MPL 45x25x10 / N38 - lamellar magnet
lamellar magnet
Catalog no 020164
GTIN/EAN: 5906301811701
length
45 mm [±0,1 mm]
Width
25 mm [±0,1 mm]
Height
10 mm [±0,1 mm]
Weight
84.38 g
Magnetization Direction
↑ axial
Load capacity
28.48 kg / 279.40 N
Magnetic Induction
306.29 mT / 3063 Gs
Coating
[NiCuNi] Nickel
35.01 ZŁ with VAT / pcs + price for transport
28.46 ZŁ net + 23% VAT / pcs
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MPL 45x25x10 / N38 - lamellar magnet
Specification / characteristics MPL 45x25x10 / N38 - lamellar magnet
| properties | values |
|---|---|
| Cat. no. | 020164 |
| GTIN/EAN | 5906301811701 |
| Production/Distribution | Dhit sp. z o.o. |
| Country of origin | Poland / China / Germany |
| Customs code | 85059029 |
| length | 45 mm [±0,1 mm] |
| Width | 25 mm [±0,1 mm] |
| Height | 10 mm [±0,1 mm] |
| Weight | 84.38 g |
| Magnetization Direction | ↑ axial |
| Load capacity ~ ? | 28.48 kg / 279.40 N |
| Magnetic Induction ~ ? | 306.29 mT / 3063 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 |
Technical simulation of the product - report
Presented information represent the direct effect of a mathematical simulation. Results rely on algorithms for the material Nd2Fe14B. Actual parameters may deviate from the simulation results. Please consider these data as a preliminary roadmap during assembly planning.
MPL 45x25x10 / N38
| Distance (mm) | Induction (Gauss) / mT | Pull Force (kg) | Risk Status |
|---|---|---|---|
| 0 mm |
3062 Gs
306.2 mT
|
28.48 kg / 28480.0 g
279.4 N
|
critical level |
| 1 mm |
2918 Gs
291.8 mT
|
25.86 kg / 25856.7 g
253.7 N
|
critical level |
| 2 mm |
2760 Gs
276.0 mT
|
23.13 kg / 23133.2 g
226.9 N
|
critical level |
| 3 mm |
2595 Gs
259.5 mT
|
20.45 kg / 20449.5 g
200.6 N
|
critical level |
| 5 mm |
2261 Gs
226.1 mT
|
15.53 kg / 15525.8 g
152.3 N
|
critical level |
| 10 mm |
1529 Gs
152.9 mT
|
7.10 kg / 7096.1 g
69.6 N
|
strong |
| 15 mm |
1018 Gs
101.8 mT
|
3.15 kg / 3147.4 g
30.9 N
|
strong |
| 20 mm |
688 Gs
68.8 mT
|
1.44 kg / 1439.4 g
14.1 N
|
safe |
| 30 mm |
340 Gs
34.0 mT
|
0.35 kg / 350.8 g
3.4 N
|
safe |
| 50 mm |
111 Gs
11.1 mT
|
0.04 kg / 37.1 g
0.4 N
|
safe |
MPL 45x25x10 / N38
| Distance (mm) | Friction coefficient | Pull Force (kg) |
|---|---|---|
| 0 mm | Stal (~0.2) |
5.70 kg / 5696.0 g
55.9 N
|
| 1 mm | Stal (~0.2) |
5.17 kg / 5172.0 g
50.7 N
|
| 2 mm | Stal (~0.2) |
4.63 kg / 4626.0 g
45.4 N
|
| 3 mm | Stal (~0.2) |
4.09 kg / 4090.0 g
40.1 N
|
| 5 mm | Stal (~0.2) |
3.11 kg / 3106.0 g
30.5 N
|
| 10 mm | Stal (~0.2) |
1.42 kg / 1420.0 g
13.9 N
|
| 15 mm | Stal (~0.2) |
0.63 kg / 630.0 g
6.2 N
|
| 20 mm | Stal (~0.2) |
0.29 kg / 288.0 g
2.8 N
|
| 30 mm | Stal (~0.2) |
0.07 kg / 70.0 g
0.7 N
|
| 50 mm | Stal (~0.2) |
0.01 kg / 8.0 g
0.1 N
|
MPL 45x25x10 / N38
| Surface type | Friction coefficient / % Mocy | Max load (kg) |
|---|---|---|
| Raw steel |
µ = 0.3
30% Nominalnej Siły
