MW 7x1.2 / N38 - cylindrical magnet
cylindrical magnet
Catalog no 010593
GTIN/EAN: 5906301815877
- Diameter Ø
- 7 mm [±0,1 mm]
- Height
- 1.2 mm [±0,1 mm]
- Weight
- 0.35 g
- Magnetization Direction
- ↑ axial
- Coating
- [NiCuNi] Nickel
How we measure these parameters — certificates and measurements
0.1800 zł net / pcs
0.221 zł with VAT (23% VAT) / pcs
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Need more?Frequently asked questions
Where can I buy strong cylindrical neodymium magnets?
Can a small cylindrical magnet provide a strong grip for precise workshop work?
Which cylindrical magnet can work at a higher temperature?
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 - MW 7x1.2 / N38 - cylindrical magnet
Specification / characteristics - MW 7x1.2 / N38 - cylindrical magnet
| properties | values |
|---|---|
| Cat. no. | 010593 |
| GTIN/EAN | 5906301815877 |
| Distributor | Dhit sp. z o.o. |
| Country of origin | Poland / China / Germany |
| Customs code | 85059029 |
| Diameter Ø | 7 mm [±0,1 mm] |
| Height | 1.2 mm [±0,1 mm] |
| Weight | 0.35 g |
| Magnetization Direction | ↑ axial |
| Load capacity ~ ? | 0.49 kg / 4.81 N |
| Magnetic Induction ~ ? | 200.91 mT / 2009 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 modeling of the assembly - report
These information constitute the direct effect of a mathematical analysis. Results were calculated on algorithms for the material Nd2Fe14B. Operational conditions may differ from theoretical values. Treat these calculations as a reference point when designing systems.
Table 1: Static force (pull vs distance) - interaction chart
MW 7x1.2 / N38
| Distance (mm) | Induction (Gauss) / mT | Pull Force (kg/lbs/g/N) | Risk Status |
|---|---|---|---|
| 0 mm |
2008 Gs
200.8 mT
|
0.49 kg / 1.08 pounds
490.0 g / 4.8 N
|
low risk |
| 1 mm |
1596 Gs
159.6 mT
|
0.31 kg / 0.68 pounds
309.6 g / 3.0 N
|
low risk |
| 2 mm |
1108 Gs
110.8 mT
|
0.15 kg / 0.33 pounds
149.0 g / 1.5 N
|
low risk |
| 3 mm |
728 Gs
72.8 mT
|
0.06 kg / 0.14 pounds
64.4 g / 0.6 N
|
low risk |
| 5 mm |
320 Gs
32.0 mT
|
0.01 kg / 0.03 pounds
12.4 g / 0.1 N
|
low risk |
| 10 mm |
66 Gs
6.6 mT
|
0.00 kg / 0.00 pounds
0.5 g / 0.0 N
|
low risk |
| 15 mm |
22 Gs
2.2 mT
|
0.00 kg / 0.00 pounds
0.1 g / 0.0 N
|
low risk |
| 20 mm |
10 Gs
1.0 mT
|
0.00 kg / 0.00 pounds
0.0 g / 0.0 N
|
low risk |
| 30 mm |
3 Gs
0.3 mT
|
0.00 kg / 0.00 pounds
0.0 g / 0.0 N
|
low risk |
| 50 mm |
1 Gs
0.1 mT
|
0.00 kg / 0.00 pounds
0.0 g / 0.0 N
|
low risk |
Table 2: Vertical hold (vertical surface)
MW 7x1.2 / N38
| Distance (mm) | Friction coefficient | Pull Force (kg/lbs/g/N) |
|---|---|---|
| 0 mm | Raw steel (µ ≈ 0.2) |
0.10 kg / 0.22 pounds
98.0 g / 1.0 N
|
| 1 mm | Raw steel (µ ≈ 0.2) |
0.06 kg / 0.14 pounds
62.0 g / 0.6 N
|
| 2 mm | Raw steel (µ ≈ 0.2) |
0.03 kg / 0.07 pounds
30.0 g / 0.3 N
|
| 3 mm | Raw steel (µ ≈ 0.2) |
0.01 kg / 0.03 pounds
12.0 g / 0.1 N
|
| 5 mm | Raw steel (µ ≈ 0.2) |
0.00 kg / 0.00 pounds
2.0 g / 0.0 N
|
| 10 mm | Raw steel (µ ≈ 0.2) |
0.00 kg / 0.00 pounds
0.0 g / 0.0 N
|
| 15 mm | Raw steel (µ ≈ 0.2) |
0.00 kg / 0.00 pounds
0.0 g / 0.0 N
|
| 20 mm | Raw steel (µ ≈ 0.2) |
0.00 kg / 0.00 pounds
0.0 g / 0.0 N
|
| 30 mm | Raw steel (µ ≈ 0.2) |
0.00 kg / 0.00 pounds
0.0 g / 0.0 N
|
| 50 mm | Raw steel (µ ≈ 0.2) |
0.00 kg / 0.00 pounds
0.0 g / 0.0 N
|
Table 3: Vertical assembly (sliding) - vertical pull
MW 7x1.2 / N38
| Surface type | Friction coefficient / % | Max load (kg/lbs/g/N) |
|---|---|---|
| Raw steel |
µ = 0.3
30% of nominal force
|
0.15 kg / 0.32 pounds
147.0 g / 1.4 N
|
| Painted steel (standard) |
µ = 0.2
20% of nominal force
|
0.10 kg / 0.22 pounds
98.0 g / 1.0 N
|
| Oily/slippery steel |
µ = 0.1
10% of nominal force
|
0.05 kg / 0.11 pounds
49.0 g / 0.5 N
|
| Magnet with anti-slip rubber |
µ = 0.5
50% of nominal force
|
0.25 kg / 0.54 pounds
