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Additionally, volumetric flow rates and shear rates were monitored by counting the stepper motor pulses as well as the pulses from a custom filament encoder to account for filament slippage and skipped motor steps. The incorporation of the sensors and the design and development of the in-line rheometer are described; and pressures, temperatures, and viscosities within the 3D printing nozzle are presented. The in-line rheometer was validated against traditional, off-line rotational rheology and capillary rheology measurements by analyzing two polymeric materials: polycarbonate and high-impact polystyrene. A variety of rheological corrections were considered for the in-line rheometer, including entrance effects, non-Newtonian corrections, shear heating, pressure effects, and temperature fluctuations\u002Finaccuracies. Excellent agreement was obtained between the in-line and off-line rheometers after applying the most critical corrections, which were found to be entrance effects, non-Newtonian corrections, and temperature inaccuracies. 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Rheol., 16, 383, 10.1122\u002F1.549257",{"doi":1273},"10.1122\u002F1.549257",{"id":24,"text":1275,"url":24,"identifiers":1276},"1997, Extensional viscosity from entrance pressure drop measurements, Rheol. Acta, 36, 144, 10.1007\u002FBF00366820",{"doi":1277},"10.1007\u002FBF00366820",{"id":24,"text":1279,"url":24,"identifiers":1280},"1988, An approximate analysis for contraction and converging flows, J. Non-Newtonian Fluid Mech., 27, 173, 10.1016\u002F0377-0257(88)85012-2",{"doi":1281},"10.1016\u002F0377-0257(88)85012-2",{"id":24,"text":1283,"url":24,"identifiers":1284},"See supplementary material at https:\u002F\u002Fdoi.org\u002F10.1122\u002F1.5054648  for additional details regarding the design of the in-line rheometer components, validation of the volumetric flow rates calculated by the pulses from the stepper motor and encoder, additional equations and analysis for calculating entrance pressure effects, and the shear heating analysis in the FDMRheo. The final, corrected viscosities are tabulated to compare the values from the three rheometers. The raw data of the equilibrated pressures, shear rates, viscosities, etc. are also tabulated in the supplementary material. Supplementary raw data, including the transient pressure, voltage, shear stress, shear rate, viscosity, and temperature, are provided in individual raw data files: HIPS 225C 1_72mmL, HIPS 250C 1_72mmL, HIPS 275C 1_72mmL, PC 250C 1_72mmL, PC 270C 1_72mmL, and PC 290C 1_72mmL. Note that these files are only for one of the two tests at each condition for the 1.72 mm length nozzle tip; the raw data provided contain data every 8 ms (data were collected every 4 ms) to reduce file sizes. Two sets of time data are included in each raw data file; “Time” refers to the time for the pressure, voltage, shear stress, shear rate, and viscosity data, while “Temp Time” refers to the time for the nozzle temperature data, which is collected at a slower rate.",{},{"id":1286,"createTime":1287,"updateTime":1287,"relativeEntities":1288,"slug":1289,"properties":1290,"entityType":144,"verifyStatus":145,"verifyTime":1287,"verifyNote":146,"syncStatus":23,"languages":1300,"translateLanguages":24,"viewCount":25,"primaryUrl":1301,"fullTextUrl":24,"authors":1302,"publicationType":173,"publisherRelationship":1399,"citationCount":1431,"citationInfo":1432,"publishDate":1437,"publishYear":1438,"citationAnalyzeStatus":23,"lastCitationAnalyze":24,"indexDatabases":24,"openAccess":24,"references":1439,"isForceReanalyzing":417},"e5ace88b-5341-44e1-a5c7-7c22f0c8aba3","2024-09-29T23:42:26.486+00:00",[],"The-performance-of-the-hot-end-in-a-plasticating-3D-printer",{"mag":1291,"keywords":1293,"openalex":1294,"abstract":1296,"title":1297,"doi":1299},{"VOID":1292},"2580950121",{},{"VOID":1295},"W2580950121",{},{"EN":1298},"The