Relevant bibliographies by topics / N-Force

Contents

  1. Journal articles
  2. Dissertations / Theses
  3. Books
  4. Book chapters
  5. Conference papers
  6. Reports

Academic literature on the topic 'N-Force'

Author: Grafiati
Published: 4 June 2021
Last updated: 6 February 2022

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Journal articles on the topic "N-Force"

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Ma, Richard, Mark Stasiak, Xiang-Hua Deng, and Scott Rodeo. "A Preclinical Model to Study the Influence of Graft Force on the Healing of the Anterior Cruciate Ligament Graft." Journal of Knee Surgery 32, no. 05 (May 4, 2018): 441–47. http://dx.doi.org/10.1055/s-0038-1646931.

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AbstractThe purpose of this study is to establish a small animal anterior cruciate ligament (ACL) reconstruction research model where ACL graft force can be varied to create different graft force patterns with controlled knee motion. Cadaveric (n = 10) and in vivo (n = 10) rat knees underwent ACL resection followed by reconstruction using a soft tissue autograft. Five cadaveric and five in vivo knees received a nonisometric, high-force femoral graft tunnel position. Five cadaveric and five in vivo knees received a more isometric, low-force graft tunnel position. ACL graft force (N) was then recorded as the knee was ranged from extension to 90 degrees using a custom knee flexion device. Our results demonstrate that distinct ACL graft force patterns were generated for the high-force and low-force femoral graft tunnels. For high-force ACL grafts, ACL graft forces increased as the knee was flexed both in cadaveric and in vivo knees. At 90 degrees of knee flexion, high-force ACL grafts had significantly greater mean graft force when compared with baseline (cadaver: 7.76 ± 0.54 N at 90 degrees vs. 4.94 ± 0.14 N at 0 degree, p = 0.004; in vivo: 7.29 ± 0.42 N at 90 degrees vs. 4.74 ± 0.13 N at 0 degree, p = 0.007). In contrast, the graft forces for low-force ACL grafts did not change with knee flexion (cadaver: 4.94 ± 0.11 N at 90 degrees vs. 4.72 ± 0.14 N at 0 degree, p = 0.41; in vivo: 4.78 ± 0.26 N at 90 degrees vs. 4.77 ± 0.06 N at 0 degree, p = 1). Compared with nonisometric ACL grafts, the graft force for grafts placed in an isometric position had significantly lower ACL graft forces at 15, 30, 45, 60, 70, and 90 degrees in both cadaveric and in vivo knees. In conclusion, we have developed a novel ACL reconstruction model that can reproducibly produce two ACL graft force patterns. This model would permit further research on how ACL graft forces may affect subsequent graft healing, maturation, and function.
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Barnes, Josh, and Piet Hut. "A hierarchical O(N log N) force-calculation algorithm." Nature 324, no. 6096 (December 1986): 446–49. http://dx.doi.org/10.1038/324446a0.

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Martin, Bernard J., Thomas J. Armstrong, James A. Foulke, Sivakumaran Natarajan, Edward Klinenberg, Elaine Serina, and David Rempel. "Keyboard Reaction Force and Finger Flexor Electromyograms during Computer Keyboard Work." Human Factors: The Journal of the Human Factors and Ergonomics Society 38, no. 4 (December 1996): 654–64. http://dx.doi.org/10.1518/001872096778827288.

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This study examines the relationship between forearm EMGs and keyboard reaction forces in 10 people during keyboard tasks performed at a comfortable speed. A linear fit of EMG force data for each person and finger was calculated during static fingertip loading. An average r2 of .71 was observed for forces below 50% of the maximal voluntary contraction (MVC). These regressions were used to characterize EMG data in force units during the typing task. Averaged peak reaction forces measured during typing ranged from 3.33 N (thumb) to 1.84 N (little finger), with an overall average of 2.54 N, which represents about 10% MVC and 5.4 times the key switch make force (0.47 N). Individual peak or mean finger forces obtained from EMG were greater (1.2 to 3.2 times) than force measurements; hence the range of r2 for EMG force was .10 to .46. A closer correspondence between EMG and peak force was obtained using EMG averaged across all fingers. For 5 of the participants the force computed from EMG was within ±20% of the reaction force. For the other 5 participants forces were overestimated. For 9 participants the difference between EMG estimated force and the reaction force was less than 13% MVC. It is suggested that the difference between EMG and finger force partly results from the amount of muscle load not captured by the measured applied force.
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Portone, Alfredo. "Force scaling for n = 0 RWMs." Nuclear Fusion 59, no. 2 (January 9, 2019): 024002. http://dx.doi.org/10.1088/1741-4326/aaf54e.

