For and negative focal length ,
The transverse magnification is , so
Thus the virtual image is upright, half the object's height, and from the lens on the object's side. A parallel incident light ray diverges after the lens as though it originated at the near optical focus; the central light ray continues undeviated in the ideal thin lens model. Their backward extensions meet at the image tip, .
Figure 1.
Ray tracing for the diverging thin lens: backward extensions locate the upright virtual image
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