245.0 g / 2.4 N
|
Table 4: Material efficiency (saturation) - sheet metal selection
MW 7x1.2 / N38
| Steel thickness (mm) | % power | Real pull force (kg/lbs/g/N) |
|---|---|---|
| 0.5 mm |
|
0.05 kg / 0.11 pounds
49.0 g / 0.5 N
|
| 1 mm |
|
0.12 kg / 0.27 pounds
122.5 g / 1.2 N
|
| 2 mm |
|
0.25 kg / 0.54 pounds
245.0 g / 2.4 N
|
| 3 mm |
|
0.37 kg / 0.81 pounds
367.5 g / 3.6 N
|
| 5 mm |
|
0.49 kg / 1.08 pounds
490.0 g / 4.8 N
|
| 10 mm |
|
0.49 kg / 1.08 pounds
490.0 g / 4.8 N
|
| 11 mm |
|
0.49 kg / 1.08 pounds
490.0 g / 4.8 N
|
| 12 mm |
|
0.49 kg / 1.08 pounds
490.0 g / 4.8 N
|
Table 5: Working in heat (stability) - power drop
MW 7x1.2 / N38
| Magnet temperature (°C) | Force change relative to 20°C | Remaining pull (kg/lbs/g/N) | Status |
|---|---|---|---|
| 20 °C | 0.0% |
0.49 kg / 1.08 pounds
490.0 g / 4.8 N
|
Estimate |
| 40 °C | -4.4% |
0.47 kg / 1.03 pounds
468.7 g / 4.6 N
|
Estimate |
| 60 °C | -8.6% |
0.45 kg / 0.99 pounds
447.8 g / 4.4 N
|
Estimate |
| 80 °C | -12.8% |
0.43 kg / 0.94 pounds
427.5 g / 4.2 N
|
Material limit |
| 100 °C | — | — | Out of range — no model |
Table 6: Two magnets (repulsion) - field range
MW 7x1.2 / N38
| Gap (mm) | Attraction (kg/lbs) (N-S) | Shear Force (kg/lbs/g/N) | Repulsion (kg/lbs) (N-N) |
|---|---|---|---|
| 0 mm |
0.96 kg / 2.11 pounds
3 498 Gs
|
0.14 kg / 0.32 pounds
144 g / 1.4 N
|
N/A |
| 1 mm |
0.80 kg / 1.76 pounds
3 664 Gs
|
0.12 kg / 0.26 pounds
119 g / 1.2 N
|
0.72 kg / 1.58 pounds
~0 Gs
|
| 2 mm |
0.60 kg / 1.33 pounds
3 192 Gs
|
0.09 kg / 0.20 pounds
91 g / 0.9 N
|
0.54 kg / 1.20 pounds
~0 Gs
|
| 3 mm |
0.43 kg / 0.95 pounds
2 689 Gs
|
0.06 kg / 0.14 pounds
64 g / 0.6 N
|
0.39 kg / 0.85 pounds
~0 Gs
|
| 5 mm |
0.19 kg / 0.42 pounds
1 801 Gs
|
0.03 kg / 0.06 pounds
29 g / 0.3 N
|
0.17 kg / 0.38 pounds
~0 Gs
|
| 10 mm |
0.02 kg / 0.05 pounds
640 Gs
|
0.00 kg / 0.01 pounds
4 g / 0.0 N
|
0.02 kg / 0.05 pounds
~0 Gs
|
| 20 mm |
0.00 kg / 0.00 pounds
132 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
11 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
6 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
4 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
3 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
2 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
1 Gs
|
0.00 kg / 0.00 pounds
0 g / 0.0 N
|
0.00 kg / 0.00 pounds
~0 Gs
|
Table 7: Axial field levels — not safety zones
MW 7x1.2 / N38
| Field level (Gs) | mT | Model distance (cm) |
|---|---|---|
| < 5 Gs | < 0.5 mT | 3.0 cm |
| < 10 Gs | < 1.0 mT | 2.5 cm |
| < 20 Gs | < 2.0 mT | 2.0 cm |
| < 40 Gs | < 4.0 mT | 1.5 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
MW 7x1.2 / N38
| Start from (mm) | Speed (km/h) | Energy (J) | Predicted outcome |
|---|---|---|---|
| 10 mm |
24.25 km/h
(6.73 m/s)
|
0.01 J | |
| 30 mm |
24.26 km/h
(6.74 m/s)
|
0.01 J | |
| 50 mm |
24.26 km/h
(6.74 m/s)
|
0.01 J | |
| 100 mm |
24.27 km/h
(6.74 m/s)
|
0.01 J |
Table 9: Coating parameters (durability)
MW 7x1.2 / 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)
MW 7x1.2 / N38
| Parameter | Value | SI Unit / Description |
|---|---|---|
| Magnetic Flux | 925 Mx | 9.3 µWb |
| Pc Coefficient | 0.25 | Low (Flat) |
Table 11: Underwater work (magnet fishing)
MW 7x1.2 / N38
| Environment | Effective steel pull | Effect |
|---|---|---|
| Air (land) | 0.49 kg | Standard |
| Water (riverbed) |
0.56 kg
(+0.07 kg buoyancy gain)
|
+14.5% |
1. Vertical hold
*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 weakens 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) = 0.25
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% |
Ecology and recycling (GPSR)
| recyclability (EoL) | 100% |
| recycled raw materials | ~10% (pre-cons) |
| carbon footprint | low / zredukowany |
| waste code (EWC) | 16 02 16 |
Other products
Advantages and disadvantages of neodymium magnets.