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Figueroa, K., R. Peña, and M. M. Campos-Vallette. "Valence Force Constants of N-Benzylideneanilines." Zeitschrift für Naturforschung B 44, no. 8 (August 1, 1989): 923–27. http://dx.doi.org/10.1515/znb-1989-0811.

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Valence force constants for N-benzylideneaniline and for two p,p′-disubstituted derivatives were estimated by means of a point-charge model using CNDO data. A vibrational assignment of bands which are sensitive to the electron donor-acceptor characteristic of substituents is proposed. The conformational changes are interpreted in terms of an intramolecular energy transfer between substituents.
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Dehnen, Walter. "A Hierarchical (N) Force Calculation Algorithm." Journal of Computational Physics 179, no. 1 (June 2002): 27–42. http://dx.doi.org/10.1006/jcph.2002.7026.

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Jung, Kihyo, Byung Hwa Lee, Sang Won Seo, Doo Sang Yoon, Baekhee Lee, Duk L. Na, and Heecheon You. "Quantitative Assessment Method of Force Tracking Capabilities for Detection of Motor Intentional Disorders." Applied Sciences 11, no. 7 (April 5, 2021): 3244. http://dx.doi.org/10.3390/app11073244.

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Early detection of motor intentional disorders associated with dysfunction in the action–intention system of the brain is clinically important to provide timely intervention. This study developed a force tracking system that can record forces exerted by the index finger while tracking 5 N, 10 N, 15 N, and 20 N of target forces varying over time. The force tracking system quantified force control measures (initiation time IT; development time, DT, maintenance error, ME; termination time, TT; tracking error, TE) for the individual and overall force control phases. This study evaluated the effectiveness of the force tracking system for a normal control group (n = 12) and two patient groups diagnosed with subcortical vascular mild cognitive impairment (svMCI, n = 11) and subcortical vascular dementia (SVaD, n = 13). Patients with SVaD showed significantly worse force control capabilities in IT (0.84 s) and ME (1.71 N) than those with svMCI (0.64 s in IT, and 1.38 N in ME). Patients with svMCI had significantly worse capabilities in IT, ME, and TE (3.80 N) than the control group (0.49 s in IT, 0.78 N in ME, and 3.07 N in TE). The prevalence rates of force control capabilities lower than the 99% confidence interval of the control group ranged from 17% to 62% for the two patient groups. The force tracking system can sensitively quantify the severity of the force control deficiencies caused by dysfunction in the action–intention system of the brain.
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Nguyen, Yann, Guillaume Kazmitcheff, Daniele De Seta, Mathieu Miroir, Evelyne Ferrary, and Olivier Sterkers. "Definition of Metrics to Evaluate Cochlear Array Insertion Forces Performed with Forceps, Insertion Tool, or Motorized Tool in Temporal Bone Specimens." BioMed Research International 2014 (2014): 1–9. http://dx.doi.org/10.1155/2014/532570.

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Introduction. In order to achieve a minimal trauma to the inner ear structures during array insertion, it would be suitable to control insertion forces. The aim of this work was to compare the insertion forces of an array insertion into anatomical specimens with three different insertion techniques: with forceps, with a commercial tool, and with a motorized tool.Materials and Methods. Temporal bones have been mounted on a 6-axis force sensor to record insertion forces. Each temporal bone has been inserted, with a lateral wall electrode array, in random order, with each of the 3 techniques.Results. Forceps manual and commercial tool insertions generated multiple jerks during whole length insertion related to fits and starts. On the contrary, insertion force with the motorized tool only rose at the end of the insertion. Overall force momentum was 1.16 ± 0.505 N (mean ± SD,n=10), 1.337 ± 0.408 N (n=8), and 1.573 ± 0.764 N (n=8) for manual insertion with forceps and commercial and motorized tools, respectively.Conclusion. Considering force momentum, no difference between the three techniques was observed. Nevertheless, a more predictable force profile could be observed with the motorized tool with a smoother rise of insertion forces.
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Katsyuba, S. A., L. V. Awakumova, D. A. Pudovik, I. Kh Shakirov, and R. R. Shagidullin. "Vibrational spectra and force constants ofS-methyl-N,N-dimethyldithiocarbamate." Russian Chemical Bulletin 44, no. 6 (June 1995): 1068–71. http://dx.doi.org/10.1007/bf00707054.

