MP 24x16x2 / N38 - ring magnet
ring magnet
Catalog no 030495
GTIN/EAN: 5906301812364
- Diameter
- 24 mm [±0,1 mm]
- internal diameter Ø
- 16 mm [±0,1 mm]
- Height
- 2 mm [±0,1 mm]
- Weight
- 3.77 g
- Magnetization Direction
- ↑ axial
- Coating
- [NiCuNi] Nickel
How we measure these parameters — certificates and measurements
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Need more?Frequently asked questions
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Which ring magnet is suitable for an outdoor structure?
Where can I check the available sizes of neodymium ring magnets?
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 24x16x2 / N38 - ring magnet
Specification / characteristics - MP 24x16x2 / N38 - ring magnet
| properties | values |
|---|---|
| Cat. no. | 030495 |
| GTIN/EAN | 5906301812364 |
| Distributor | Dhit sp. z o.o. |
| Country of origin | Poland / China / Germany |
| Customs code | 85059029 |
| Diameter | 24 mm [±0,1 mm] |
| internal diameter Ø | 16 mm [±0,1 mm] |
| Height | 2 mm [±0,1 mm] |
| Weight | 3.77 g |
| Magnetization Direction | ↑ axial |
| Load capacity ~ ? | 0.94 kg / 9.22 N |
| Magnetic Induction ~ ? | 101.91 mT / 1019 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 product - technical parameters
The following information constitute the direct effect of a physical analysis. Results are based on models for the material Nd2Fe14B. Actual conditions might slightly differ from theoretical values. Please consider these data as a supplementary guide during assembly planning.
Table 1: Static force (pull vs distance) - characteristics
MP 24x16x2 / N38
| Distance (mm) | Induction (Gauss) / mT | Pull Force (kg/lbs/g/N) | Risk Status |
|---|---|---|---|
| 0 mm |
1019 Gs
101.9 mT
|
0.94 kg / 2.07 LBS
940.0 g / 9.2 N
|
low risk |
| 1 mm |
989 Gs
98.9 mT
|
0.89 kg / 1.95 LBS
885.1 g / 8.7 N
|
low risk |
| 2 mm |
941 Gs
94.1 mT
|
0.80 kg / 1.77 LBS
802.1 g / 7.9 N
|
low risk |
| 3 mm |
881 Gs
88.1 mT
|
0.70 kg / 1.55 LBS
702.4 g / 6.9 N
|
low risk |
| 5 mm |
739 Gs
73.9 mT
|
0.49 kg / 1.09 LBS
494.8 g / 4.9 N
|
low risk |
| 10 mm |
415 Gs
41.5 mT
|
0.16 kg / 0.34 LBS
155.8 g / 1.5 N
|
low risk |
| 15 mm |
224 Gs
22.4 mT
|
0.05 kg / 0.10 LBS
45.3 g / 0.4 N
|
low risk |
| 20 mm |
126 Gs
12.6 mT
|
0.01 kg / 0.03 LBS
14.5 g / 0.1 N
|
low risk |
| 30 mm |
49 Gs
4.9 mT
|
0.00 kg / 0.00 LBS
2.1 g / 0.0 N
|
low risk |
| 50 mm |
12 Gs
1.2 mT
|
0.00 kg / 0.00 LBS
0.1 g / 0.0 N
|
low risk |
Table 2: Sliding load (vertical surface)
MP 24x16x2 / N38
| Distance (mm) | Friction coefficient | Pull Force (kg/lbs/g/N) |
|---|---|---|
| 0 mm | Raw steel (µ ≈ 0.2) |
0.19 kg / 0.41 LBS
188.0 g / 1.8 N
|
| 1 mm | Raw steel (µ ≈ 0.2) |
0.18 kg / 0.39 LBS
178.0 g / 1.7 N
|
| 2 mm | Raw steel (µ ≈ 0.2) |
0.16 kg / 0.35 LBS
160.0 g / 1.6 N
|
| 3 mm | Raw steel (µ ≈ 0.2) |
0.14 kg / 0.31 LBS
140.0 g / 1.4 N
|
| 5 mm | Raw steel (µ ≈ 0.2) |
0.10 kg / 0.22 LBS
98.0 g / 1.0 N
|
| 10 mm | Raw steel (µ ≈ 0.2) |
0.03 kg / 0.07 LBS
32.0 g / 0.3 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 / 0.00 LBS
2.0 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) - vertical pull
MP 24x16x2 / N38
| Surface type | Friction coefficient / % | Max load (kg/lbs/g/N) |
|---|---|---|
| Raw steel |
µ = 0.3
30% of nominal force
|
0.28 kg / 0.62 LBS
282.0 g / 2.8 N
|
| Painted steel (standard) |
µ = 0.2
20% of nominal force
|
0.19 kg / 0.41 LBS
188.0 g / 1.8 N
|
| Oily/slippery steel |
µ = 0.1
10% of nominal force
|
0.09 kg / 0.21 LBS
94.0 g / 0.9 N
|
| Magnet with anti-slip rubber |
µ = 0.5
50% of nominal force
|
0.47 kg / 1.04 LBS