performance of the hot end in a plasticating 3D printer",{"VOID":1219},[148],"https:\u002F\u002Fpubs.aip.org\u002Fsor\u002Fjor\u002Farticle\u002F61\u002F2\u002F229-236\u002F241222",[1303,1325,1340,1360,1377],{"id":1304,"sortIndex":210,"researcher":24,"roles":1305,"affiliations":1306,"properties":1318},"fe0f36ec-c18d-4d7f-bd30-df17f3828642",[],[1307],{"id":1308,"sortIndex":25,"affiliation":1309,"properties":24},"a2cf31eb-1aee-481d-b6e1-20589be14606",{"id":1310,"createTime":1311,"updateTime":1312,"relativeEntities":1313,"slug":1314,"properties":1315,"entityType":69,"verifyStatus":23,"verifyTime":24,"verifyNote":24,"syncStatus":23,"languages":24,"translateLanguages":24,"viewCount":25},"f913a796-a962-4714-a691-f34bfdb36da8","2024-09-29T23:42:26.506+00:00","2024-10-06T21:02:37.739+00:00",[],"Department-of-Materials-Science-and-Engineering-University-of-Delaware-Newark-Delaware-19716",{"title":1316},{"EN":1317},"Department of Materials Science and Engineering, University of Delaware, Newark, Delaware 19716",{"openalex":1319,"orcid":1321,"title":1323},{"VOID":1320},"A5088655944",{"VOID":1322},"https:\u002F\u002Forcid.org\u002F0000-0003-2869-705X",{"EN":1324},"Zachary R. 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Rosen , and B. Stucker , Additive Manufacture Technologies: Rapid Prototyping to Direct Digital Manufacturing ( Springer, New York, 2010).",{"doi":1443},"10.1007\u002F978-1-4419-1120-9",{"id":24,"text":1223,"url":24,"identifiers":1445},{"doi":1223},{"id":24,"text":1447,"url":24,"identifiers":1448},"Yardimci, M. , T. Hattori , S. Guceri , and S. Danforth , in Solid Freeform Fabrication Proceedings, edited by D. Bourell , J. Beaman , R. Crawford , H. Marcus , and J. Barlow ( University of Texas, Austin, TX, 1997), pp. 689–698.",{},{"id":24,"text":1155,"url":24,"identifiers":1450},{"doi":1155},{"id":24,"text":1151,"url":24,"identifiers":1452},{"doi":1151},{"id":24,"text":1454,"url":24,"identifiers":1455},"Cox, W. P. , and E. H. Merz , “ Correlation of dynamic and steady flow viscosities,” J. Polym. Sci. 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Melt pressures are observed to increase when printing parts with small layer heights, which is attributed to the confined space created between the nozzle and the previous layer (i.e., an exit pressure). These exit pressures (referred to as contact pressure) and the resulting interlayer contact areas are analyzed for 2863 layers created at 21 different processing conditions. The measured contact pressure was found to directly influence the shape of the layers and the resulting interlayer contact. An intimate contact model based on contact pressure is combined with a wetting model to accurately predict the interlayer contact of FFF parts. This pressure-driven intimate contact model for FFF shows strong agreement with the observed interlayer contact. No theoretical model has previously existed for predicting interlayer contact, so this research provides a critical component for developing a comprehensive part strength model. Both the measurements and proposed model are sufficiently simple and accurate for real-time analysis of FFF quality, so the described in-line sensors provide valuable quality insights and are recommended for future researchers, printer manufacturers, and end-users.