Strengths
- Their strength is durable, and after approximately ten years it decreases only by ~1% (theoretically),
- Neodymium magnets prove to be highly resistant to loss of magnetic properties caused by external interference,
- In other words, due to the shiny layer of silver, the element looks attractive,
- Magnetic induction on the working part of the magnet remains strong,
- Thanks to resistance to high temperature, they can operate (depending on the form) even at temperatures up to 230°C and higher...
- Thanks to versatility in constructing and the ability to adapt to client solutions,
- Key role in electronics industry – they are used in HDD drives, motor assemblies, advanced medical instruments, also other advanced devices.
- Relatively small size with high pulling force – neodymium magnets offer high power in tiny dimensions, which makes them useful in compact constructions
Cons
- At very strong impacts they can crack, therefore we advise placing them in special holders. 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.
- Magnets exposed to a humid environment can corrode. Therefore while using outdoors, we suggest using water-impermeable magnets made of rubber, plastic or other material protecting against moisture
- Due to limitations in realizing threads and complicated shapes in magnets, we propose using casing - magnetic holder.
- Possible danger resulting from small fragments of magnets can be dangerous, when accidentally swallowed, which becomes key in the context of child safety. It is also worth noting that small components of these magnets are able to be problematic in diagnostics medical when they are in the body.
- With large orders the cost of neodymium magnets is economically unviable,
Lifting parameters
Highest magnetic holding force – what it depends on?
- on a plate made of structural steel, perfectly concentrating the magnetic field
- possessing a thickness of at least 10 mm to avoid saturation
- characterized by smoothness
- without the slightest air gap between the magnet and steel
- for force applied at a right angle (pull-off, not shear)
- at standard ambient temperature
Key elements affecting lifting force
- Gap between surfaces – every millimeter of distance (caused e.g. by veneer or dirt) significantly weakens the magnet efficiency, often by half at just 0.5 mm.
- Angle of force application – highest force is available only during perpendicular pulling. The shear force of the magnet along the surface is usually many times lower (approx. 1/5 of the lifting capacity).
- Substrate thickness – for full efficiency, the steel must be sufficiently thick. Paper-thin metal restricts the lifting capacity (the magnet "punches through" it).
- Material type – the best choice is high-permeability steel. Stainless steels may have worse magnetic properties.
- Surface structure – the smoother and more polished the surface, the larger the contact zone and higher the lifting capacity. Roughness creates an air distance.
- Temperature – temperature increase results in weakening of induction. It is worth remembering the thermal limit for a given model.
Holding force was measured on a smooth steel plate of 20 mm thickness, when a perpendicular force was applied, in contrast under parallel forces the lifting capacity is smaller. Moreover, even a slight gap between the magnet’s surface and the plate decreases the holding force.
Safety rules for work with neodymium magnets
ICD Warning
People with a heart stimulator should keep an absolute distance from magnets. The magnetic field can disrupt the operation of the implant.
Compass and GPS
Remember: rare earth magnets generate a field that confuses precision electronics. Maintain a safe distance from your mobile, tablet, and navigation systems.
Keep away from computers
Equipment safety: Strong magnets can damage data carriers and sensitive devices (pacemakers, medical aids, timepieces).
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.
Product not for children
Always keep magnets away from children. Ingestion danger is high, and the consequences of magnets clamping inside the body are fatal.
Material brittleness
Beware of splinters. Magnets can fracture upon violent connection, launching shards into the air. Eye protection is mandatory.
Serious injuries
Pinching hazard: The attraction force is so immense that it can cause blood blisters, pinching, and even bone fractures. Protective gloves are recommended.
Dust is flammable
Dust produced during cutting of magnets is combustible. Avoid drilling into magnets unless you are an expert.
Sensitization to coating
Studies show that nickel (the usual finish) is a strong allergen. If your skin reacts to metals, prevent direct skin contact or select encased magnets.
Handling guide
Be careful. Neodymium magnets act from a distance and connect with huge force, often quicker than you can move away.
