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| Hauptseite > Publikationsdatenbank > On the Fractal Dimension of Rough Surfaces > print |
| 001 | 201510 | ||
| 005 | 20210129215812.0 | ||
| 024 | 7 | _ | |a 10.1007/s11249-014-0313-4 |2 doi |
| 024 | 7 | _ | |a 1023-8883 |2 ISSN |
| 024 | 7 | _ | |a 1573-2711 |2 ISSN |
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| 037 | _ | _ | |a FZJ-2015-03805 |
| 041 | _ | _ | |a English |
| 082 | _ | _ | |a 670 |
| 100 | 1 | _ | |a Persson, Bo |0 P:(DE-Juel1)130885 |b 0 |e Corresponding Author |
| 245 | _ | _ | |a On the Fractal Dimension of Rough Surfaces |
| 260 | _ | _ | |a Basel |c 2014 |b Baltzer |
| 336 | 7 | _ | |a Journal Article |b journal |m journal |0 PUB:(DE-HGF)16 |s 1435238638_9505 |2 PUB:(DE-HGF) |
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| 336 | 7 | _ | |a article |2 DRIVER |
| 520 | _ | _ | |a Most natural surfaces and surfaces of engineering interest, e.g., polished or sandblasted surfaces, are self-affine fractal over a wide range of length scales, with the fractal dimension Df=2.15±0.15. We give several examples illustrating this and a simple argument, based on surface fragility, for why the fractal dimension usually is <2.3. A kinetic model of sandblasting is presented, which gives surface topographies and surface roughness power spectra in good agreement with experiments. |
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| 773 | _ | _ | |a 10.1007/s11249-014-0313-4 |g Vol. 54, no. 1, p. 99 - 106 |0 PERI:(DE-600)2015908-0 |n 1 |p 99 - 106 |t Tribology letters |v 54 |y 2014 |x 1573-2711 |
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