The school science attitude survey: a new instrument for measuring attitudes towards school science

2016 ◽  
Vol 39 (4) ◽  
pp. 422-445 ◽  
Author(s):  
JohnPaul Kennedy ◽  
Frances Quinn ◽  
Neil Taylor
PLoS ONE ◽  
2019 ◽  
Vol 14 (1) ◽  
pp. e0209027 ◽  
Author(s):  
Radu Bogdan Toma ◽  
Jesús Ángel Meneses Villagrá

2019 ◽  
Author(s):  
Radu Bogdan Toma ◽  
Jesús Ángel Meneses Villagrá

2018 ◽  
Vol 5 (1) ◽  
pp. 1-22 ◽  
Author(s):  
Sophie Bartlett ◽  
Michael T. Fitzgerald ◽  
David H. McKinnon ◽  
Lena Danaia ◽  
Jasmina Lazendic-Galloway

A new survey for measuring students’ astronomy and science attitudes that has been validated for use with high school students (with a future intent to expand to middle school and university) is presented. We initially present a short review of instruments in the literature that attempt to measure attitudes in astronomy together with the difficulties encountered in measuring these by researchers in the subsequent analyses of results. To illustrate this, we present an example from an Astro101-level university course to display the problems with the current, most commonly used, astronomy attitude instrument. We then present the initial design and the Factor Analysis of a new instrument designed to address the deficiencies of this existing instrument from a sample of students in a high school-level astronomy education project. The factors identified by this instrument include: Interest in Astronomy, Interest in Science Outside of School, Practical Work in Science, Teacher’s Actions in science, Perceptions of Ability in Science, Future Aspirations in Science, Benefits of Science, and Personal Relevance of School Science, all of which possess high internal response consistency and construct validity.


Author(s):  
H. Tochigi ◽  
H. Uchida ◽  
S. Shirai ◽  
K. Akashi ◽  
D. J. Evins ◽  
...  

A New High Excitation Objective Lens (Second-Zone Objective Lens) was discussed at Twenty-Sixth Annual EMSA Meeting. A new commercially available Transmission Electron Microscope incorporating this new lens has been completed.Major advantages of the new instrument allow an extremely small beam to be produced on the specimen plane which minimizes specimen beam damages, reduces contamination and drift.


Author(s):  
John F. Mansfield

The current imaging trend in optical microscopy, scanning electron microscopy (SEM) or transmission electron microscopy (TEM) is to record all data digitally. Most manufacturers currently market digital acquisition systems with their microscope packages. The advantages of digital acquisition include: almost instant viewing of the data as a high-quaity positive image (a major benefit when compared to TEM images recorded onto film, where one must wait until after the microscope session to develop the images); the ability to readily quantify features in the images and measure intensities; and extremely compact storage (removable 5.25” storage devices which now can hold up to several gigabytes of data).The problem for many researchers, however, is that they have perfectly serviceable microscopes that they routinely use that have no digital imaging capabilities with little hope of purchasing a new instrument.


Author(s):  
Lee H. Veneklasen

This paper discusses some of the unique aspects of a spectroscopic emission microscope now being tested in Clausthal. The instrument is designed for the direct parallel imaging of both elastic and inelastic electrons from flat surfaces. Elastic contrast modes of the familiar LEEM include large and small angle LEED, mirror microscopy, backscatter diffraction contrast (for imaging of surface structure), and phase contrast (for imaging of step dynamics)(1). Inelastic modes include topology sensitive secondary, and work function sensitive photoemission. Most important, the new instrument will also allow analytical imaging using characteristic Auger or soft X-ray emissions. The basic instrument has been described by Bauer and Telieps (2). This configuration has been redesigned to include an airlock, and a LaB6 gun, triple condensor lens, magnetic objective lens, a double focussing separator field, an imaging energy analyzer, and a real time image processor.Fig. 1 shows the new configuration. The basic beam voltage supply Vo = 20 KV, upon which separate supplies for the gun Vg, specimen Vs, lens electrode Vf, and analyzer bias Vb float. The incident energy at the sample can be varied from Vs = 0-1 KV for elastic imaging, or from Vg + Vs = (3 + Vs) KV for inelastic imaging. The image energy window Vs±V/2 may be varied without readjusting either the illumation, or imaging/analyzer optics. The diagram shows conjugate diffraction and image planes. The apertures defining incoming Humiliation and outgoing image angles are placed below the separator magnet to allow for their independent optimization. The instrument can illuminate and image 0.5-100 μm fields at 0-1 keV emission energies with an energy window down to 0.2 eV.


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