|
8.54 kg / 8544.0 g
83.8 N
|
| Painted steel (standard) |
µ = 0.2
20% Nominalnej Siły
|
5.70 kg / 5696.0 g
55.9 N
|
| Oily/slippery steel |
µ = 0.1
10% Nominalnej Siły
|
2.85 kg / 2848.0 g
27.9 N
|
| Magnet with anti-slip rubber |
µ = 0.5
50% Nominalnej Siły
|
14.24 kg / 14240.0 g
139.7 N
|
MPL 45x25x10 / N38
| Steel thickness (mm) | % power | Real pull force (kg) |
|---|---|---|
| 0.5 mm |
|
1.42 kg / 1424.0 g
14.0 N
|
| 1 mm |
|
3.56 kg / 3560.0 g
34.9 N
|
| 2 mm |
|
7.12 kg / 7120.0 g
69.8 N
|
| 5 mm |
|
17.80 kg / 17800.0 g
174.6 N
|
| 10 mm |
|
28.48 kg / 28480.0 g
279.4 N
|
MPL 45x25x10 / N38
| Ambient temp. (°C) | Power loss | Remaining pull | Status |
|---|---|---|---|
| 20 °C | 0.0% |
28.48 kg / 28480.0 g
279.4 N
|
OK |
| 40 °C | -2.2% |
27.85 kg / 27853.4 g
273.2 N
|
OK |
| 60 °C | -4.4% |
27.23 kg / 27226.9 g
267.1 N
|
|
| 80 °C | -6.6% |
26.60 kg / 26600.3 g
260.9 N
|
|
| 100 °C | -28.8% |
20.28 kg / 20277.8 g
198.9 N
|
MPL 45x25x10 / N38
| Gap (mm) | Attraction (kg) (N-S) | Repulsion (kg) (N-N) |
|---|---|---|
| 0 mm |
65.04 kg / 65044 g
638.1 N
4 590 Gs
|
N/A |
| 1 mm |
62.12 kg / 62117 g
609.4 N
5 985 Gs
|
55.91 kg / 55906 g
548.4 N
~0 Gs
|
| 2 mm |
59.05 kg / 59053 g
579.3 N
5 836 Gs
|
53.15 kg / 53148 g
521.4 N
~0 Gs
|
| 3 mm |
55.95 kg / 55947 g
548.8 N
5 680 Gs
|
50.35 kg / 50352 g
494.0 N
~0 Gs
|
| 5 mm |
49.74 kg / 49743 g
488.0 N
5 356 Gs
|
44.77 kg / 44769 g
439.2 N
~0 Gs
|
| 10 mm |
35.46 kg / 35459 g
347.9 N
4 522 Gs
|
31.91 kg / 31913 g
313.1 N
~0 Gs
|
| 20 mm |
16.21 kg / 16206 g
159.0 N
3 057 Gs
|
14.59 kg / 14586 g
143.1 N
~0 Gs
|
| 50 mm |
1.58 kg / 1580 g
15.5 N
955 Gs
|
1.42 kg / 1422 g
14.0 N
~0 Gs
|
MPL 45x25x10 / N38
| Object / Device | Limit (Gauss) / mT | Safe distance |
|---|---|---|
| Pacemaker | 5 Gs (0.5 mT) | 16.0 cm |
| Hearing aid | 10 Gs (1.0 mT) | 12.5 cm |
| Mechanical watch | 20 Gs (2.0 mT) | 10.0 cm |
| Mobile device | 40 Gs (4.0 mT) | 7.5 cm |
| Remote | 50 Gs (5.0 mT) | 7.0 cm |
| Payment card | 400 Gs (40.0 mT) | 3.0 cm |
| HDD hard drive | 600 Gs (60.0 mT) | 2.5 cm |
MPL 45x25x10 / N38
| Start from (mm) | Speed (km/h) | Energy (J) | Predicted outcome |
|---|---|---|---|
| 10 mm |
21.22 km/h
(5.89 m/s)
|
1.47 J | |
| 30 mm |
32.34 km/h
(8.98 m/s)
|
3.40 J | |
| 50 mm |
41.46 km/h
(11.52 m/s)
|
5.60 J | |
| 100 mm |
58.59 km/h
(16.28 m/s)
|
11.18 J |
MPL 45x25x10 / 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) |
MPL 45x25x10 / N38
| Parameter | Value | SI Unit / Description |
|---|---|---|
| Magnetic Flux | 35 829 Mx | 358.3 µWb |
| Pc Coefficient | 0.36 | Low (Flat) |
MPL 45x25x10 / N38
| Environment | Effective steel pull | Effect |
|---|---|---|
| Air (land) | 28.48 kg | Standard |
| Water (riverbed) |
32.61 kg
(+4.13 kg Buoyancy gain)
|
+14.5% |
1. Vertical hold
*Note: On a vertical surface, the magnet retains only approx. 20-30% of its perpendicular strength.