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Fox, Ross J., Christopher D. Harner, Masataka Sakane, Gregory J. Carlin, and Savio L.-Y. Woo. "Determination of the In Situ Forces in the Human Posterior Cruciate Ligament Using Robotic Technology." American Journal of Sports Medicine 26, no. 3 (May 1998): 395–401. http://dx.doi.org/10.1177/03635465980260030901.

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We examined the in situ forces in the posterior cruciate ligament as well as the force distribution between its anterolateral and posteromedial bundles. Using a robotic manipulator in conjunction with a universal force-moment sensor system, we applied posterior tibial loads from 22 to 110 N to the joint at 0° to 90° of knee flexion. The magnitude of the in situ force in the posterior cruciate ligament and its bundles was significantly affected by knee flexion angle and posterior tibial loading. In situ forces in the posterior cruciate ligament ranged from 6.1 6.0 N under a 22-N posterior tibial load at 0° of knee flexion to 112.3 28.5 N under a 110-N load at 90°. The force in the posteromedial bundle reached a maximum of 67.9 31.5 N at 90° of knee flexion, and the force in the anterolateral bundle reached a maximum of 47.8 23.0 N at 60° of knee flexion under a 110-N load. No significant differences existed between the in situ forces in the two bundles at any knee flexion angle. This study provides insight into the knee flexion angle at which each bundle of the posterior cruciate ligament experiences the highest in situ forces under posterior tibial loading. This information can help guide us in more accurate graft placement, fixation, and tensioning, and serve as an assessment of graft performance.
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Dissertations / Theses on the topic "N-Force"

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Rhee, Sung Wu. "Corrections to the tra[n]sverse force for superfluid vortices /." Thesis, Connect to this title online; UW restricted, 2003. http://hdl.handle.net/1773/9671.

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Musanur, Abrar Siraj. "Development of an empirical force field and molecular dynamics simulation of N,N'-dialkylimidazolium ionic liquids." Thesis, Stellenbosch : Stellenbosch University, 2004. http://hdl.handle.net/10019.1/53737.

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Thesis (MSc)--Stellenbosch University, 2004
ENGLISH ABSTRACT: In an ongoing study an empirical force field that can correctly model N,N'- dialkylimidazolium halide ionic liquids, the Imidazolium Ionic Liquid Force Field - IILFF, was developed based on experimental data obtained from the Cambridge Structural Database (CSD) and data calculated using Gaussian98. Different conformations of the isolated cations were optimised at the Hartree-Fock level using the 6-31G(d) basis set. Structural, vibrational and partial atomic charge data of the lowest energy conformation of each cation were taken as observables during optimisation of the force field parameters. Initial parameters of the IILFF were taken from existing force fields and were optimised using the above mentioned data. The IILFF was used to minimise isolated cations as well as crystals. These results were successfully tested against isolated cations minimised using Gaussian98 and the experimental crystals. Finally, the melting process of the 1,3-dimethylimidazolium chloride crystal was studied using an NPT ensemble starting from an ordered crystal cell and increasing the simulation temperature beyond the experimental melting temperature. The IILFF was then used to calculate the potential energy of the system.
AFRIKAANSE OPSOMMING: In 'n voortgaande studie om 'n empiriese kragveld te bou wat N,N' -dialkielimidasoliumhalied ioniese vloeistowwe korrek kan modelleer is die Imidasolium Ioniese Vloeistof Kragveld (nVK) ontwikkel. Die kragveld is ontwikkel gebasseer op eksperimentele data verkry uit die Cambridge Strukturele Databasis (CSD) asook uit data vanaf Gaussian98 berekeninge. Verskillende konformasies van die geïsoleerde katione is geoptimiseer deur middel van Hartree Fock 6-31G(d) berekeninge. Strukturele data, asook vibrasies en gedeeltelike atoom ladings van die laagste energie konformasie van elke katioon is gebruik as waarneembare veranderlikes vir die bepaling van die optimale kragveld parameters. Beginwaardes vir die nVK is geneem uit bestaande kragvelde en geoptimiseer met behulp van bogenoemde data. Die IIVK is gebruik om geïsoleerde katione asook kristalle te minimiseer. Die resultate is suksesvol getoets teen geïsoleerde katione wat met behulp van Gaussian98 geminimiseer is en eksperimenteel bepaalde kristalle. Laastens is die smeltproses van die 1,3-dimetielimidasolium chloried kristal bestudeer met behulp van 'n NPT ensemble. Daar is begin by 'n geordende kristal en die simulasie temperatuur is verhoog tot meer as die eksperimentele smeltpunt. Die IIVK is dan gebruik om die potensiële energie van die sisteem te bepaal.
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Mngadi, Vela. "Development of a force field with condensed phase consistent charges for N,N' - dialkylimidazolium room temperature ionic liquids." Master's thesis, University of Cape Town, 2015. http://hdl.handle.net/11427/20001.

