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blends","created_at":"2022-01-31T00:19:52.366-08:00","url":"https://www.academia.edu/70113346/Influence_of_phase_miscibility_and_morphology_on_crack_resistance_behaviour_and_kinetics_of_crack_propagation_of_nanostructured_binary_styrene_styrene_butadiene_styrene_triblock_copolymer_blends?f_ri=792388","dom_id":"work_70113346","summary":null,"downloadable_attachments":[{"id":79978324,"asset_id":70113346,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":60472152,"first_name":"Konrad","last_name":"Knoll","domain_name":"independent","page_name":"KonradKnoll","display_name":"Konrad Knoll","profile_url":"https://independent.academia.edu/KonradKnoll?f_ri=792388","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":56,"name":"Materials Engineering","url":"https://www.academia.edu/Documents/in/Materials_Engineering?f_ri=792388","nofollow":false},{"id":60,"name":"Mechanical 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Mechanism","url":"https://www.academia.edu/Documents/in/Deformation_Mechanism?f_ri=792388"},{"id":1295917,"name":"Block Copolymers","url":"https://www.academia.edu/Documents/in/Block_Copolymers?f_ri=792388"},{"id":1431635,"name":"Dynamic Mechanical Analysis","url":"https://www.academia.edu/Documents/in/Dynamic_Mechanical_Analysis?f_ri=792388"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_12213699" data-work_id="12213699" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/12213699/Cavitation_Erosion_Behavior_of_HPDL_Treated_TWAS_Coated_Ti6Al4V_Alloy_and_Its_Similarity_with_Water_Droplet_Erosion">Cavitation Erosion Behavior of HPDL-Treated TWAS-Coated Ti6Al4V Alloy and Its Similarity with Water Droplet Erosion</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Twin wire arc-sprayed (TWAS) coating of commercially available SHS 7170-cored wire was obtained on Ti6AL4V alloy, and to improve its properties, it was further surface treated with high-power diode laser (HPDL). The cavitation erosion... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_12213699" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Twin wire arc-sprayed (TWAS) coating of commercially available SHS 7170-cored wire was obtained on Ti6AL4V alloy, and to improve its properties, it was further surface treated with high-power diode laser (HPDL). The cavitation erosion (CE) resistance of TWAS-coated samples was evaluated as per ASTM G-32-2003 and it was compared with laser-treated and untreated Ti6Al4V alloys. The CE resistance of TWAS-coated</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/12213699" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="7eb501d96f81627213db9946bb5c0cdd" rel="nofollow" data-download="{"attachment_id":46298816,"asset_id":12213699,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/46298816/download_file?st=MTczMzI2MjQ2MCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="30690108" href="https://independent.academia.edu/VivekArya6">Vivek Arya</a><script data-card-contents-for-user="30690108" type="text/json">{"id":30690108,"first_name":"Vivek","last_name":"Arya","domain_name":"independent","page_name":"VivekArya6","display_name":"Vivek Arya","profile_url":"https://independent.academia.edu/VivekArya6?f_ri=792388","photo":"https://0.academia-photos.com/30690108/8940425/9977131/s65_vivek.arya.jpg"}</script></span></span></li><li class="js-paper-rank-work_12213699 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="12213699"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 12213699, container: ".js-paper-rank-work_12213699", }); 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The cavitation erosion (CE) resistance of TWAS-coated samples was evaluated as per ASTM G-32-2003 and it was compared with laser-treated and untreated Ti6Al4V alloys. The CE resistance of TWAS-coated","downloadable_attachments":[{"id":46298816,"asset_id":12213699,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":30690108,"first_name":"Vivek","last_name":"Arya","domain_name":"independent","page_name":"VivekArya6","display_name":"Vivek Arya","profile_url":"https://independent.academia.edu/VivekArya6?f_ri=792388","photo":"https://0.academia-photos.com/30690108/8940425/9977131/s65_vivek.arya.jpg"}],"research_interests":[{"id":56,"name":"Materials Engineering","url":"https://www.academia.edu/Documents/in/Materials_Engineering?f_ri=792388","nofollow":false},{"id":591063,"name":"Diode Laser","url":"https://www.academia.edu/Documents/in/Diode_Laser?f_ri=792388","nofollow":false},{"id":792388,"name":"Fracture Toughness","url":"https://www.academia.edu/Documents/in/Fracture_Toughness?f_ri=792388","nofollow":false}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div 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Materials</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">A detailed analytical and experimental investigation is presented to understand the dynamic fracture behavior of functionally graded materials (FGMs) under mode I and mixed mode loading conditions. Crack-tip stress, strain and... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_4985945" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">A detailed analytical and experimental investigation is presented to understand the dynamic fracture behavior of functionally graded materials (FGMs) under mode I and mixed mode loading conditions. Crack-tip stress, strain and displacement fields for a mixed mode crack propagating at an angle from the direction of property gradation were obtained through an asymptotic analysis coupled with a displacement potential approach. This was followed by a comprehensive series of experiments to gain further insight into the behavior of propagating cracks in FGMs. Dynamic photoelasticity coupled with high-speed photography was used to obtain crack tip velocities and dynamic stress fields around the propagating cracks. Birefringent coatings were used to conduct the photoelastic study due to the opaqueness of the FGMs. Dynamic fracture experiments were performed using different specimen geometries to develop a dynamic constitutive fracture relationship between the mode I dynamic stress intensity factor (K ID ) and crack-tip velocity ( ${\mathop a\limits^ \cdot }$ ) for FGMs with the crack moving in the direction of increasing fracture toughness. A similar ${\mathop a\limits^ \cdot }$ -K ID relation was also obtained for matrix material (polyester) for comparison purposes. The results obtained show that crack propagation velocities in FGMs were about 80% higher than the polyester matrix. Crack arrest toughness was found to be about 10% lower than the value of local fracture toughness in FGMs.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/4985945" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="90998c6bd0ddaaae155532d61ec5174a" rel="nofollow" data-download="{"attachment_id":49499151,"asset_id":4985945,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/49499151/download_file?st=MTczMzI2MjQ2MCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="6592252" href="https://independent.academia.edu/NiteshJain2">Nitesh Jain</a><script data-card-contents-for-user="6592252" type="text/json">{"id":6592252,"first_name":"Nitesh","last_name":"Jain","domain_name":"independent","page_name":"NiteshJain2","display_name":"Nitesh Jain","profile_url":"https://independent.academia.edu/NiteshJain2?f_ri=792388","photo":"/images/s65_no_pic.png"}</script></span></span></li><li class="js-paper-rank-work_4985945 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="4985945"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 4985945, container: ".js-paper-rank-work_4985945", }); 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Crack-tip stress, strain and displacement fields for a mixed mode crack propagating at an angle from the direction of property gradation were obtained through an asymptotic analysis coupled with a displacement potential approach. This was followed by a comprehensive series of experiments to gain further insight into the behavior of propagating cracks in FGMs. Dynamic photoelasticity coupled with high-speed photography was used to obtain crack tip velocities and dynamic stress fields around the propagating cracks. Birefringent coatings were used to conduct the photoelastic study due to the opaqueness of the FGMs. Dynamic fracture experiments were performed using different specimen geometries to develop a dynamic constitutive fracture relationship between the mode I dynamic stress intensity factor (K ID ) and crack-tip velocity ( ${\\mathop a\\limits^ \\cdot }$ ) for FGMs with the crack moving in the direction of increasing fracture toughness. A similar ${\\mathop a\\limits^ \\cdot }$ -K ID relation was also obtained for matrix material (polyester) for comparison purposes. The results obtained show that crack propagation velocities in FGMs were about 80% higher than the polyester matrix. Crack arrest toughness was found to be about 10% lower than the value of local fracture toughness in FGMs.","downloadable_attachments":[{"id":49499151,"asset_id":4985945,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":6592252,"first_name":"Nitesh","last_name":"Jain","domain_name":"independent","page_name":"NiteshJain2","display_name":"Nitesh Jain","profile_url":"https://independent.academia.edu/NiteshJain2?f_ri=792388","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":60,"name":"Mechanical Engineering","url":"https://www.academia.edu/Documents/in/Mechanical_Engineering?f_ri=792388","nofollow":false},{"id":73,"name":"Civil Engineering","url":"https://www.academia.edu/Documents/in/Civil_Engineering?f_ri=792388","nofollow":false},{"id":9732,"name":"Experimental Mechanics","url":"https://www.academia.edu/Documents/in/Experimental_Mechanics?f_ri=792388","nofollow":false},{"id":17038,"name":"Stress 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work_11196158" data-work_id="11196158" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/11196158/Characterisation_by_means_of_a_finite_element_model_of_the_influence_of_moisture_content_on_the_mechanical_and_fracture_properties_of_the_polyamide_6_reinforced_with_short_glass_fibre">Characterisation by means of a finite element model of the influence