MP 5x2.7/1.2x5 Z / N38 - ring magnet
ring magnet
Catalog no 030203
GTIN/EAN: 5906301812203
- Diameter
- 5 mm [±0,1 mm]
- internal diameter Ø
- 2.7/1.2 mm [±0,1 mm]
- Height
- 5 mm [±0,1 mm]
- Weight
- 0.69 g
- Magnetization Direction
- ↑ axial
- Coating
- [NiCuNi] Nickel
How we measure these parameters — certificates and measurements
0.680 zł net / pcs
0.836 zł with VAT (23% VAT) / pcs
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Need more?Frequently asked questions
What is the hole in a ring magnet for?
What is the polarisation?
What sizes are available?
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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Product card - MP 5x2.7/1.2x5 Z / N38 - ring magnet
Specification / characteristics - MP 5x2.7/1.2x5 Z / N38 - ring magnet
| properties | values |
|---|---|
| Cat. no. | 030203 |
| GTIN/EAN | 5906301812203 |
| Production/Distribution | Dhit sp. z o.o. |
| Country of origin | Poland / China / Germany |
| Customs code | 85059029 |
| Diameter | 5 mm [±0,1 mm] |
| internal diameter Ø | 2.7/1.2 mm [±0,1 mm] |
| Height | 5 mm [±0,1 mm] |
| Weight | 0.69 g |
| Magnetization Direction | ↑ axial |
| Load capacity ~ ? | 0.75 kg / 7.31 N |
| Magnetic Induction ~ ? | 553.14 mT / 5531 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 simulation of the assembly - report
Presented data represent the result of a engineering simulation. Results were calculated on algorithms for the class Nd2Fe14B. Real-world performance might slightly deviate from the simulation results. Please consider these calculations as a supplementary guide for designers.
Table 1: Static pull force (pull vs gap) - interaction chart
MP 5x2.7/1.2x5 Z / N38
| Distance (mm) | Induction (Gauss) / mT | Pull Force (kg/lbs/g/N) | Risk Status |
|---|---|---|---|
| 0 mm |
5322 Gs
532.2 mT
|
0.75 kg / 1.65 pounds
750.0 g / 7.4 N
|
weak grip |
| 1 mm |
3295 Gs
329.5 mT
|
0.29 kg / 0.63 pounds
287.5 g / 2.8 N
|
weak grip |
| 2 mm |
1883 Gs
188.3 mT
|
0.09 kg / 0.21 pounds
93.9 g / 0.9 N
|
weak grip |
| 3 mm |
1098 Gs
109.8 mT
|
0.03 kg / 0.07 pounds
31.9 g / 0.3 N
|
weak grip |
| 5 mm |
440 Gs
44.0 mT
|
0.01 kg / 0.01 pounds
5.1 g / 0.1 N
|
weak grip |
| 10 mm |
92 Gs
9.2 mT
|
0.00 kg / 0.00 pounds
0.2 g / 0.0 N
|
weak grip |
| 15 mm |
33 Gs
3.3 mT
|
0.00 kg / 0.00 pounds
0.0 g / 0.0 N
|
weak grip |
| 20 mm |
15 Gs
1.5 mT
|
0.00 kg / 0.00 pounds
0.0 g / 0.0 N
|
weak grip |
| 30 mm |
5 Gs
0.5 mT
|
0.00 kg / 0.00 pounds
0.0 g / 0.0 N
|
weak grip |
| 50 mm |
1 Gs
0.1 mT
|
0.00 kg / 0.00 pounds
0.0 g / 0.0 N
|
weak grip |
Table 2: Slippage capacity (vertical surface)
MP 5x2.7/1.2x5 Z / N38
| Distance (mm) | Friction coefficient | Pull Force (kg/lbs/g/N) |
|---|---|---|
