491 |
Development of a teaching coulometry instrument for the direct determination of sulfur compounds and of zinc indirectlyPadilla Mercado, Jeralyne Beatriz 20 July 2017 (has links)
No description available.
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492 |
Structure-Property Studies of Substituted Azadipyrromethene-Based Dyes and High Dielectric Constant Polymers for Organic Electronic ApplicationsPejic, Sandra 31 August 2018 (has links)
No description available.
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493 |
Characterization of Vertical Interconnects in 3-D Monolithic Microwave Integrated Circuits (3-D MMIC)Kang, Qinghua (George) 01 July 2003 (has links)
No description available.
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494 |
On the Satisfaction of Modulus and Ambiguity Function Constraints in Radar Waveform Optimization for DetectionPatton, Lee Kenneth 27 July 2009 (has links)
No description available.
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495 |
Adaptive Robust Regression Approaches in data analysis and their ApplicationsZhang, Zongjun January 2015 (has links)
No description available.
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496 |
VARIABILITY AND LOCATION OF MOVEMENT ENDPOINT DISTRIBUTIONS: THE INFLUENCE OF INSTRUCTIONS FOR MOVEMENT SPEED AND ACCURACYDey, Abhishek 24 May 2016 (has links)
No description available.
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497 |
Topics in the Physics of Inhomogeneous MaterialsBarabash, Sergey V. 30 July 2003 (has links)
No description available.
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498 |
Teaching imitation skills to preschool children with severe disabilities: The effects of embedding constant time delay within a small group activityValk, Jennie Elise 16 October 2003 (has links)
No description available.
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499 |
Identification and biochemical characterization of a novel receptor:ligand interaction between FcRn and albuminChaudhury, Chaity 09 March 2005 (has links)
No description available.
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500 |
Design of passively loaded specimen for constant KI during crack growth / Design av passivt belastad provstav för konstant KI vid spricktillväxtTofferi, Liisa January 2021 (has links)
Passive loading of a specimen is a relatively cheap method to use in fracture mechanical testing compared to an actively loaded specimen. For stress corrosion cracking testing it is easier to use a passively loaded specimen since the specimen easily can be placed in a specific corrosive environment. The passive method lacks information about the crack growth over time and the load can not be regulated during the test to ensure crack growth. This thesis work was mainly about finding a specimen with a region of constant KI to ensure crack growth without the need of controlling the load and to find a way to estimate the crack growth over time. The work is based on Linear Elastic Fracture Mechanics and the Finite Element Method. The thesis work resulted in a specimen with constant KI in the region 23/50 ≤ a/W ≤ 33/50 of crack growth and an equation was found to describe the relation between the crack propagation and the strain measured on the specimens back face. / Passiv belastning av en provstav är en relativt billig metod att använda för brottmekanisk provning jämfört med en aktivt belastad provstav. En passivt belastad provstav är enklare att använda vid provning av spänningskorrosion då provstaven enkelt kan placeras i en specifik korrosiv miljö. Den passiva metoden är bristande i information om spricktillväxen över tid och belastningen på provstaven kan inte justeras för att upprätthålla fortsatt spricktillväxt under provningens gång. Detta examensarbete syftade till att ta fram en provstav med ett spricktillväxtomrade med konstant KI för fortsatt spricktillväxt vid konstant belastning samt att hitta en metod för att uppskatta spricktillväxten över tid. Arbetet är baserat på linjärelastisk brottmekanik och finita elementmetoden. Arbetet resulterade i en provstav med konstant KI i spricktillväxtområdet 23/50 ≤ a/W ≤ 33/50 och en relation mellan spricktillväxt och töjningen som mäts på provstavens baksida.
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