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Most force field models for Room temperature ionic liquids cannot properly elucidate statics and dynamics. It is in this context that we set to assess the most efficient way to model RTILs while maintaining the integrity of the liquids statics and dynamics. The development approach begins with the investigation of the effects that the linear scaling of partial atomic charges on nonpolarisable force fields from a reference potential has on the structure and dynamics of the room temperature ionic liquids (RTILs) 1-butyl-3-methylimidazolium tetraflouroborate [C4MIM][BF4] and 1-butyl-3-methylimidazolium hexaflourophosphate [C4MIM][PF6]. The results show that the three-dimensional structure of the liquid is changed ever so slighter by the linear scaling of atomic charges. While dynamic properties such as viscosity and self-diffusion coefficients were majorly affected by charge scaling. Self-diffusion coefficients that span a range of four orders of magnitude between the original model and the scaled model where the ionic charge was ±0.6 e. Viscosity estimates calculated using the Green-Kubo and the Einstein relationships revealed that the linear scaling of atomic charges results in increased mobility of the simulated liquid. Implicit inclusion of polarisation effects was investigated, Here a new charge scheme development using Quantum mechanics/Molecular mechanics (QM/MM) methods in CHARMM 35 interfaced with GAMESS-UK was propose. The atomic charges were derived from liquid phase calculations using an iterative procedure. This was carried out for individual ions and cation-anion pairs, for the analysis of charge transfer, within the liquid environment. The results obtained gave predictions of density, liquid structure and self-diffusion coefficients that were in excellent agreement with experimental data available. This method is preferable over the commonly used charge scaling methodology which is deem as an unphysical approach for the simulation of [C4MIM][BF4] and [C4MIM][PF6]. A polarisable force field based on the Drude oscillator model is presented. The model proves to be most effective for the simulation of RTILs. The force field accurately reproduced experimental results for the physicochemical properties reviewed.
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Gupta, Shelly. "A sensor based fixturing system to determine the minimum required clamping force for unte[n]ded machining operations." The Ohio State University, 1988. http://rave.ohiolink.edu/etdc/view?acc_num=osu1094830578.

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Duguet, Thomas. "Problème à N corps nucléaire et force effective dans les méthodes de champ moyen auto-cohérent." Phd thesis, Université Pierre et Marie Curie - Paris VI, 2002. http://tel.archives-ouvertes.fr/tel-00001784.

