Waves move in a special way. 
Waves move in a special way. 
A flat group is called a plane wave. A round group is called a spherical wave. These groups move through space.
Lenses can change the shape of a wave. A lens can turn a flat wave into a round one. This happens when waves go through the lens.
Waves can also bend. This happens when they hit a small opening. The waves act like many tiny new waves.
Sunlight hits the Earth as a giant round wave. It is very big!
Imagine a wave moving through space. A wavefront is a set of points that all move together.
Wavefronts can have different shapes. A plane wave has flat wavefronts. These waves move in one direction.
Shapes can also change. When waves go through a lens, they change shape. This is called refraction. A lens can turn a flat wave into a round one. 
Scientists use a wavefront sensor to study these waves. This tool measures how much a wave is out of shape. These tools help us fix telescopes. They can even help us study the human eye.
A wavefront is a special part of a moving wave. It is a set of points that all have the same phase. Phase tells us where a wave is in its cycle.
Wavefronts come in different shapes like planes or spheres. A plane wave has flat wavefronts that move together. These waves travel in one direction. We call this light collimated light. A spherical wave has round wavefronts that expand outward. This happens when energy carries away in all directions. The paths of this energy are called rays. These rays are always perpendicular to the wavefront. 
Shapes can change when waves hit different objects. This often happens through a process called refraction. Refraction occurs when the speed of a wave changes at different points. Lenses can change the shape of optical wavefronts. They can turn a flat plane wave into a spherical one. You can also see waves bend through diffraction. This happens when a wave hits a small slit or aperture. The Huygens–Fresnel principle helps explain this bending. It treats every point on a wavefront as a new source of tiny waves.
Sometimes, wavefronts do not stay in a perfect shape. These errors are called optical aberrations. They can happen because of lens thickness or small mistakes. A perfect lens might have a spherical surface. However, the ideal surface would actually be aspheric. Large telescopes also face aberrations from the atmosphere. Changes in the air can cause the wavefront to deviate. This deviation from a perfect plane is the wavefront aberration. Scientists try to minimize these errors in many different systems.
Special tools called wavefront sensors help measure these errors. These devices describe the optical quality of a system. One common tool is the Shack–Hartmann wavefront sensor. It uses a special array of tiny lenses called lenslets. Other tools include the wavefront curvature sensor and the pyramid wavefront sensor. Scientists use these to improve adaptive optics in telescopes. They can even use them to measure the eye. A weak laser can reflect off the retina to help study it. 
In physics, a wavefront is a specific set of points within a time-varying wave field. These points all share the same phase. Phase describes a specific stage in a wave's cycle. This concept is most useful for fields that vary sinusoidally in time. This means the field changes following a smooth, repeating pattern with a single frequency. Without this consistent frequency, the phase is not well defined.
Wavefronts generally move through space as time passes. Their geometric shape depends on the dimensions of the medium. In a unidimensional medium, a wavefront is typically a single point. In a two-dimensional medium, wavefronts appear as curves. In a three-dimensional medium, they exist as surfaces.
There are different types of simple wavefronts, such as plane waves and spherical waves. A plane wave consists of flat wavefronts that move together in one direction. The light from such a wave is called collimated light. A spherical wave consists of spherical surfaces that expand outward. This expansion happens because the wave carries energy equally in all directions. The paths of this energy flow are called rays. These rays are always perpendicular to the wavefront.
Sunlight provides a massive example of a spherical wavefront. It strikes the Earth with a radius of about 150 million kilometers, also known as 1 AU. Because this radius is so large, the wavefront can be treated as a plane over distances equal to Earth's diameter. The shape of a wavefront can also change through refraction. Refraction occurs if the speed of propagation differs at different points on the wavefront. For example, lenses can change optical wavefronts from planar to spherical or vice versa. 
Classical physics explains wave bending through the Huygens–Fresnel principle. This principle treats every point on a propagating wavefront as a source of secondary spherical waves. When a coherent source, like a laser, hits a small slit or aperture, a bending pattern appears. This happens because secondary waves from each point interfere with one another. If there are multiple closely spaced openings, such as a diffraction grating, a complex pattern of varying intensity results. Scientists use Huygens' principle as a quick way to predict how wavefronts move through free space.
Sometimes, wavefronts do not maintain their ideal shapes. This deviation from a perfect planar wavefront is called a wavefront aberration. These errors can be caused by lens thickness or manufacturing imperfections. For instance, a lens might have a spherical surface, even though an aspheric surface would be ideal. These shortcomings create optical aberrations like coma or spherical aberration. Large telescopes also face aberrations due to spatial variations in the atmosphere's index of refraction. 
To manage these errors, scientists use devices called wavefront sensors. These tools measure wavefront aberrations to describe the optical quality of a system. One common type is the Shack–Hartmann wavefront sensor, which uses a lenslet array. Other types include the pyramid wavefront sensor and the wavefront curvature sensor, also known as the Roddier test. These sensors are vital for adaptive optics and optical metrology. They are even used to measure aberrations in the human eye. In medical uses, a weak laser can reflect off the retina to sample the wavefront. 
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