470.0 g / 4.6 N
|
Table 4: Material efficiency (saturation) - power losses
MP 24x16x2 / N38
| Steel thickness (mm) | % power | Real pull force (kg/lbs/g/N) |
|---|---|---|
| 0.5 mm |
|
0.09 kg / 0.21 LBS
94.0 g / 0.9 N
|
| 1 mm |
|
0.24 kg / 0.52 LBS
235.0 g / 2.3 N
|
| 2 mm |
|
0.47 kg / 1.04 LBS
470.0 g / 4.6 N
|
| 3 mm |
|
0.71 kg / 1.55 LBS
705.0 g / 6.9 N
|
| 5 mm |
|
0.94 kg / 2.07 LBS
940.0 g / 9.2 N
|
| 10 mm |
|
0.94 kg / 2.07 LBS
940.0 g / 9.2 N
|
| 11 mm |
|
0.94 kg / 2.07 LBS
940.0 g / 9.2 N
|
| 12 mm |
|
0.94 kg / 2.07 LBS
940.0 g / 9.2 N
|
Table 5: Thermal resistance (material behavior) - power drop
MP 24x16x2 / N38
| Magnet temperature (°C) | Force change relative to 20°C | Remaining pull (kg/lbs/g/N) | Status |
|---|---|---|---|
| 20 °C | 0.0% |
0.94 kg / 2.07 LBS
940.0 g / 9.2 N
|
Estimate |
| 40 °C | -4.4% |
0.90 kg / 1.98 LBS
899.1 g / 8.8 N
|
Estimate |
| 60 °C | -8.6% |
0.86 kg / 1.89 LBS
859.1 g / 8.4 N
|
Estimate |
| 80 °C | -12.8% |
0.82 kg / 1.81 LBS
820.0 g / 8.0 N
|
Material limit |
| 100 °C | — | — | Out of range — no model |
Table 6: Magnet-Magnet interaction (repulsion) - forces in the system
MP 24x16x2 / N38
| Gap (mm) | Attraction (kg/lbs) (N-S) | Lateral Force (kg/lbs/g/N) | Repulsion (kg/lbs) (N-N) |
|---|---|---|---|
| 0 mm |
1.61 kg / 3.55 LBS
1 960 Gs
|
0.24 kg / 0.53 LBS
241 g / 2.4 N
|
N/A |
| 1 mm |
1.57 kg / 3.46 LBS
2 013 Gs
|
0.24 kg / 0.52 LBS
235 g / 2.3 N
|
1.41 kg / 3.11 LBS
~0 Gs
|
| 2 mm |
1.52 kg / 3.34 LBS
1 978 Gs
|
0.23 kg / 0.50 LBS
227 g / 2.2 N
|
1.36 kg / 3.01 LBS
~0 Gs
|
| 3 mm |
1.45 kg / 3.19 LBS
1 934 Gs
|
0.22 kg / 0.48 LBS
217 g / 2.1 N
|
1.30 kg / 2.87 LBS
~0 Gs
|
| 5 mm |
1.29 kg / 2.84 LBS
1 825 Gs
|
0.19 kg / 0.43 LBS
194 g / 1.9 N
|
1.16 kg / 2.56 LBS
~0 Gs
|
| 10 mm |
0.85 kg / 1.87 LBS
1 479 Gs
|
0.13 kg / 0.28 LBS
127 g / 1.2 N
|
0.76 kg / 1.68 LBS
~0 Gs
|
| 20 mm |
0.27 kg / 0.59 LBS
830 Gs
|
0.04 kg / 0.09 LBS
40 g / 0.4 N
|
0.24 kg / 0.53 LBS
~0 Gs
|
| 50 mm |
0.01 kg / 0.02 LBS
152 Gs
|
0.00 kg / 0.00 LBS
1 g / 0.0 N
|
0.00 kg / 0.00 LBS
~0 Gs
|
| 60 mm |
0.00 kg / 0.01 LBS
97 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
65 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
46 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
33 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
25 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
MP 24x16x2 / N38
| Field level (Gs) | mT | Model distance (cm) |
|---|---|---|
| < 5 Gs | < 0.5 mT | 7.0 cm |
| < 10 Gs | < 1.0 mT | 5.5 cm |
| < 20 Gs | < 2.0 mT | 4.5 cm |
| < 40 Gs | < 4.0 mT | 3.5 cm |
| < 50 Gs | < 5.0 mT | 3.0 cm |
| < 400 Gs | < 40.0 mT | 1.5 cm |
| < 600 Gs | < 60.0 mT | 1.0 cm |
Table 8: Dynamics (kinetic energy) - warning
MP 24x16x2 / N38
| Start from (mm) | Speed (km/h) | Energy (J) | Predicted outcome |
|---|---|---|---|
| 10 mm |
18.74 km/h
(5.21 m/s)
|
0.05 J | |
| 30 mm |
19.86 km/h
(5.52 m/s)
|
0.06 J | |
| 50 mm |
19.88 km/h
(5.52 m/s)
|
0.06 J | |
| 100 mm |
19.89 km/h
(5.52 m/s)
|
0.06 J |
Table 9: Anti-corrosion coating durability
MP 24x16x2 / 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 (Pc)
MP 24x16x2 / N38
| Parameter | Value | SI Unit / Description |
|---|---|---|
| Magnetic Flux | 4 402 Mx | 44.0 µWb |
| Pc Coefficient | 0.17 | Low (Flat) |
Table 11: Physics of underwater searching
MP 24x16x2 / N38
| Environment | Effective steel pull | Effect |
|---|---|---|
| Air (land) | 0.94 kg | Standard |
| Water (riverbed) |
1.08 kg
(+0.14 kg buoyancy gain)
|
+14.5% |
1. Vertical hold
*Note: On a vertical surface, the magnet holds just ~20% of its perpendicular strength.
