbs
5 645 Gs
|
0.66 kg / 1.46 lbs
663 g / 6.5 N
|
3.98 kg / 8.77 lbs
~0 Gs
|
| 2 mm |
2.39 kg / 5.26 lbs
4 148 Gs
|
0.36 kg / 0.79 lbs
358 g / 3.5 N
|
2.15 kg / 4.74 lbs
~0 Gs
|
| 3 mm |
1.29 kg / 2.85 lbs
3 053 Gs
|
0.19 kg / 0.43 lbs
194 g / 1.9 N
|
1.16 kg / 2.57 lbs
~0 Gs
|
| 5 mm |
0.44 kg / 0.96 lbs
1 773 Gs
|
0.07 kg / 0.14 lbs
65 g / 0.6 N
|
0.39 kg / 0.86 lbs
~0 Gs
|
| 10 mm |
0.06 kg / 0.14 lbs
672 Gs
|
0.01 kg / 0.02 lbs
9 g / 0.1 N
|
0.06 kg / 0.12 lbs
~0 Gs
|
| 20 mm |
0.01 kg / 0.01 lbs
211 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
31 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
19 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
13 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
9 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
7 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
5 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 30x3x2 / N38
| Field level (Gs) | mT | Model distance (cm) |
|---|---|---|
| < 5 Gs | < 0.5 mT | 4.0 cm |
| < 10 Gs | < 1.0 mT | 3.0 cm |
| < 20 Gs | < 2.0 mT | 2.5 cm |
| < 40 Gs | < 4.0 mT | 2.0 cm |
| < 50 Gs | < 5.0 mT | 1.5 cm |
| < 400 Gs | < 40.0 mT | 0.5 cm |
| < 600 Gs | < 60.0 mT | 0.5 cm |
Table 8: Impact energy (cracking risk) - warning
MPL 30x3x2 / N38
| Start from (mm) | Speed (km/h) | Energy (J) | Predicted outcome |
|---|---|---|---|
| 10 mm |
23.29 km/h
(6.47 m/s)
|
0.03 J | |
| 30 mm |
23.32 km/h
(6.48 m/s)
|
0.03 J | |
| 50 mm |
23.31 km/h
(6.47 m/s)
|
0.03 J | |
| 100 mm |
23.32 km/h
(6.48 m/s)
|
0.03 J |
Table 9: Anti-corrosion coating durability
MPL 30x3x2 / 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)
MPL 30x3x2 / N38
| Parameter | Value | SI Unit / Description |
|---|---|---|
| Magnetic Flux | 2 295 Mx | 23.0 µWb |
| Pc Coefficient | 0.27 | Low (Flat) |
Table 11: Physics of underwater searching
MPL 30x3x2 / N38
| Environment | Effective steel pull | Effect |
|---|---|---|
| Air (land) | 3.14 kg | Standard |
| Water (riverbed) |
3.60 kg
(+0.46 kg buoyancy gain)
|
+14.5% |
1. Sliding resistance
*Note: On a vertical wall, the magnet retains just a fraction of its nominal pull.
2. Efficiency vs thickness
*Thin steel (e.g. 0.5mm PC case) severely limits the holding force.
3. Heat tolerance
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
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% |
Environmental data
| recyclability (EoL) | 100% |
| recycled raw materials | ~10% (pre-cons) |
| carbon footprint | low / zredukowany |
| waste code (EWC) | 16 02 16 |
Other proposals
Pros and cons of rare earth magnets.
Benefits
- They virtually do not lose strength, because even after 10 years the performance loss is only ~1% (based on calculations),
- Magnets perfectly defend themselves against demagnetization caused by ambient magnetic noise,
- The use of an aesthetic layer of noble metals (nickel, gold, silver) causes the element to be more visually attractive,
- The surface of neodymium magnets generates a powerful magnetic field – this is a distinguishing feature,
- Thanks to resistance to high temperature, they are capable of working (depending on the form) even at temperatures up to 230°C and higher...
- Thanks to freedom in forming and the ability to modify to unusual requirements,
- Versatile presence in modern technologies – they find application in computer drives, electromotive mechanisms, advanced medical instruments, as well as modern systems.
- Compactness – despite small sizes they provide effective action, making them ideal for precision applications
Weaknesses
- At very strong impacts they can crack, therefore we recommend placing them in strong housings. 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 recommend using waterproof magnets made of rubber, plastic or other material stable to moisture, when using outdoors
- Limited ability of producing threads in the magnet and complicated shapes - preferred is casing - magnetic holder.
- Health risk resulting from small fragments of magnets pose a threat, if swallowed, which becomes key in the context of child health protection. Furthermore, small elements of these magnets can be problematic in diagnostics medical in case of swallowing.
- Due to expensive raw materials, their price is relatively high,
Holding force characteristics
Maximum magnetic pulling force – what contributes to it?
- on a plate made of structural steel, optimally conducting the magnetic flux
- whose transverse dimension equals approx. 10 mm
- with a surface perfectly flat
- without the slightest clearance between the magnet and steel
- during detachment in a direction vertical to the plane
- in stable room temperature
Practical aspects of lifting capacity – factors
- Distance – the presence of foreign body (paint, dirt, gap) acts as an insulator, which reduces capacity rapidly (even by 50% at 0.5 mm).
- Force direction – remember that the magnet has greatest strength perpendicularly. Under shear forces, the holding force drops drastically, often to levels of 20-30% of the maximum value.
- Steel thickness – too thin plate causes magnetic saturation, causing part of the flux to be wasted into the air.
- Plate material – mild steel gives the best results. Alloy admixtures decrease magnetic properties and lifting capacity.
- Surface quality – the more even the surface, the larger the contact zone and stronger the hold. Roughness acts like micro-gaps.
- Thermal environment – temperature increase causes a temporary drop of force. It is worth remembering the thermal limit for a given model.
Lifting capacity was assessed by applying a polished steel plate of optimal thickness (min. 20 mm), under perpendicular detachment force, however under attempts to slide the magnet the holding force is lower. Additionally, even a slight gap between the magnet’s surface and the plate reduces the load capacity.
Precautions when working with neodymium magnets
Dust is flammable
Combustion risk: Neodymium dust is explosive. Avoid machining magnets in home conditions as this risks ignition.
Avoid contact if allergic
It is widely known that nickel (standard magnet coating) is a strong allergen. If you have an allergy, prevent touching magnets with bare hands and select encased magnets.
Electronic devices
Equipment safety: Neodymium magnets can ruin payment cards and sensitive devices (pacemakers, medical aids, mechanical watches).
Choking Hazard
Always keep magnets away from children. Ingestion danger is high, and the consequences of magnets connecting inside the body are fatal.
Hand protection
Risk of injury: The attraction force is so immense that it can cause blood blisters, crushing, and even bone fractures. Use thick gloves.
Implant safety
Patients with a ICD must keep an safe separation from magnets. The magnetism can stop the operation of the life-saving device.
Handling rules
Use magnets with awareness. Their immense force can surprise even professionals. Stay alert and do not underestimate their force.
Power loss in heat
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.
Material brittleness
Beware of splinters. Magnets can explode upon violent connection, launching sharp fragments into the air. Wear goggles.
Keep away from electronics
Note: rare earth magnets generate a field that interferes with precision electronics. Keep a separation from your phone, device, and navigation systems.
