An observer above the plane surface of a liquid of index of refraction n, looking at a point object which is a distance Y below the surface, will see a virtual image of the object. For light rays which emerge in air at an angle of refraction θ2=0, the virtual image will be at a distance (Y/n) below the surface. The case where θ2≠0 is rarely discussed in texts. As a result, students may be left with the impression that the location of the virtual image is independent of θ2. The virtual image is astigmatic and the locations of the different components of the astigmatic image depend on the angle of refraction θ2. The location of the various components of the astigmatic image are derived; a laboratory experiment to measure the locations of the components is described. The results of the measurements are in good agreement with the theory.
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July 1984
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July 01 1984
Note on a common virtual image Available to Purchase
Albert A. Bartlett;
Albert A. Bartlett
Department of Physics, Box 390, University of Colorado, Boulder, Colorado 80309
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Rodger Lucero;
Rodger Lucero
Department of Physics, Box 390, University of Colorado, Boulder, Colorado 80309
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Gordon O. Johnson
Gordon O. Johnson
Department of Physics, Walla Walla College, College Place, Washington 99324
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Albert A. Bartlett
Department of Physics, Box 390, University of Colorado, Boulder, Colorado 80309
Rodger Lucero
Department of Physics, Box 390, University of Colorado, Boulder, Colorado 80309
Gordon O. Johnson
Department of Physics, Walla Walla College, College Place, Washington 99324
Am. J. Phys. 52, 640–643 (1984)
Article history
Received:
June 03 1982
Accepted:
September 26 1983
Citation
Albert A. Bartlett, Rodger Lucero, Gordon O. Johnson; Note on a common virtual image. Am. J. Phys. 1 July 1984; 52 (7): 640–643. https://doi.org/10.1119/1.13585
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