In classical physics light is assumed to be an electromagnetic wave. Electromagnetic waves are categorized according to their frequency f or, equivalently, according to their wavelength λ. The speed of any electromagnetic waves in free space is the speed of light c = 3*108 m/s. Electromagnetic waves can have any wavelength λ or any frequency f as long as λf = c. Visible light has a wavelength range from ~400 nm to ~750 nm. Violet light has a wavelength of ~400 nm, and a frequency of ~7.5*1014 Hz. Red light has a wavelength of ~700 nm, and a frequency of ~4.3*1014 Hz.
Electromagnetic (EM) waves are changing electric and magnetic
fields, carrying energy through space. EM waves require no medium, they
can travel through empty space. Let E denote the electric field
vector and B the magnetic field vector of the EM wave. For
electromagnetic waves E and B are always perpendicular to each
other, and perpendicular to the direction of propagation of the wave.
In general we pay more attention to the electric field E, because detectors such as the eye, photographic film, and CCDs interact with the electric field.
Electromagnetic waves are transverse waves. In this session you will measure the intensity of a light wave as a function of distance from the source and you will investigate various polarization effects.
Open a Microsoft Word document to keep a log of your experimental procedures, results and discussions. This log will become your lab report. Address the points highlighted in blue. Answer all questions.
If light propagates through a transparent material such as water or glass, it
interacts in various ways with the atoms or molecules that make up the material.
This interaction can be wavelength and polarization dependent. Due to the
interaction, light moves through a transparent material with an apparent speed v = c/n.
The index of refraction n is a property of the material. It is greater
than 1, so that v is less than c. In most transparent materials the index
of refraction depends slightly on the wavelength of the light, and in some
materials it depends on the polarization.
Linear polarization: An ideal linear polarizer is a material that passes only light waves for which the electric field vector is parallel to its transmission axis. If E0 is the incident field vector and the angle between E0 and the transmission axis is θ, then the magnitude of transmitted field vector is E0 cosθ, and its direction is the direction of the transmission axis. The intensity I of an electromagnetic wave is proportional to the square of the magnitude of the electric field vector. We therefore have
Itransmitted = I0 cos2θ.
|Polarizers with parallel
|Polarizers with perpendicular
|Polarizer 3 between
polarizers 1 and 2.
Spend a few minutes exploring with the three pieces of linear polarizing material provided to you in an envelope.
Put the pieces of polarizing materials back into the envelope for the next lab session.
In this experiment you will use a linear polarizer to produces a polarized beam and then pass this beam through a second polarizer whose transmission axis makes an angle θ with respect to the transmission axis of the first one. You will check that Itransmitted = I0 cos2θ. This is called the Law of Malus.
Do not move the bases on the rail. Do not remove the components from the post holders. Only adjust the height and orientation of the components.
In Excel create a table.
|angle (deg)||I||angle (rad)||I - IB||I0*cos2(angle)|
When unpolarized light is incident on a boundary between two transparent materials, for example on an air-glass boundary, then the reflected and transmitted components are partially plane polarized. The reflected wave is 100% linearly polarized when the incident angle is equal to the Brewster angle θB, where tanθB = n2/n1. The Brewster angle for reflecting off glass is between 50o and 60o.
You will reflect the light from a diode laser off a glass plate. You will make sure that the
incident angle is close to the Brewster angle and verify that light polarized in
the plane of incidence it will not be reflected at the Brewster angle. The
plane of incidence is a plane perpendicular to the reflecting surface that
contains the incident beam.
If the reflecting surface is horizontal, then the plane of incidence is vertical. The reflected light at the Brewster angle is horizontally polarized and can be blocked by a polarizer with a vertical transmission axis. If the reflecting surface is vertical, then the plane of incidence is horizontal, and horizontally polarized light will not be reflected at the Brewster angle. Then the reflected light is vertically polarized at the Brewster angle and can be blocked by a polarizer with a horizontal transmission axis. You will reflect the laser light off a vertical glass surface (a microscope slide) and find the Brewster angle.
Convert your log into a lab report.
Laboratory 6 Report
Save your Word document (your name_lab6.docx), go to Canvas, Assignments, Lab 6, and submit your document.