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Le travail présenté porte sur deux aspects des méthodes microscopiques variationnelles utilisées de manière extensive dans les calculs de structure nucléaire à basse énergie. La première étude se situe à l'approximation du champ moyen où la formalisation du lien entre la fonction d'onde d'un noyau pair-pair et celle du voisin pair-impair est revisitée. Afin d'en obtenir une description cohérente quelle que soit l'intensité de l'appariement dans le système, l'utilité de la formalisation de ce lien selon un processus en deux étapes est démontrée. La séparation des étapes autorise l'extraction d'effets associés à différents canaux de la force lors de l'ajout d'un nucléon dans la fonction d'onde du système. En particulier, des formules perturbatives évaluant la contribution des termes de la fonctionnelle impairs sous renversement du temps à l'énergie de séparation d'un nucléon en présence et en l'absence d'appariement sont dérivées. Des calculs auto-cohérents valident ensuite le schéma théorique ainsi que les formules d'approximation d'un point de vue quantitatif. Cette première étude se termine par une analyse approfondie de l'oscillation pair/impair des masses dans les noyaux. Le schéma développé permet à nouveau d'identifier la contribution de chacun des canaux de la force à cette observable. La nécessité d'une meilleure connaissance des termes impairs de la fonctionnelle de l'énergie pour conclure quant à la formule de différence de masses la plus apte à isoler le gap d'appariement au niveau de Fermi est identifiée. Ces termes n'étant pas sous contrôle aujourd'hui, c'est au prix d'un travail significatif sur ceux-ci qu'un ajustement précis de la force d'appariement sur l'oscillation pair/impair des masses expérimentales sera possible. La seconde étude porte sur les méthodes de calculs au-delà du champ moyen visant à inclure les corrélations associées aux mouvements de grande amplitude dans le noyaux. Leurs effets sont introduits au moyen de la GCM et de la méthode du champ moyen projeté qui se caractérisent par l'utilisation d'un mélange de fonctions de champ moyen non-orthogonales comme fonction d'essai dans le processus variationnel. Une théorie de perturbation permettant pour la première fois de fonder ces calculs sur une base diagrammatique est développée. Dans le même temps, la resommation des corrélations à deux corps autorise la définition de l'interaction effective minimale renormalisant les divergences associées au cur dur de l'interaction nucléon-nucléon libre dans ce contexte. Procédant à une approximation locale de cette interaction, la première prescription reposant sur des bases théoriques solides est proposée pour la dépendance en densité des forces effectives phénoménologiques à utiliser dans les calculs de mélange de configurations. Traitant d'une autre origine de la dépendance en densité de l'interaction, la possible renormalisation de l'effet des forces à plus de deux corps par une dépendance en la densité mixte est démontrée pour les calculs de mélange de configurations. La forme étendue de la force de Skyrme issue de ces développements formels est alors testée au moyen de calculs de mélange de configurations visant à reproduire le phénomène de coexistence de forme dans le 186Pb.
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Duguet, Thomas. "Problème à N corps nucléaire et force effective dans les méthodes du champ moyen auto-cohérent." Paris 6, 2002. https://tel.archives-ouvertes.fr/tel-00001784.

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Gupta, Shelly Bagchi Amit. "A sensor based fixturing system to determine the minimum required clamping force for unte[n]ded machining operations /." Connect to this title online, 1988. http://rave.ohiolink.edu/etdc/view?acc%5Fnum=osu1094830578.

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FONTAINE, JEAN-PIERRE, and F. FILLAUX. "Etude par diffusion inelastique des neutrons de la dynamique des protons et calcul du champ de force du n-methylacetamide." Paris 6, 1993. http://www.theses.fr/1993PA066551.

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Les spectres de diffusion inelastique des neutrons (din) de quatre des derives isotopiques du n-methylacetamide (ch#3conhch#3, cd#3conhch#3, ch#3conhcd#3, cd#3conhcd#3) ont ete enregistres a 20k dans la gamme 30-4000 cm#-#1. Les frequences des bandes din sont comparees a celles des bandes obtenues en infrarouge et en raman a basse temperature. Dans le cadre de l'approximation du champ de force harmonique, la simulation quantitative des intensites de diffusion inelastique des neutrons du proton (n)h montre que la dynamique de celui-ci est completement differente de celle generalement admise. Le modele de la liaison de valence ne permet pas de reproduire les spectres observes: la dynamique du proton est independante de celle du squelette moleculaire. Une description phenomenologique est proposee, fondee sur la description des modes (n)h en termes de modes localises. De plus, les intensites din calculees revelent que le mode d'elongation (n)h doit etre attribue a la frequence 1575 cm#-#1. Il s'agit d'une interpretation tout a fait nouvelle: les attributions precedentes, fondees sur des donnees infrarouge et raman, donnaient ce mode a la frequence 3250 cm#-#1. La dynamique du proton (n)h est associee a l'affaiblissement de la liaison n-h consequence du caractere ionique de la liaison hydrogene (n##-h#+o##'#-) et du transfert de proton. Les spectres infrarouge et raman ont ete reconsideres et une nouvelle attribution des bandes amide est proposee en termes d'echange dynamique du proton (n)h entre les formes amidique (ocnh) et imidolique ((ho)cn) du n-methylacetamide dans des chaines infinies de molecules liees par liaison hydrogene
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Briffaut-Le, Guiner Françoise. "Etude par spectrométries vibrationnelles de dérivés de la 4-nitropyridine N-oxyde à l'état fondamental et à l'état excité triplet." Châtenay-Malabry, Ecole centrale de Paris, 1992. http://www.theses.fr/1992ECAP0245.