| 0 mm | Stal (~0.2) |
0.15 kg / 0.33 pounds
150.0 g / 1.5 N
|
| 1 mm | Stal (~0.2) |
0.06 kg / 0.13 pounds
58.0 g / 0.6 N
|
| 2 mm | Stal (~0.2) |
0.02 kg / 0.04 pounds
18.0 g / 0.2 N
|
| 3 mm | Stal (~0.2) |
0.01 kg / 0.01 pounds
6.0 g / 0.1 N
|
| 5 mm | Stal (~0.2) |
0.00 kg / 0.00 pounds
2.0 g / 0.0 N
|
| 10 mm | Stal (~0.2) |
0.00 kg / 0.00 pounds
0.0 g / 0.0 N
|
| 15 mm | Stal (~0.2) |
0.00 kg / 0.00 pounds
0.0 g / 0.0 N
|
| 20 mm | Stal (~0.2) |
0.00 kg / 0.00 pounds
0.0 g / 0.0 N
|
| 30 mm | Stal (~0.2) |
0.00 kg / 0.00 pounds
0.0 g / 0.0 N
|
| 50 mm | Stal (~0.2) |
0.00 kg / 0.00 pounds
0.0 g / 0.0 N
|
Table 3: Wall mounting (shearing) - vertical pull
MP 5x2.7/1.2x5 Z / N38
| Surface type | Friction coefficient / % Mocy | Max load (kg/lbs/g/N) |
|---|---|---|
| Raw steel |
µ = 0.3
30% Nominalnej Siły
|
0.22 kg / 0.50 pounds
225.0 g / 2.2 N
|
| Painted steel (standard) |
µ = 0.2
20% Nominalnej Siły
|
0.15 kg / 0.33 pounds
150.0 g / 1.5 N
|
| Oily/slippery steel |
µ = 0.1
10% Nominalnej Siły
|
0.08 kg / 0.17 pounds
75.0 g / 0.7 N
|
| Magnet with anti-slip rubber |
µ = 0.5
50% Nominalnej Siły
|
0.38 kg / 0.83 pounds
375.0 g / 3.7 N
|
Table 4: Steel thickness (saturation) - power losses
MP 5x2.7/1.2x5 Z / N38
| Steel thickness (mm) | % power | Real pull force (kg/lbs/g/N) |
|---|---|---|
| 0.5 mm |
|
0.08 kg / 0.17 pounds
75.0 g / 0.7 N
|
| 1 mm |
|
0.19 kg / 0.41 pounds
187.5 g / 1.8 N
|
| 2 mm |
|
0.38 kg / 0.83 pounds
375.0 g / 3.7 N
|
| 3 mm |
|
0.56 kg / 1.24 pounds
562.5 g / 5.5 N
|
| 5 mm |
|
0.75 kg / 1.65 pounds
750.0 g / 7.4 N
|
| 10 mm |
|
0.75 kg / 1.65 pounds
750.0 g / 7.4 N
|
| 11 mm |
|
0.75 kg / 1.65 pounds
750.0 g / 7.4 N
|
| 12 mm |
|
0.75 kg / 1.65 pounds
750.0 g / 7.4 N
|
Table 5: Thermal stability (stability) - power drop
MP 5x2.7/1.2x5 Z / N38
| Ambient temp. (°C) | Power loss | Remaining pull (kg/lbs/g/N) | Status |
|---|---|---|---|
| 20 °C | 0.0% |
0.75 kg / 1.65 pounds
750.0 g / 7.4 N
|
OK |
| 40 °C | -2.2% |
0.73 kg / 1.62 pounds
733.5 g / 7.2 N
|
OK |
| 60 °C | -4.4% |
0.72 kg / 1.58 pounds
717.0 g / 7.0 N
|
OK |
| 80 °C | -6.6% |
0.70 kg / 1.54 pounds
700.5 g / 6.9 N
|
|
| 100 °C | -28.8% |
0.53 kg / 1.18 pounds
534.0 g / 5.2 N
|
Table 6: Magnet-Magnet interaction (repulsion) - field collision
MP 5x2.7/1.2x5 Z / N38
| Gap (mm) | Attraction (kg/lbs) (N-S) | Lateral Force (kg/lbs/g/N) | Repulsion (kg/lbs) (N-N) |
|---|---|---|---|
| 0 mm |
2.75 kg / 6.06 pounds
5 924 Gs
|
0.41 kg / 0.91 pounds
412 g / 4.0 N
|
N/A |
| 1 mm |
1.77 kg / 3.90 pounds
8 541 Gs
|
0.27 kg / 0.58 pounds
265 g / 2.6 N
|
1.59 kg / 3.51 pounds
~0 Gs
|
| 2 mm |
1.05 kg / 2.32 pounds
6 590 Gs
|
0.16 kg / 0.35 pounds
158 g / 1.5 N
|
0.95 kg / 2.09 pounds
~0 Gs
|
| 3 mm |
0.60 kg / 1.33 pounds
