For a perfect optical system, every ray that leaves a given object point P
successfully travels to the corresponding image point P'.
Lenses with spherical surfaces only image P to P' in the paraxial approximation, when the light stays close to the optic axis and rays make small angles with the optic axis. Otherwise the image of a point can become a more or less smeared out blob.
Spherical aberrations dominate when
a wide beam, which is parallel to the optic axis, is focused by a
converging lens with spherical surfaces. The focal length for rays
which travel through the outer regions of the lens is shorter than that
for the rays traveling through the center of the lens.
The figure to below shows rays incident parallel to the optical axis from a very distant on-axis object point, such as a star. They are refracted as they travel towards the paraxial focal plane. The least blurry image is produced a short distance to the left of the paraxial focal plane and is called the circle of least confusion.
The amount of refraction at the two surfaces of the lens is not the same. Spherical aberrations can be reduced by equalizing the amount of refraction at both surfaces of a lens. This can be done by varying the shape of the lens, while keeping the index of refraction, thickness, and focal length constant. Only the radii of the lens are changed. This is called bending the lens.
Due to spherical aberration, the image of an object point that lies on the optical axis is not a point but a spherical blob.
Link: YouTube, Spherical Aberration
Coma aberrations degrade the image of an off-axis object point. The point is imaged to a blob, whose shape resembles that of a comet tail. A streak of light appears to emanate from a focused spot. On a sunny day use a magnifying glass to focus an image of the sun. When you tilt he magnifying glass with respect to the line of sight to the sun, the sun's image will elongate into a comet-like shape that is characteristic of coma aberration.
Link: YouTube, coma aberration
Astigmatism aberrations degrade the images of off-axis object points formed by lenses with spherical surfaces and the images of all points formed by lenses with two different radii of curvature in two perpendicular planes. (These are lenses that are shaped more like a football than a sphere.) The image of an off-axis point appears as a line or ellipse instead of a discrete point. Rays that propagate in to perpendicular planes have different focal points. Astigmatism is very common in the human eye.
Because there are two different image planes, an object with spokes can have an image in one plane for which the vertical lines are sharp, but lines that make an angle with the vertical become more and more blurred as the angle approaches 90o. In the other image plane, horizontal lines can be sharp and vertical lines are blurred. Eye examinations detect astigmatism if the spokes appear to go from black to gray.
Assume we want to image an off-axis object point
If we move a screen into the focal plane of the blue fan, then the image of a point is a horizontal line segment. The image of a series of points forming a horizontal line will be a sharp horizontal line formed by overlapping horizontal line segments. But the image of a series of points forming a vertical line will be a very blurry vertical line formed by vertically stacked horizontal line segments. If we move the screen into the focal plane of the red fan, then the image of a point is a horizontal line segment. Now the image of a series of points forming a vertical line will be a sharp vertical line formed by overlapping vertical line segments. But the image of a series of points forming a horizontal line will be a very blurry horizontal line formed by horizontally stacked vertical line segments.
Curvature of field is not a point aberration, but an aberration associated with an extended object. When extended objects are imaged with spherical lenses all transverse points on the image are in focus at the same time on a curved surface instead of on a plane. On a plane screen capturing the image, the center and the outer regions of an extended object are in focus at different distances away from the lens. This defect is called Petzval curvature or curvature of field defect.
Distortion is another aberration associated with extended objects is distortion. Distortion results when the magnification is a function of the distance away from the optical axis. Distortion is what causes vertical lines to bulge outward (barrel distortion) or inward (pincushion distortion) at the image plane.
Chromatic aberrations result from material dispersion. Because
Snell's law depends on the index of refraction n, and different
colors of light refract by different amounts, an image point formed by light of
one color does not coincide with the corresponding image point formed by light
of a different color. This is not a geometrical aberration.
Images formed by spherical mirrors can also be affected by spherical aberrations, coma, astigmatism, curvature of field and distortion. But images formed by spherical mirrors are free from chromatic aberrations, since, unlike Snell's law, the law of reflection does not depend on the index of refraction n.
A real spherical concave
mirror does not perfectly focus the light from a point source. This can be
due to which defects?
Point aberrations associated with spherical surfaces are spherical aberrations, coma, and astigmatism. A mirror produces no chromatic aberrations, since the law of reflection does not involve the index of refraction.