2. Plate thickness effect
*Thin steel (e.g. 0.5mm PC case) severely reduces 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) = 0.17
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. At low Pc values (typical for flat magnets, below about 1) 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
Advantages and disadvantages of rare earth magnets.
Strengths
- They do not lose power, even during around ten years – the reduction in lifting capacity is only ~1% (theoretically),
- They show high resistance to demagnetization induced by external magnetic fields,
- In other words, due to the smooth surface of nickel, the element gains a professional look,
- Magnets possess maximum magnetic induction on the working surface,
- Made from properly selected components, these magnets show impressive resistance to high heat, enabling them to function (depending on their form) at temperatures up to 230°C and above...
- Thanks to flexibility in designing and the ability to modify to complex applications,
- Universal use in future technologies – they serve a role in mass storage devices, drive modules, medical equipment, and modern systems.
- Compactness – despite small sizes they offer powerful magnetic field, making them ideal for precision applications
Cons
- They are fragile upon heavy impacts. To avoid cracks, it is worth protecting magnets using a steel holder. Such protection not only protects the magnet but also increases its resistance to damage
- Do not exceed this material temperature limit: 80°C. Overheating may permanently weaken the magnet.
- When exposed to humidity, magnets start to rust. For applications outside, it is recommended to use protective magnets, such as magnets in rubber or plastics, which prevent oxidation and corrosion.
- We recommend a housing - magnetic mount, due to difficulties in realizing threads inside the magnet and complicated shapes.
- Health risk to health – tiny shards of magnets are risky, when accidentally swallowed, which becomes key in the context of child safety. Furthermore, small elements of these devices can disrupt the diagnostic process medical when they are in the body.
- Due to expensive raw materials, their price exceeds standard values,
Holding force characteristics
Maximum magnetic pulling force – what contributes to it?
- using a base made of mild steel, functioning as a magnetic yoke
- whose transverse dimension equals approx. 10 mm
- characterized by even structure
- without any clearance between the magnet and steel
- under perpendicular force vector (90-degree angle)
- at standard ambient temperature
Lifting capacity in practice – influencing factors
- Gap (betwixt the magnet and the plate), since even a microscopic clearance (e.g. 0.5 mm) results in a decrease in force by up to 50% (this also applies to varnish, corrosion or dirt).
- Loading method – declared lifting capacity refers to detachment vertically. When slipping, the magnet exhibits much less (typically approx. 20-30% of nominal force).
- Plate thickness – insufficiently thick sheet causes magnetic saturation, causing part of the flux to be escaped into the air.
- Plate material – low-carbon steel gives the best results. Higher carbon content reduce magnetic properties and lifting capacity.
- Base smoothness – the smoother and more polished the surface, the better the adhesion and stronger the hold. 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 they can be stronger (up to a certain limit).
Lifting capacity was assessed by applying a polished steel plate of optimal thickness (min. 20 mm), under vertically applied force, in contrast under shearing force the lifting capacity is smaller. Additionally, even a slight gap between the magnet’s surface and the plate reduces the load capacity.
H&S for magnets
Combustion hazard
Fire warning: Neodymium dust is highly flammable. Avoid machining magnets in home conditions as this risks ignition.
Heat warning
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.
Crushing risk
Danger of trauma: The attraction force is so immense that it can result in hematomas, pinching, and even bone fractures. Use thick gloves.
Data carriers
Do not bring magnets near a purse, laptop, or screen. The magnetism can permanently damage these devices and wipe information from cards.
Caution required
Handle magnets consciously. Their immense force can shock even professionals. Stay alert and do not underestimate their force.
Protective goggles
Neodymium magnets are ceramic materials, which means they are very brittle. Clashing of two magnets will cause them breaking into shards.
Pacemakers
For implant holders: Powerful magnets disrupt medical devices. Maintain at least 30 cm distance or ask another person to work with the magnets.
Allergy Warning
Warning for allergy sufferers: The nickel-copper-nickel coating contains nickel. If redness occurs, immediately stop working with magnets and wear gloves.
Choking Hazard
Adult use only. Tiny parts can be swallowed, causing severe trauma. Keep away from kids and pets.
Impact on smartphones
An intense magnetic field interferes with the functioning of magnetometers in smartphones and GPS navigation. Keep magnets near a device to prevent breaking the sensors.