4 992 Gs
|
0.09 kg / 0.20 pounds
91 g / 0.9 N
|
0.54 kg / 1.20 pounds
~0 Gs
|
| 5 mm |
0.20 kg / 0.44 pounds
2 860 Gs
|
0.03 kg / 0.07 pounds
30 g / 0.3 N
|
0.18 kg / 0.39 pounds
~0 Gs
|
| 10 mm |
0.02 kg / 0.04 pounds
880 Gs
|
0.00 kg / 0.01 pounds
3 g / 0.0 N
|
0.02 kg / 0.04 pounds
~0 Gs
|
| 20 mm |
0.00 kg / 0.00 pounds
184 Gs
|
0.00 kg / 0.00 pounds
0 g / 0.0 N
|
0.00 kg / 0.00 pounds
~0 Gs
|
| 50 mm |
0.00 kg / 0.00 pounds
16 Gs
|
0.00 kg / 0.00 pounds
0 g / 0.0 N
|
0.00 kg / 0.00 pounds
~0 Gs
|
| 60 mm |
0.00 kg / 0.00 pounds
10 Gs
|
0.00 kg / 0.00 pounds
0 g / 0.0 N
|
0.00 kg / 0.00 pounds
~0 Gs
|
| 70 mm |
0.00 kg / 0.00 pounds
6 Gs
|
0.00 kg / 0.00 pounds
0 g / 0.0 N
|
0.00 kg / 0.00 pounds
~0 Gs
|
| 80 mm |
0.00 kg / 0.00 pounds
4 Gs
|
0.00 kg / 0.00 pounds
0 g / 0.0 N
|
0.00 kg / 0.00 pounds
~0 Gs
|
| 90 mm |
0.00 kg / 0.00 pounds
3 Gs
|
0.00 kg / 0.00 pounds
0 g / 0.0 N
|
0.00 kg / 0.00 pounds
~0 Gs
|
| 100 mm |
0.00 kg / 0.00 pounds
2 Gs
|
0.00 kg / 0.00 pounds
0 g / 0.0 N
|
0.00 kg / 0.00 pounds
~0 Gs
|
Table 7: Protective zones (implants) - warnings
MP 5x2.7/1.2x5 Z / 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 |
| Car key | 50 Gs (5.0 mT) | 1.5 cm |
| Payment card | 400 Gs (40.0 mT) | 1.0 cm |
| HDD hard drive | 600 Gs (60.0 mT) | 0.5 cm |
Table 8: Collisions (cracking risk) - collision effects
MP 5x2.7/1.2x5 Z / N38
| Start from (mm) | Speed (km/h) | Energy (J) | Predicted outcome |
|---|---|---|---|
| 10 mm |
16.76 km/h
(4.65 m/s)
|
0.01 J | |
| 30 mm |
16.76 km/h
(4.66 m/s)
|
0.01 J | |
| 50 mm |
16.76 km/h
(4.66 m/s)
|
0.01 J | |
| 100 mm |
16.76 km/h
(4.66 m/s)
|
0.01 J |
Table 9: Corrosion resistance
MP 5x2.7/1.2x5 Z / 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)
MP 5x2.7/1.2x5 Z / N38
| Parameter | Value | SI Unit / Description |
|---|---|---|
| Magnetic Flux | 862 Mx | 8.6 µWb |
| Pc Coefficient | 0.83 | High (Stable) |
Table 11: Hydrostatics and buoyancy
MP 5x2.7/1.2x5 Z / N38
| Environment | Effective steel pull | Effect |
|---|---|---|
| Air (land) | 0.75 kg | Standard |
| Water (riverbed) |
0.86 kg
(+0.11 kg buoyancy gain)
|
+14.5% |
1. Sliding resistance
*Warning: On a vertical surface, the magnet holds merely ~20% of its perpendicular strength.
2. Steel saturation
*Thin metal sheet (e.g. computer case) drastically weakens 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) = 0.83
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.
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% |
Ecology and recycling (GPSR)
| recyclability (EoL) | 100% |
| recycled raw materials | ~10% (pre-cons) |
| carbon footprint | low / zredukowany |
| waste code (EWC) | 16 02 16 |
See also products
Strengths and weaknesses of rare earth magnets.