of moisture content on the mechanical and fracture properties of the polyamide 6 reinforced with short glass fibre</a></div></div><div class="u-pb4x u-mt3x"></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/11196158" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i 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type="text/json">{"id":4496,"name":"Composites","url":"https://www.academia.edu/Documents/in/Composites?f_ri=792388","nofollow":false}</script><a class="InlineList-item-text" data-has-card-for-ri="6177" href="https://www.academia.edu/Documents/in/Modeling">Modeling</a>, <script data-card-contents-for-ri="6177" type="text/json">{"id":6177,"name":"Modeling","url":"https://www.academia.edu/Documents/in/Modeling?f_ri=792388","nofollow":false}</script><a class="InlineList-item-text" data-has-card-for-ri="166454" href="https://www.academia.edu/Documents/in/Delamination">Delamination</a><script data-card-contents-for-ri="166454" type="text/json">{"id":166454,"name":"Delamination","url":"https://www.academia.edu/Documents/in/Delamination?f_ri=792388","nofollow":false}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=30776494]'), work: {"id":30776494,"title":"Facesheet delamination of composite sandwich materials at 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Mechanical Properties and Fracture Mechanisms</a></div></div><div class="u-pb4x u-mt3x"></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/30489848" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="68ca509332614e5f81bde91170715169" rel="nofollow" data-download="{"attachment_id":50928612,"asset_id":30489848,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" 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class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_8504351" data-work_id="8504351" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/8504351/Correlation_between_fracture_toughness_and_microstructure_of_seeded_silicon_nitride_ceramics">Correlation between fracture toughness and microstructure of seeded silicon nitride ceramics</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Microstructure development and fracture toughness of Si3N4 composites were studied in the presence of seeds and Al2O3 + Y2O3 as sintering aids. The elongated β-Si3N4 seeds were introduced into two different α-Si3N4 matrix powders; one was... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_8504351" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Microstructure development and fracture toughness of Si3N4 composites were studied in the presence of seeds and Al2O3 + Y2O3 as sintering aids. The elongated β-Si3N4 seeds were introduced into two different α-Si3N4 matrix powders; one was the ultra fine powder matrix and the other was the coarse powder matrix. The amount of seeds varied from 0 to 6 wt%. The grain growth inhibition and the mechanism of toughening were discussed and correlated with microstructure. The maximum fracture toughness of 9.0 MPa m1/2 was obtained for ultra fine powder with 5 wt% seeds hot pressed at 1,700 °C for 6 h.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/8504351" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="de7e4d1ba9da9628e88a91627aa436af" rel="nofollow" data-download="{"attachment_id":48073798,"asset_id":8504351,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/48073798/download_file?st=MTczMzI2MjQ2MCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="17406698" href="https://independent.academia.edu/DusanBucevac">Dusan Bucevac</a><script data-card-contents-for-user="17406698" type="text/json">{"id":17406698,"first_name":"Dusan","last_name":"Bucevac","domain_name":"independent","page_name":"DusanBucevac","display_name":"Dusan Bucevac","profile_url":"https://independent.academia.edu/DusanBucevac?f_ri=792388","photo":"https://0.academia-photos.com/17406698/4830722/5560503/s65_dusan.bucevac.jpg_oh_d866f38ac4a98a78f6c2598ae5081a2c_oe_54d030d0___gda___1418492900_5f1b6acb8ee7e21c34b891e37409c1fb"}</script></span></span></li><li class="js-paper-rank-work_8504351 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="8504351"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 8504351, container: ".js-paper-rank-work_8504351", }); 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u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_21299865" data-work_id="21299865" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/21299865/THE_EFFECT_OF_LOADING_RATE_AND_DIRECTION_OF_FORMATION_ON_FRACTURE_TOUGHNESS_OF_RIGID_POLYURETHANE_FOAMS">THE EFFECT OF LOADING RATE AND DIRECTION OF FORMATION ON FRACTURE TOUGHNESS OF RIGID POLYURETHANE FOAMS</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">This paper presents the effect of loading rate, (ELR), and direction of formation, (DF), of rigid polyurethane foams, (PUR 40 and PUR 140), on fracture toughness. Nominal densities of used foams in the experimental program were 140 kg/m 3... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_21299865" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">This paper presents the effect of loading rate, (ELR), and direction of formation, (DF), of rigid polyurethane foams, (PUR 40 and PUR 140), on fracture toughness. Nominal densities of used foams in the experimental program were 140 kg/m 3 , (for ELS) and 40 kg/m 3 , (for DF), which is closed-cell rigid foams widely used for sandwich cores. Determination of fracture toughness for Mode I fracture of studied materials has made by three-point bending tests, (3PB), on specimens with notches, at room temperature (20 ± 2 ºC). All the specimens were cut from one and the same plate. The specimens were subjected to 3PB at a loading speed of 2 mm/min, except samples for determining the ELR where 2, 20, 200 and 400 mm/min loading speeds were used, and were taken into account the fact that the load must act exactly on the notch direction. All the specimens present brittle failure without plastic deformation.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/21299865" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="e5284e47f761b15cc1538a68e4cb3b14" rel="nofollow" data-download="{"attachment_id":41805730,"asset_id":21299865,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/41805730/download_file?st=MTczMzI2MjQ2MCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="5014397" href="https://upt.academia.edu/EmanoilLinul">Emanoil LINUL</a><script data-card-contents-for-user="5014397" type="text/json">{"id":5014397,"first_name":"Emanoil","last_name":"LINUL","domain_name":"upt","page_name":"EmanoilLinul","display_name":"Emanoil LINUL","profile_url":"https://upt.academia.edu/EmanoilLinul?f_ri=792388","photo":"https://0.academia-photos.com/5014397/2177840/3999225/s65_emanoil.linul.jpg"}</script></span></span></li><li class="js-paper-rank-work_21299865 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="21299865"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 21299865, container: ".js-paper-rank-work_21299865", }); 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Nominal densities of used foams in the experimental program were 140 kg/m 3 , (for ELS) and 40 kg/m 3 , (for DF), which is closed-cell rigid foams widely used for sandwich cores. Determination of fracture toughness for Mode I fracture of studied materials has made by three-point bending tests, (3PB), on specimens with notches, at room temperature (20 ± 2 ºC). All the specimens were cut from one and the same plate. The specimens were subjected to 3PB at a loading speed of 2 mm/min, except samples for determining the ELR where 2, 20, 200 and 400 mm/min loading speeds were used, and were taken into account the fact that the load must act exactly on the notch direction. All the specimens present brittle failure without plastic deformation.","downloadable_attachments":[{"id":41805730,"asset_id":21299865,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":5014397,"first_name":"Emanoil","last_name":"LINUL","domain_name":"upt","page_name":"EmanoilLinul","display_name":"Emanoil LINUL","profile_url":"https://upt.academia.edu/EmanoilLinul?f_ri=792388","photo":"https://0.academia-photos.com/5014397/2177840/3999225/s65_emanoil.linul.jpg"}],"research_interests":[{"id":37333,"name":"Anisotropy","url":"https://www.academia.edu/Documents/in/Anisotropy?f_ri=792388","nofollow":false},{"id":243700,"name":"Cellular Materials","url":"https://www.academia.edu/Documents/in/Cellular_Materials?f_ri=792388","nofollow":false},{"id":792388,"name":"Fracture Toughness","url":"https://www.academia.edu/Documents/in/Fracture_Toughness?f_ri=792388","nofollow":false},{"id":952555,"name":"SEM 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href="https://www.academia.edu/8356386/Preparation_and_Investigation_on_Properties_of_Cryogenically_Solidified_Nano_Metal_Matrix_Composites">Preparation and Investigation on Properties of Cryogenically Solidified Nano Metal Matrix Composites</a></div></div><div class="u-pb4x u-mt3x"></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/8356386" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="41ab4c06482a35a941f482fb727fe7e8" rel="nofollow" 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class="u-tcGray u-textDecorationNone u-linkUnstyled u-fw500 hidden" data-unfollow-ri-id="239252">Following</a></div></li></ul></div></div></div></div></div></div><script>// MIT License // Copyright © 2011 Sebastian Tschan, https://blueimp.net // Permission is hereby granted, free of charge, to any person obtaining a copy of // this software and associated documentation files (the "Software"), to deal in // the Software without restriction, including without limitation the rights to // use, copy, modify, merge, publish, distribute, sublicense, and/or sell copies of // the Software, and to permit persons to whom the Software is furnished to do so, // subject to the following conditions: // The above copyright notice and this permission notice shall be included in all // copies or substantial portions of the Software. // THE SOFTWARE IS PROVIDED "AS IS", WITHOUT WARRANTY OF ANY KIND, EXPRESS OR // IMPLIED, INCLUDING BUT NOT LIMITED TO THE WARRANTIES OF MERCHANTABILITY, FITNESS // FOR A 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