On the Stress Distribution of Granular Materials Conically Piled on the Ground [Translated]†

Two-directional stress cells which can measure the small normal and friction stress of granular materials on a wall were recently developed. With these cells, the stress distributions of granular materials (silica sand and millet grain) piled conically on a plate are measured and compared with the r...

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Main Authors: Takaaki Nagao, Yotaro Hatamura, Takatsugu Takeuchi, Nobuyuki Nakajima
Format: Article
Language:English
Published: Hosokawa Powder Technology Foundation 2014-06-01
Series:KONA Powder and Particle Journal
Online Access:https://www.jstage.jst.go.jp/article/kona/6/0/6_1988010/_pdf/-char/en
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spelling doaj-2556527a35be4da88894661b2ed20b892021-02-03T01:40:33ZengHosokawa Powder Technology FoundationKONA Powder and Particle Journal0288-45342187-55372014-06-0160576410.14356/kona.1988010konaOn the Stress Distribution of Granular Materials Conically Piled on the Ground [Translated]†Takaaki Nagao0Yotaro Hatamura1Takatsugu Takeuchi2Nobuyuki Nakajima3Dept. of Mechanical Engineering for Production, Faculty of Eng., University of TokyoDept. of Mechanical Engineering for Production, Faculty of Eng., University of TokyoDept. of Mechanical Engineering for Production, Faculty of Eng., University of TokyoDept. of Mechanical Engineering for Production, Faculty of Eng., University of TokyoTwo-directional stress cells which can measure the small normal and friction stress of granular materials on a wall were recently developed. With these cells, the stress distributions of granular materials (silica sand and millet grain) piled conically on a plate are measured and compared with the results of theoretical analysis. The results are as follows:1) The maximum normal stress occurs at a distance of a quarter of the outer radius of the cone of the pile, which is about (0.7∼0.8)γH, where γ is the apparent specific gravity, and H denotes the height of cone.2) The normal stress at the center is rather small, about (0.4∼0.6)γH.3) The maximum frictional stress also occurs at the same position as the maximum normal stress.4) Theoretical analysis gives a maximum normal stress of 0.5γKH(√2/K-k-√K)2/(1-kK)2 at a radius of r=H/√k(2/K-k) and a normal stress at the center of γH[1-K2(ƒ- k)(2/K-k-ƒ)/(1-kK)2]. k denotes the friction coefficient, and K denotes the friction coefficient between granular material and the surface of plate. ƒ is given by the formula (40). This agrees well with the experimental result.† This report was originally printed in J. Soc. Powder Technology, Japan, 23(12), 850-856 (1986) in Japanese, before being translated into English by KONA Editorial Committee with the permission of the editorial committee of the Soc. Powder Technology, Japan.https://www.jstage.jst.go.jp/article/kona/6/0/6_1988010/_pdf/-char/en
collection DOAJ
language English
format Article
sources DOAJ
author Takaaki Nagao
Yotaro Hatamura
Takatsugu Takeuchi
Nobuyuki Nakajima
spellingShingle Takaaki Nagao
Yotaro Hatamura
Takatsugu Takeuchi
Nobuyuki Nakajima
On the Stress Distribution of Granular Materials Conically Piled on the Ground [Translated]†
KONA Powder and Particle Journal
author_facet Takaaki Nagao
Yotaro Hatamura
Takatsugu Takeuchi
Nobuyuki Nakajima
author_sort Takaaki Nagao
title On the Stress Distribution of Granular Materials Conically Piled on the Ground [Translated]†
title_short On the Stress Distribution of Granular Materials Conically Piled on the Ground [Translated]†
title_full On the Stress Distribution of Granular Materials Conically Piled on the Ground [Translated]†
title_fullStr On the Stress Distribution of Granular Materials Conically Piled on the Ground [Translated]†
title_full_unstemmed On the Stress Distribution of Granular Materials Conically Piled on the Ground [Translated]†
title_sort on the stress distribution of granular materials conically piled on the ground [translated]†
publisher Hosokawa Powder Technology Foundation
series KONA Powder and Particle Journal
issn 0288-4534
2187-5537
publishDate 2014-06-01
description Two-directional stress cells which can measure the small normal and friction stress of granular materials on a wall were recently developed. With these cells, the stress distributions of granular materials (silica sand and millet grain) piled conically on a plate are measured and compared with the results of theoretical analysis. The results are as follows:1) The maximum normal stress occurs at a distance of a quarter of the outer radius of the cone of the pile, which is about (0.7∼0.8)γH, where γ is the apparent specific gravity, and H denotes the height of cone.2) The normal stress at the center is rather small, about (0.4∼0.6)γH.3) The maximum frictional stress also occurs at the same position as the maximum normal stress.4) Theoretical analysis gives a maximum normal stress of 0.5γKH(√2/K-k-√K)2/(1-kK)2 at a radius of r=H/√k(2/K-k) and a normal stress at the center of γH[1-K2(ƒ- k)(2/K-k-ƒ)/(1-kK)2]. k denotes the friction coefficient, and K denotes the friction coefficient between granular material and the surface of plate. ƒ is given by the formula (40). This agrees well with the experimental result.† This report was originally printed in J. Soc. Powder Technology, Japan, 23(12), 850-856 (1986) in Japanese, before being translated into English by KONA Editorial Committee with the permission of the editorial committee of the Soc. Powder Technology, Japan.
url https://www.jstage.jst.go.jp/article/kona/6/0/6_1988010/_pdf/-char/en
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