Benefits
- They virtually do not lose power, because even after 10 years the decline in efficiency is only ~1% (based on calculations),
- They show high resistance to demagnetization induced by presence of other magnetic fields,
- The use of an metallic layer of noble metals (nickel, gold, silver) causes the element to look better,
- They are known for high magnetic induction at the operating surface, which improves attraction properties,
- Through (adequate) combination of ingredients, they can achieve high thermal resistance, allowing for action at temperatures approaching 230°C and above...
- Thanks to the option of precise shaping and adaptation to unique requirements, magnetic components can be created in a wide range of geometric configurations, which amplifies use scope,
- Huge importance in future technologies – they serve a role in mass storage devices, motor assemblies, diagnostic systems, and industrial machines.
- Thanks to efficiency per cm³, small magnets offer high operating force, in miniature format,
Limitations
- They are prone to damage upon too strong impacts. To avoid cracks, it is worth protecting magnets using a steel holder. Such protection not only shields the magnet but also improves its resistance to damage
- When exposed to high temperature, neodymium magnets experience a drop in force. Often, when the temperature exceeds 80°C, their power decreases (depending on the size, as well as 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. For use outdoors we recommend using waterproof magnets e.g. in rubber, plastic
- We suggest casing - magnetic mount, due to difficulties in creating nuts inside the magnet and complicated forms.
- Health risk to health – tiny shards of magnets pose a threat, in case of ingestion, which is particularly important in the context of child safety. Furthermore, small elements of these magnets are able to be problematic in diagnostics medical after entering the body.
- With mass production the cost of neodymium magnets is a challenge,
Pull force analysis
Best holding force of the magnet in ideal parameters – what affects it?
- with the application of a yoke made of low-carbon steel, guaranteeing maximum field concentration
- with a thickness minimum 10 mm
- with an ground touching surface
- with zero gap (without paint)
- during detachment in a direction perpendicular to the mounting surface
- in stable room temperature
Determinants of lifting force in real conditions
- Gap between surfaces – even a fraction of a millimeter of separation (caused e.g. by varnish or unevenness) drastically reduces the pulling force, often by half at just 0.5 mm.
- Force direction – note that the magnet has greatest strength perpendicularly. Under sliding down, the capacity drops significantly, often to levels of 20-30% of the maximum value.
- Substrate thickness – for full efficiency, the steel must be sufficiently thick. Paper-thin metal restricts the attraction force (the magnet "punches through" it).
- Material composition – not every steel attracts identically. Alloy additives worsen the attraction effect.
- Surface structure – the smoother and more polished the plate, the larger the contact zone and higher the lifting capacity. Unevenness creates an air distance.
- Thermal conditions – NdFeB sinters have a sensitivity to temperature. When it is hot they are weaker, and at low temperatures gain strength (up to a certain limit).
Holding force was measured on a smooth steel plate of 20 mm thickness, when a perpendicular force was applied, whereas under parallel forces the load capacity is reduced by as much as 75%. Additionally, even a small distance between the magnet’s surface and the plate decreases the lifting capacity.
Safety rules for work with neodymium magnets
Fire risk
Fire warning: Rare earth powder is highly flammable. Do not process magnets without safety gear as this risks ignition.
Do not give to children
Neodymium magnets are not suitable for play. Eating several magnets can lead to them pinching intestinal walls, which constitutes a critical condition and requires urgent medical intervention.
Magnetic interference
A strong magnetic field interferes with the operation of compasses in smartphones and GPS navigation. Do not bring magnets near a smartphone to prevent damaging the sensors.
Caution required
Before use, check safety instructions. Uncontrolled attraction can break the magnet or hurt your hand. Be predictive.
Warning for allergy sufferers
Medical facts indicate that nickel (the usual finish) is a strong allergen. For allergy sufferers, refrain from touching magnets with bare hands and choose encased magnets.
Thermal limits
Control the heat. Heating the magnet to high heat will ruin its magnetic structure and pulling force.
Keep away from computers
Do not bring magnets close to a purse, computer, or TV. The magnetism can permanently damage these devices and wipe information from cards.
Bodily injuries
Big blocks can break fingers instantly. Under no circumstances place your hand between two strong magnets.
Medical implants
Individuals with a pacemaker should maintain an safe separation from magnets. The magnetism can interfere with the functioning of the life-saving device.
Material brittleness
Neodymium magnets are ceramic materials, meaning they are very brittle. Collision of two magnets leads to them breaking into small pieces.
