Mechanics of peeling of rubbery materials. II. Initiation and propagation of peeling
The peel strength of a joint with flexible materials bonded by an elastic adhesive was evaluated in relation to the fracture mechanism. It was found that initiation and propagation of peeling are governed by different mechanisms. Initiation (the formation of an initial crack) occurs when the maximum...
Ausführliche Beschreibung
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E-Artikel |
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Sprache: |
Englisch |
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1978 |
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Umfang: |
5 Ill. ; 1 Tab. 8 |
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Reproduktion: |
Wiley InterScience Backfile Collection 1832-2000 |
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Übergeordnetes Werk: |
in: Journal of Polymer Science: Polymer Physics Edition - New York : John Wiley & Sons, Inc., 16(1978) vom: März, Seite 407-414 |
Übergeordnetes Werk: |
volume:16 ; year:1978 ; month:03 ; pages:407-414 ; extent:8 |
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NLEJ163901686 |
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520 | |a The peel strength of a joint with flexible materials bonded by an elastic adhesive was evaluated in relation to the fracture mechanism. It was found that initiation and propagation of peeling are governed by different mechanisms. Initiation (the formation of an initial crack) occurs when the maximum stress in the adhesive layer reaches a definite value. In this case, the strength fi in a trousers-type peeling is given by 2fi = y0σb∊b, where y0 is the half-thickness of the adhesive layer, σb is the tensile strength, and ∊b is the tensile elongation of the adhesive. On the other hand, propagation is governed by the surface energy of the adhesive. In this case, the peeling strength fs is determined by a balance of energies. For trousers-type peeling it is given by 2fs = Γ, where Γ is twice the surface energy. These results were verified experimentally. | ||
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(DE-627)NLEJ163901686 DE-627 ger DE-627 rakwb eng Mechanics of peeling of rubbery materials. II. Initiation and propagation of peeling 1978 5 Ill. 1 Tab. 8 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The peel strength of a joint with flexible materials bonded by an elastic adhesive was evaluated in relation to the fracture mechanism. It was found that initiation and propagation of peeling are governed by different mechanisms. Initiation (the formation of an initial crack) occurs when the maximum stress in the adhesive layer reaches a definite value. In this case, the strength fi in a trousers-type peeling is given by 2fi = y0σb∊b, where y0 is the half-thickness of the adhesive layer, σb is the tensile strength, and ∊b is the tensile elongation of the adhesive. On the other hand, propagation is governed by the surface energy of the adhesive. In this case, the peeling strength fs is determined by a balance of energies. For trousers-type peeling it is given by 2fs = Γ, where Γ is twice the surface energy. These results were verified experimentally. Wiley InterScience Backfile Collection 1832-2000 Igarashi, Takashi oth in Journal of Polymer Science: Polymer Physics Edition New York : John Wiley & Sons, Inc. 16(1978) vom: März, Seite 407-414 (DE-627)NLEJ159071518 0098-1273 nnns volume:16 year:1978 month:03 pages:407-414 extent:8 http://dx.doi.org/10.1002/pol.1978.180160304 text/html Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-WIS GBV_NL_ARTICLE AR 16 1978 3 407-414 8 |
spelling |
