Image 1 Caption: A plane reflection of a distorted brown oval through a plane to create a distorted green oval followed by a second plane reflection through a second plane parallel to the first one in order to create a distorted blue oval.
Features:
The mirror surface is the reflection plane, of course.
To understand real image and virtual image in optics, let's consider real image formation and then virtual image formation:
Consider a point source of light. Say in an optical device, a fraction of light rays from the point source converge to an image point, actually pass through it, and then diverge from that image point which is then seen in some directions as the image of the point source: in other directions there is nothing to be seen: the image is NOT a complete recreation of the point source. A continuum of point sources creates a finite source and a continuum of image points which creates a finite image: which can only be seen in certain directions.
The image is called a real image since there is actual light at the image points and you can detect it for example with a camera.
In virtual image formation, light rays from a source diverge from the image points, but do NOT actually start at those image points. Reflections and/or refractions in an optical device put the light rays on those divergent paths. Image 2 below shows an example of light rays being put on divergent paths from an image point.
The image is called a virtual image since it has the effect of being a source of light rays, but there is NO light at the image points: there's nothing at them and you CANNOT take an image at them.
As aforesaid, mirror reflections
always give virtual images---the
images exist in "mirror space."
Mirror reflection
is illustrated adjacently in the Image 2.
Mirror inversion
is, in fact, the combination of front-to-back inversion and the observer's orientation.
The observer's orientation is important in looking at sources too.
If you look at source and then stand on your stand on your head---which is NOT
recommended---there's an inversion.
For an example of mirror inversion,
say you are facing a cross marked with
cardinal directions: NESW
going clockwise per usual.
Behind you is a mirror.
You can rotate your head to look at the cross image in different ways:
The upshot is that
plane reflection
(which gives the intrinsic
front-to-back inversion through the reflection plane) plus the observer orientation
results in mirror inversion.