Specification for a motion and time study laboratory.

Date

1970

Author

Timurkan, Ahmet

Metadata

Show full item record

Item Usage Stats

37
views

0
downloads

URI

https://hdl.handle.net/11511/5942

Collections

Graduate School of Natural and Applied Sciences, Thesis

Suggestions

OpenMETU
Core

Design of a radio frequency identification (rfid) antenna Kalaycı, Sefa; Birand, Mehmet Tuncay; Department of Electrical and Electronics Engineering (2009) Fundamental features of Radio Frequency Identification (RFID) systems used in different application areas will be reviewed. Techniques used in realizing RFID antenna systems will be studied and the procedure to realize a specific RFID antenna type possessing desired characteristics will be described. Electrical properties such as radiation pattern, impedance will be predicted using analytical and/or computer simulation techniques. Experimental investigations will be carried out to complement the theoretical...
Design of a warm air heater. Dölen, Özhan; Department of Mechanical Engineering (1963)
Design of a high-precision, 0.5 m aperture Cassegrain collimator Karci, Ozgur; Ekinci, Mustafa (The Optical Society, 2020-09-01) We present the realization of a high-precision, 0.5m aperture size Cassegrain collimator system. The optical design, the optomechanical design, the mirror manufacturing, and the telescope alignment with a performance evaluation are extensively discussed. The optical design of the collimator is based on the Cassegrain telescope design with two aspheric mirrors. An athermalized, high stability optomechanical structure is conceived for the collimator to meet stringent performance requirements. The high-quality...
Implementation of a multiple-input, multiple-output (MIMO) active noise control system Başçi, Faysal; Çiloğlu, Tolga; Department of Electrical and Electronics Engineering (2002)
Implementation of a data acquisition system for contactless conductivity imaging Ulker, B; Gençer, Nevzat Güneri (2002-09-01) A data acquisition system is realized for conductivity imaging via contactless measurements. It is observed that field profiles are good representatives of the conductive objects scanned by the measurement system. Three different data sets are taken with different scanning resolutions. Note that although the scanning resolution is decreased 25 times, it is still possible to observe the conductive object. The data acquisition time is due to the data acquisition time limit of the lock-in amplifier. As might b...

Citation Formats

A. Timurkan, “Specification for a motion and time study laboratory.,” Middle East Technical University, 1970.