2. Steel thickness impact
*Thin metal sheet (e.g. computer case) significantly reduces the holding force.
3. Temperature resistance
*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) = 0.36
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.
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 products
Pros as well as cons of rare earth magnets.
Strengths
- They have stable power, and over nearly 10 years their performance decreases symbolically – ~1% (in testing),
- Magnets effectively resist against loss of magnetization caused by ambient magnetic noise,
- In other words, due to the shiny surface of nickel, the element gains a professional look,
- Magnetic induction on the top side of the magnet is exceptional,
- Thanks to resistance to high temperature, they can operate (depending on the shape) even at temperatures up to 230°C and higher...
- Possibility of exact shaping and modifying to defined applications,
- Wide application in advanced technology sectors – they are utilized in computer drives, electric drive systems, advanced medical instruments, as well as other advanced devices.
- Relatively small size with high pulling force – neodymium magnets offer strong magnetic field in compact dimensions, which allows their use in miniature devices
Cons
- Susceptibility to cracking is one of their disadvantages. Upon intense impact they can break. We advise keeping them in a special holder, which not only secures them against impacts but also increases their durability
- When exposed to high temperature, neodymium magnets experience a drop in strength. Often, when the temperature exceeds 80°C, their strength decreases (depending on the size and shape of the magnet). For those who need magnets for extreme conditions, we offer [AH] versions withstanding up to 230°C
- They oxidize in a humid environment - during use outdoors we suggest using waterproof magnets e.g. in rubber, plastic
- Due to limitations in producing threads and complicated shapes in magnets, we recommend using casing - magnetic mechanism.
- Potential hazard resulting from small fragments of magnets are risky, in case of ingestion, which gains importance in the context of child safety. It is also worth noting that tiny parts of these devices can disrupt the diagnostic process medical in case of swallowing.
- Due to expensive raw materials, their price exceeds standard values,
Lifting parameters
Best holding force of the magnet in ideal parameters – what it depends on?
- with the application of a yoke made of low-carbon steel, ensuring maximum field concentration
- possessing a thickness of min. 10 mm to ensure full flux closure
- characterized by even structure
- without any clearance between the magnet and steel
- during detachment in a direction vertical to the plane
- at ambient temperature room level
Key elements affecting lifting force
- Space between surfaces – every millimeter of distance (caused e.g. by veneer or unevenness) drastically reduces the pulling force, often by half at just 0.5 mm.
- Direction of force – highest force is available only during pulling at a 90° angle. The shear force of the magnet along the plate is typically several times smaller (approx. 1/5 of the lifting capacity).
- Element thickness – to utilize 100% power, the steel must be sufficiently thick. Thin sheet limits the lifting capacity (the magnet "punches through" it).
- Steel grade – ideal substrate is high-permeability steel. Stainless steels may attract less.
- Surface quality – the more even the plate, the better the adhesion and higher the lifting capacity. Unevenness acts like micro-gaps.
- Temperature influence – high temperature weakens magnetic field. Exceeding the limit temperature can permanently damage the magnet.
Holding force was tested on the plate surface of 20 mm thickness, when the force acted perpendicularly, in contrast under attempts to slide the magnet the holding force is lower. Additionally, even a slight gap between the magnet’s surface and the plate decreases the load capacity.
Fragile material
Neodymium magnets are ceramic materials, meaning they are very brittle. Collision of two magnets leads to them cracking into shards.
Safe operation
Handle with care. Rare earth magnets act from a long distance and snap with massive power, often faster than you can react.
Demagnetization risk
Monitor thermal conditions. Heating the magnet above 80 degrees Celsius will destroy its magnetic structure and strength.
Precision electronics
GPS units and mobile phones are highly sensitive to magnetic fields. Close proximity with a powerful NdFeB magnet can permanently damage the internal compass in your phone.
Dust is flammable
Machining of NdFeB material carries a risk of fire hazard. Neodymium dust oxidizes rapidly with oxygen and is hard to extinguish.
Physical harm
Large magnets can smash fingers instantly. Under no circumstances put your hand betwixt two attracting surfaces.
Do not give to children
Always store magnets away from children. Ingestion danger is high, and the consequences of magnets connecting inside the body are tragic.
Danger to pacemakers
Medical warning: Neodymium magnets can turn off pacemakers and defibrillators. Stay away if you have electronic implants.
Sensitization to coating
It is widely known that the nickel plating (the usual finish) is a common allergen. For allergy sufferers, refrain from touching magnets with bare hands and select encased magnets.
Magnetic media
Equipment safety: Neodymium magnets can damage data carriers and delicate electronics (heart implants, medical aids, timepieces).