\u003C\u002Fjats:p>",{"EN":1490},"Modeling of interlayer contact and contact pressure during fused filament fabrication",{"VOID":1492},"10.1122\u002F1.5093033",[148],"https:\u002F\u002Fpubs.aip.org\u002Fjor\u002Farticle\u002F63\u002F4\u002F655\u002F923475\u002FModeling-of-interlayer-contact-and-contact",[1496,1516],{"id":1497,"sortIndex":25,"researcher":24,"roles":1498,"affiliations":1499,"properties":1512},"5de0f4ef-c082-4f2c-a80a-5bef9b89e908",[],[1500,1506],{"id":1501,"sortIndex":25,"affiliation":1502,"properties":24},"b0848832-fab1-4c79-828d-fccfb7fcb760",{"id":906,"createTime":907,"updateTime":908,"relativeEntities":1503,"slug":910,"properties":1504,"entityType":69,"verifyStatus":23,"verifyTime":24,"verifyNote":24,"syncStatus":23,"languages":24,"translateLanguages":24,"viewCount":25},[],{"title":1505},{"EN":913},{"id":1507,"sortIndex":210,"affiliation":1508,"properties":24},"b426d541-01d0-4b57-8091-058aee07bd31",{"id":917,"createTime":918,"updateTime":919,"relativeEntities":1509,"slug":921,"properties":1510,"entityType":69,"verifyStatus":23,"verifyTime":24,"verifyNote":24,"syncStatus":23,"languages":24,"translateLanguages":24,"viewCount":25},[],{"title":1511},{"EN":924},{"openalex":1513,"orcid":1514,"title":1515},{"VOID":927},{"VOID":929},{"EN":931},{"id":1517,"sortIndex":210,"researcher":24,"roles":1518,"affiliations":1519,"properties":1532},"26c046f9-a908-44cd-8565-6eaad0ceff50",[],[1520,1526],{"id":1521,"sortIndex":25,"affiliation":1522,"properties":24},"6ef31fe9-d016-455c-b04e-911c37c48734",{"id":939,"createTime":940,"updateTime":941,"relativeEntities":1523,"slug":943,"properties":1524,"entityType":69,"verifyStatus":23,"verifyTime":24,"verifyNote":24,"syncStatus":23,"languages":24,"translateLanguages":24,"viewCount":25},[],{"title":1525},{"EN":946},{"id":1527,"sortIndex":210,"affiliation":1528,"properties":24},"c0bb332d-4426-4e4d-ba29-1551f86cf627",{"id":906,"createTime":907,"updateTime":908,"relativeEntities":1529,"slug":910,"properties":1530,"entityType":69,"verifyStatus":23,"verifyTime":24,"verifyNote":24,"syncStatus":23,"languages":24,"translateLanguages":24,"viewCount":25},[],{"title":1531},{"EN":913},{"openalex":1533,"orcid":1534,"title":1535},{"VOID":955},{"VOID":957},{"EN":959},{"url":24,"publisher":1537,"properties":1562},{"id":6,"createTime":7,"updateTime":8,"relativeEntities":1538,"slug":10,"properties":1539,"entityType":22,"verifyStatus":23,"verifyTime":24,"verifyNote":24,"syncStatus":23,"languages":24,"translateLanguages":24,"viewCount":25,"subjectFields":1545,"manageAffiliations":1546,"indexDatabases":1547,"url":123,"thumbnailPath":24,"statistic":24,"gsStatistic":24,"type":24,"analyzePriority":24},[],{"country":1540,"issn":1541,"introduce":1542,"eissn":1543,"title":1544},{"VOID":13},{"VOID":15},{"EN":17},{"VOID":19},{"EN":21},[],[],[1548,1555],{"id":105,"indexDatabase":1549,"url":120,"indexYears":24,"academicFieldIds":1554,"indexDatabaseRanking":24},{"id":107,"createTime":108,"updateTime":109,"relativeEntities":1550,"label":1551,"description":1552,"key":116,"publicationTags":1553,"standard":24},[],{"EN":112,"VI":112},{"VI":114,"EN":115},[118,119],[122],{"id":83,"indexDatabase":1556,"url":96,"indexYears":97,"academicFieldIds":1561,"indexDatabaseRanking":103},{"id":85,"createTime":86,"updateTime":87,"relativeEntities":1557,"label":1558,"description":1559,"key":93,"publicationTags":1560,"standard":24},[],{"EN":90,"VI":90},{"EN":90,"VI":92},[95],[99,100,101,102],{"volume":1563,"pages":1564,"issue":1566},{"VOID":988},{"VOID":1565},"655-672",{"VOID":528},77,{"total":1567,"publishYear":24,"statisticByYear":1569},{"2019":210,"2020":217,"2021":1435,"2022":1570,"2023":1571,"2024":214},22,18,"2019-07-01",[1574,1577,1580,1583,1585,1588,1590,1593,1595,1598,1602,1606,1610,1613,1617,1620,1623,1625,1628,1632,1635,1639,1643,1647,1651,1654,1658,1662,1664,1668,1672,1676,1680,1684,1687,1691,1695,1697,1701,1704,1708,1710,1712,1714,1718],{"id":24,"text":1575,"url":24,"identifiers":1576},"2017, Bond and part strength in fused deposition modeling, Rapid Prototyp. 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