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Ce travail a pour objet l'étude par spectrométries vibrationnelles de dérivés de la 4-nitropyridine N-oxyde à l'état fondamental et à l'état excité triplet. Cette étude prolonge celle réalisée au laboratoire au cours d'une thèse précédente sur l'état fondamental de la 4-nitropyridine N-oxyde (NPO) et a requis l'utilisation des techniques classiques de spectrométries d'absorption IR et de diffusion Raman pour les composés à l'état fondamental, ainsi que la mise en œuvre d'une technique de diffusion Raman de résonance résolue dans le temps (nanoseconde), non encore développée au laboratoire PCM, pour caractériser les états transitoires T1. Nous présentons tout d'abord une analyse vibrationnelle détaillée de la 3-methyl 4-nitropyridine N-oxyde (POM) dans l'état fondamental. L'examen des déplacements de fréquence des raies IR en solution dans différents solvants protiques ou aprotiques a permis de mettre en évidence un transfert de charge du groupement nitro vers le groupement N-oxyde (moins important) que pour NPO) lorsque ce dernier est engagé dans une liaison hydrogène avec le solvant. Nous avons affiné cette attribution par le calcul d'un champ de force de valence général simplifié de POM. Ce calcul a été mené en transférant en en couplant les champs de force déjà connus pour NPO et le groupement méthyle. Dans une dernière partie, nous avons effectué l'étude Raman de résonance résolue dans le temps de l'état triplet de NPO, NPO-d4 et de POM. L'étude des effets d'exaltation des intensités des raies diffusion nous a conduit à des informations sur la structure de l'état T1: ainsi, il apparait que, pour NPO, cet état est caractérisé par une structure plane, et, tout comme pour POM, présente un fort transfert de charge du groupement N-oxyde vers le groupement nitro, ainsi qu'un affaiblissement de la densité électronique sur le cycle. Une telle structure permet de comprendre la forte réactivité du groupement Nitro de NPO au cours de ses réactions photochimiques
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Ladenthin, Janina N. [Verfasser]. "Force-, Heat- and Electron-Induced Switching of Single Molecules on Metal Surfaces : Tautomerization of Porphycene Investigated with Scanning Probe Microscopy / Janina N. Ladenthin." Berlin : Freie Universität Berlin, 2017. http://d-nb.info/1124465294/34.

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Books on the topic "N-Force"

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New York State Task Force on Life and the Law. Do n ot resuscitate orders: The proposed legislation and report of the New York State Task Force on Life and the Law, April 1986. 2nd ed. New York, NY (33 W. 34th St., New York 10001-3071): The Task Force, 1988.

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Bryan, Daniel W. A wind-forced modeling study of the Canary Current System from 30° N to 42.5° N. Monterey, Calif: Naval Postgraduate School, 1998.

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Byrd, Martha. Kenneth N. Walker: Airpower's untempered crusader. Maxwell Air Force Base, Ala: Air University Press, 1997.

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King's County (N.B.). Regulations and ordinances made and passed by the King's County general sessions, and at present in force. [Saint John, N.B.?: s.n.], 1987.

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Davis, Richard P. Mirror hate: The convergent ideology of Northern Ireland paramilitaries, 1966-1992. Aldershot, Hants, England: Dartmouth, 1994.

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The Jack Ford story: Newfoundland's POW in Nagasaki. St. John's, NL: Creative Publishers, 2007.

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The tunnel king: The true story of Wally Floody and the great escape. Toronto: HarperTrophy Canada, 2004.

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DeMaria, Rusel, and Zach Meston. Sega Genesis Secrets, Volume 2. Rocklin, CA: Prima Publishing, 1991.

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Nintendo Strategies. Lincolnwood, IL: Publications International, Ltd., 1989.

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Super NES games secrets: For the super nintendo entertainment system. Rocklin, CA: Prima Pub., 1992.