(DE-627)NLEJ163901686 DE-627 ger DE-627 rakwb eng Mechanics of peeling of rubbery materials. II. Initiation and propagation of peeling 1978 5 Ill. 1 Tab. 8 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The peel strength of a joint with flexible materials bonded by an elastic adhesive was evaluated in relation to the fracture mechanism. It was found that initiation and propagation of peeling are governed by different mechanisms. Initiation (the formation of an initial crack) occurs when the maximum stress in the adhesive layer reaches a definite value. In this case, the strength fi in a trousers-type peeling is given by 2fi = y0σb∊b, where y0 is the half-thickness of the adhesive layer, σb is the tensile strength, and ∊b is the tensile elongation of the adhesive. On the other hand, propagation is governed by the surface energy of the adhesive. In this case, the peeling strength fs is determined by a balance of energies. For trousers-type peeling it is given by 2fs = Γ, where Γ is twice the surface energy. These results were verified experimentally. Wiley InterScience Backfile Collection 1832-2000 Igarashi, Takashi oth in Journal of Polymer Science: Polymer Physics Edition New York : John Wiley & Sons, Inc. 16(1978) vom: März, Seite 407-414 (DE-627)NLEJ159071518 0098-1273 nnns volume:16 year:1978 month:03 pages:407-414 extent:8 http://dx.doi.org/10.1002/pol.1978.180160304 text/html Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-WIS GBV_NL_ARTICLE AR 16 1978 3 407-414 8 |
allfields_unstemmed |
(DE-627)NLEJ163901686 DE-627 ger DE-627 rakwb eng Mechanics of peeling of rubbery materials. II. Initiation and propagation of peeling 1978 5 Ill. 1 Tab. 8 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The peel strength of a joint with flexible materials bonded by an elastic adhesive was evaluated in relation to the fracture mechanism. It was found that initiation and propagation of peeling are governed by different mechanisms. Initiation (the formation of an initial crack) occurs when the maximum stress in the adhesive layer reaches a definite value. In this case, the strength fi in a trousers-type peeling is given by 2fi = y0σb∊b, where y0 is the half-thickness of the adhesive layer, σb is the tensile strength, and ∊b is the tensile elongation of the adhesive. On the other hand, propagation is governed by the surface energy of the adhesive. In this case, the peeling strength fs is determined by a balance of energies. For trousers-type peeling it is given by 2fs = Γ, where Γ is twice the surface energy. These results were verified experimentally. Wiley InterScience Backfile Collection 1832-2000 Igarashi, Takashi oth in Journal of Polymer Science: Polymer Physics Edition New York : John Wiley & Sons, Inc. 16(1978) vom: März, Seite 407-414 (DE-627)NLEJ159071518 0098-1273 nnns volume:16 year:1978 month:03 pages:407-414 extent:8 http://dx.doi.org/10.1002/pol.1978.180160304 text/html Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-WIS GBV_NL_ARTICLE AR 16 1978 3 407-414 8 |
allfieldsGer |
(DE-627)NLEJ163901686 DE-627 ger DE-627 rakwb eng Mechanics of peeling of rubbery materials. II. Initiation and propagation of peeling 1978 5 Ill. 1 Tab. 8 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The peel strength of a joint with flexible materials bonded by an elastic adhesive was evaluated in relation to the fracture mechanism. It was found that initiation and propagation of peeling are governed by different mechanisms. Initiation (the formation of an initial crack) occurs when the maximum stress in the adhesive layer reaches a definite value. In this case, the strength fi in a trousers-type peeling is given by 2fi = y0σb∊b, where y0 is the half-thickness of the adhesive layer, σb is the tensile strength, and ∊b is the tensile elongation of the adhesive. On the other hand, propagation is governed by the surface energy of the adhesive. In this case, the peeling strength fs is determined by a balance of energies. For trousers-type peeling it is given by 2fs = Γ, where Γ is twice the surface energy. These results were verified experimentally. Wiley InterScience Backfile Collection 1832-2000 Igarashi, Takashi oth in Journal of Polymer Science: Polymer Physics Edition New York : John Wiley & Sons, Inc. 16(1978) vom: März, Seite 407-414 (DE-627)NLEJ159071518 0098-1273 nnns volume:16 year:1978 month:03 pages:407-414 extent:8 http://dx.doi.org/10.1002/pol.1978.180160304 text/html Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-WIS GBV_NL_ARTICLE AR 16 1978 3 407-414 8 |
allfieldsSound |
