Specular reflection is the mirror-like reflection of light from a surface, in which light from
a single incoming direction is reflected into a single outgoing direction.
Such behavior is described by the law of reflection, which states that the direction of incoming
light, and the direction of outgoing light reflected make the same angle with respect
to the surface normal, thus the angle of incidence equals the angle of reflection, and that the
incident, normal, and reflected directions are coplanar.
This behavior was first discovered through careful observation and measurement by Hero
of Alexandria.
Explanation Specular reflection is distinct from diffuse
reflection, where incoming light is reflected in a broad range of directions.
An example of the distinction between specular and diffuse reflection would be glossy and
matte paints.
Matte paints have almost exclusively diffuse reflection, while glossy paints have both
specular and diffuse reflection.
A surface built from a non-absorbing powder, such as plaster, can be a nearly perfect diffuser,
whereas polished metallic objects can specularly reflect light very efficiently.
The reflecting material of mirrors is usually aluminum or silver.
Even when a surface exhibits only specular reflection with no diffuse reflection, not
all of the light is necessarily reflected.
Some of the light may be absorbed by the materials.
Additionally, depending on the type of material behind the surface, some of the light may
be transmitted through the surface.
For most interfaces between materials, the fraction of the light that is reflected increases
with increasing angle of incidence . If the light is propagating in a material with a
higher index of refraction than the material whose surface it strikes, then total internal
reflection may occur if the angle of incidence is greater than a certain critical angle.
Specular reflection from a dielectric such as water can affect polarization and at Brewster's
angle reflected light is completely linearly polarized parallel to the interface.
The law of reflection arises from diffraction of a plane wave with small wavelength on a
flat boundary: when the boundary size is much larger than the wavelength then electrons
of the boundary are seen oscillating exactly in phase only from one direction – the specular
direction.
If a mirror becomes very small compared to the wavelength, the law of reflection no longer
holds and the behavior of light is more complicated.
Waves other than visible light can also exhibit specular reflection.
This includes other electromagnetic waves, as well as non-electromagnetic waves.
Examples include ionospheric reflection of radiowaves, reflection of radio- or microwave
radar signals by flying objects, acoustic mirrors, which reflect sound, and atomic mirrors,
which reflect neutral atoms.
For the efficient reflection of atoms from a solid-state mirror, very cold atoms and/or
grazing incidence are used in order to provide significant quantum reflection; ridged mirrors
are used to enhance the specular reflection of atoms.
The reflectivity of a surface is the ratio of reflected power to incident power.
The reflectivity is a material characteristic, depends on the wavelength, and is related
to the refractive index of the material through Fresnel's equations.
In absorbing materials, like metals, it is related to the electronic absorption spectrum
through the imaginary component of the complex refractive index.
Measurements of specular reflection are performed with normal or varying incidence reflectometers
using a scanning variable-wavelength light source.
Lower quality measurements using a glossmeter quantify the glossy appearance of a surface
in gloss units.
The image in a flat mirror has these features: It is the same distance behind the mirror
as the object is in front.
It is the same size as the object.
It is the right way up.
It is reversed.
It is virtual, meaning that the image appears to be behind the mirror, and cannot be projected
onto a screen.
The reversal of images by a plane mirror is perceived differently depending on the circumstances.
In many cases, the image in a mirror appears to be reversed from left to right.
If a flat mirror is mounted on the ceiling it can appear to reverse up and down if a
person stands under it and looks up at it.
Similarly a car turning left will still appear to be turning left in the rear view mirror
for the driver of a car in front of it.
The reversal of directions, or lack thereof, depends on how the directions are defined.
More specifically a mirror changes the handedness of the coordinate system, one axis of the
coordinate system appears to be reversed, and the chirality of the image may change.
For example the image of a right shoe will look like a left shoe.
See also: Mirror Image.
Direction of reflection
The direction of a reflected ray is determined by the vector of incidence and the surface
normal vector.
Given an incident direction from the surface to the light source and the surface normal
direction the specularly reflected direction is:
where is a scalar obtained with the dot product.
Different authors may define the incident and reflection directions with different signs.
Assuming these Euclidean vectors are represented in column form, the equation can be equivalently
expressed as a matrix-vector multiplication:
where is the so-called Householder transformation matrix, defined as:
denotes transposition and is the identity matrix.
See also Fresnel equations, which describe the behavior
of light when moving between media of differing refractive index
Geometric optics Hamiltonian optics
Mirror, a device designed for specular reflection Atomic mirror, a device for specular reflection
of atoms
Reflection coefficient Reflection
Specular highlight Specularity
Plane of incidence References