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Book chapters on the topic "N-Force"

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Gooch, Jan W. "Force Between Two Charges n, Coulomb’s Law." In Encyclopedic Dictionary of Polymers, 321. New York, NY: Springer New York, 2011. http://dx.doi.org/10.1007/978-1-4419-6247-8_5218.

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Glielmo, Aldo, Claudio Zeni, Ádám Fekete, and Alessandro De Vita. "Building Nonparametric n-Body Force Fields Using Gaussian Process Regression." In Machine Learning Meets Quantum Physics, 67–98. Cham: Springer International Publishing, 2020. http://dx.doi.org/10.1007/978-3-030-40245-7_5.

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Ueda, T., K. Tominaga, and M. Yamaguchi. "The Λ N, ΛΛ and ΞN Attractions in the Intermediate Force Range." In Few-Body Problems in Physics ’99, 372–77. Vienna: Springer Vienna, 2000. http://dx.doi.org/10.1007/978-3-7091-6287-3_65.

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Xue, Guoliang. "A Cost Optimal Parallel Algorithm for Computing Force Field in N-Body Simulations." In Lecture Notes in Computer Science, 95–104. Berlin, Heidelberg: Springer Berlin Heidelberg, 1998. http://dx.doi.org/10.1007/3-540-68535-9_13.

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Jendrsczok, Johannes, Rolf Hoffmann, and Thomas Lenck. "Generated Horizontal and Vertical Data Parallel GCA Machines for the N-Body Force Calculation." In Architecture of Computing Systems – ARCS 2009, 96–107. Berlin, Heidelberg: Springer Berlin Heidelberg, 2009. http://dx.doi.org/10.1007/978-3-642-00454-4_12.

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Antoni, M., C. Sandoz, and Y. Elskens. "Numerical Study of Turbulence in N-Body Hamiltonian Systems with Long Range Force: I. Relaxation." In Hamiltonian Systems with Three or More Degrees of Freedom, 290–94. Dordrecht: Springer Netherlands, 1999. http://dx.doi.org/10.1007/978-94-011-4673-9_25.

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Demetropoulos, I. N., I. P. Gerothanassis, and D. G. Papageorgiou. "The First Solvation Sphere of N-Methylformamide (NMF) in Water: MM2(87) Force Field and Ab Initio Studies." In Spectroscopy of Biological Molecules, 43–44. Dordrecht: Springer Netherlands, 1995. http://dx.doi.org/10.1007/978-94-011-0371-8_17.

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Tian, Xin Li, Zhi Yuan Wu, An Ying She, and Zhong Xiang Hu. "Passivation Model of Diamond Grinding Wheel in Constant-Force Grinding of Si3N4 Ceramic." In Advances in Grinding and Abrasive Technology XIV, 94–97. Stafa: Trans Tech Publications Ltd., 2007. http://dx.doi.org/10.4028/0-87849-459-6.94.

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Chevtchenko, S., Q. Fan, Cole W. Litton, A. A. Baski, and Hadis Morkoç. "Effects of Rapid Thermal Annealing Treatment on the Surface Band Bending of n-type GaN Studied by Surface Potential Electric Force Microscopy." In Silicon Carbide and Related Materials 2005, 1529–32. Stafa: Trans Tech Publications Ltd., 2006. http://dx.doi.org/10.4028/0-87849-425-1.1529.

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Klages, H. O., K. Hofmann, W. Nitz, P. Doll, R. Garrett, W. Heeringa, and H. Krupp. "Analyzing power of the $$^2 H(\vec n, n)d^*$$ (FSI) breakup reaction from 20 to 50 MeV." In The Three-Body Force in the Three-Nucleon System, 311–12. Berlin, Heidelberg: Springer Berlin Heidelberg, 1986. http://dx.doi.org/10.1007/3-540-16805-2_43.

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Conference papers on the topic "N-Force"

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XU, M. S., J. B. XU, and J. AN. "REAL-TIME VISUALIZATION OF MORPHOLOGICAL EVOLUTION OF N,N'-di(naphthalene-1-yl)-N,N'-diphthalbenzidine THIN FILMS: VARIABLE TEMPERATURE ATOMIC FORCE MICROSCOPY STUDY." In Proceedings of the Asian Symposium on Nanotechnology and Nanoscience 2002. WORLD SCIENTIFIC, 2003. http://dx.doi.org/10.1142/9789812796714_0061.