(DE-627)NLEJ163901686 DE-627 ger DE-627 rakwb eng Mechanics of peeling of rubbery materials. II. Initiation and propagation of peeling 1978 5 Ill. 1 Tab. 8 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The peel strength of a joint with flexible materials bonded by an elastic adhesive was evaluated in relation to the fracture mechanism. It was found that initiation and propagation of peeling are governed by different mechanisms. Initiation (the formation of an initial crack) occurs when the maximum stress in the adhesive layer reaches a definite value. In this case, the strength fi in a trousers-type peeling is given by 2fi = y0σb∊b, where y0 is the half-thickness of the adhesive layer, σb is the tensile strength, and ∊b is the tensile elongation of the adhesive. On the other hand, propagation is governed by the surface energy of the adhesive. In this case, the peeling strength fs is determined by a balance of energies. For trousers-type peeling it is given by 2fs = Γ, where Γ is twice the surface energy. These results were verified experimentally. Wiley InterScience Backfile Collection 1832-2000 Igarashi, Takashi oth in Journal of Polymer Science: Polymer Physics Edition New York : John Wiley & Sons, Inc. 16(1978) vom: März, Seite 407-414 (DE-627)NLEJ159071518 0098-1273 nnns volume:16 year:1978 month:03 pages:407-414 extent:8 http://dx.doi.org/10.1002/pol.1978.180160304 text/html Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-WIS GBV_NL_ARTICLE AR 16 1978 3 407-414 8 |
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mechanics of peeling of rubbery materials. ii. initiation and propagation of peeling |
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Mechanics of peeling of rubbery materials. II. Initiation and propagation of peeling |
abstract |
The peel strength of a joint with flexible materials bonded by an elastic adhesive was evaluated in relation to the fracture mechanism. It was found that initiation and propagation of peeling are governed by different mechanisms. Initiation (the formation of an initial crack) occurs when the maximum stress in the adhesive layer reaches a definite value. In this case, the strength fi in a trousers-type peeling is given by 2fi = y0σb∊b, where y0 is the half-thickness of the adhesive layer, σb is the tensile strength, and ∊b is the tensile elongation of the adhesive. On the other hand, propagation is governed by the surface energy of the adhesive. In this case, the peeling strength fs is determined by a balance of energies. For trousers-type peeling it is given by 2fs = Γ, where Γ is twice the surface energy. These results were verified experimentally. |
abstractGer |
The peel strength of a joint with flexible materials bonded by an elastic adhesive was evaluated in relation to the fracture mechanism. It was found that initiation and propagation of peeling are governed by different mechanisms. Initiation (the formation of an initial crack) occurs when the maximum stress in the adhesive layer reaches a definite value. In this case, the strength fi in a trousers-type peeling is given by 2fi = y0σb∊b, where y0 is the half-thickness of the adhesive layer, σb is the tensile strength, and ∊b is the tensile elongation of the adhesive. On the other hand, propagation is governed by the surface energy of the adhesive. In this case, the peeling strength fs is determined by a balance of energies. For trousers-type peeling it is given by 2fs = Γ, where Γ is twice the surface energy. These results were verified experimentally. |
abstract_unstemmed |
The peel strength of a joint with flexible materials bonded by an elastic adhesive was evaluated in relation to the fracture mechanism. It was found that initiation and propagation of peeling are governed by different mechanisms. Initiation (the formation of an initial crack) occurs when the maximum stress in the adhesive layer reaches a definite value. In this case, the strength fi in a trousers-type peeling is given by 2fi = y0σb∊b, where y0 is the half-thickness of the adhesive layer, σb is the tensile strength, and ∊b is the tensile elongation of the adhesive. On the other hand, propagation is governed by the surface energy of the adhesive. In this case, the peeling strength fs is determined by a balance of energies. For trousers-type peeling it is given by 2fs = Γ, where Γ is twice the surface energy. These results were verified experimentally. |
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Mechanics of peeling of rubbery materials. II. Initiation and propagation of peeling |
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