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Cappelleri, D. J., G. Piazza, and V. Kumar. "Two-dimensional, vision-based μN force sensor for microrobotics." In 2009 IEEE International Conference on Robotics and Automation (ICRA). IEEE, 2009. http://dx.doi.org/10.1109/robot.2009.5152647.

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Bounab, B., D. Sidobre, and A. Zaatri. "Central axis approach for computing n-finger force-closure grasps." In 2008 IEEE International Conference on Robotics and Automation (ICRA). IEEE, 2008. http://dx.doi.org/10.1109/robot.2008.4543362.

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Niino, T., S. Egawa, N. Nishiguchi, and T. Higuchi. "Development of an electrostatic actuator exceeding 10 N propulsive force." In [1992] Proceedings IEEE Micro Electro Mechanical Systems. IEEE, 1992. http://dx.doi.org/10.1109/memsys.1992.187702.

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Meissner, T. "Meson mixing from QCD sum rules and its application to the charge symmetry breaking N-N force." In The 5th conference on the intersections of particle and nuclear physics. AIP, 1995. http://dx.doi.org/10.1063/1.48526.

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El-Khoury, S., and A. Sahbani. "On computing robust n-finger force-closure grasps of 3D objects." In 2009 IEEE International Conference on Robotics and Automation (ICRA). IEEE, 2009. http://dx.doi.org/10.1109/robot.2009.5152272.

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Yu Zheng, Ming C. Lin, and Dinesh Manocha. "A fast n-dimensional ray-shooting algorithm for grasping force optimization." In 2010 IEEE International Conference on Robotics and Automation (ICRA 2010). IEEE, 2010. http://dx.doi.org/10.1109/robot.2010.5509297.

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Wang, Yinfeng, Anping Liu, and Xueheng Yang. "Study on Nano-(Ti, Zr)N Film by Atomic Force Microscopy." In 2006 1st IEEE International Conference on Nano/Micro Engineered and Molecular Systems. IEEE, 2006. http://dx.doi.org/10.1109/nems.2006.334851.

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Kenji Miyamoto, Tomoya Jomori, Koji Sugano, Osamu Tabata, and Toshiyuki Tsuchiya. "Mechanical calibration of MEMS spring with 0.1-μn force resolution." In 2007 IEEE 20th International Conference on Micro Electro Mechanical Systems (MEMS). IEEE, 2007. http://dx.doi.org/10.1109/memsys.2007.4432965.

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Meissner, Th, E. M. Henley, T. Hatsuda, and C. Chan. "Meson mixing in the QCD sum rules and its application to the charge symmetry breaking N-N force." In The 14th international conference of few-body problems in physics. AIP, 1995. http://dx.doi.org/10.1063/1.48109.

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Reports on the topic "N-Force"

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Caspi, S. Forces in a thin cosine(n{theta}) helical wiggler. Office of Scientific and Technical Information (OSTI), March 1995. http://dx.doi.org/10.2172/125418.

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Luc, Brunet. Systematic Equations Handbook : Book 1-Energy. R&D Médiation, May 2015. http://dx.doi.org/10.17601/rd_mediation2015:1.

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Abstract:
The energy equation handbook is the complete collection of physically coherent expression of energy computed using from 2 to 7 physical units among: density(ML-3) energy (ML2T-2) time (T) force (MLT-2) power (ML2T-3) current (I) temperature (Th) quantity (N) mass (M) length (L) candela (J) surface (L2) volume (L3) concentration (ML-3) frequency (T-1) acceleration (LT- 2) speed (LT-1) pressure (ML-1T-2) viscosity (ML-1T-1) luminance (L- 2J) MolarMass (MN-1) MassicEnergy (L2T-2) resistance (ML2T-3I-2) voltage (ML2T-3I-1) Farad (M-1L-2T4I2) Thermal- Conductivity (MLT-3Th-1) SpecificHeat (L2T-2Th-1) MassFlux (MT-1) SurfaceTension (MT-2) Charge (TI) Resistivity (ML3T-3I-2) The complete list of 4196 equations is sorted by number of variable required to obtain an energy in Joules. All the units are in MKSA.
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