Wednesday, February 29, 2012
Outreach scientific videos
Tuesday, August 30, 2011
Sam's Laser FAQ
ps: check out the laser equipment gallery
Wednesday, June 23, 2010
LAB2 - The Virtual Femtosecond Laboratory
As examples they mention:
- propagation through a linear medium
- prism compressor
- second harmonic generation with depleted fundamental wave
- crystal wizard - how to find the phase matching angle
LabII was developed in 1998 at the Institute for Optics and Quantum Electronics (IOQ) in Jena. Since Fall 2004 it is at the Institute of Applied Physics in Bern with Prof. Thomas Feurer. The download is free but you have to register. What I like is the detailed manual which will help you to use efficiently LAB2. Basics and concepts are introduced too and always worth to read it. If you have used LAB2 already, please write a comment about your experience with it.
Tuesday, March 9, 2010
"Your Own Laser Experiments"
Doing laser experiments at home are in most cases challenging due missing tools. Nevertheless some easy but still very interesting experiments can be done demonstrating fundamental phenomena. By chance I found a homepage which describes in detail and well explained some very interesting and easy to do experiments.The page is the EU-HOU project: “Hands on Universe, Europe. Bringing frontline interactive astronomy to the classroom” and has the goal of renewing the teaching of science and awaking the interest of science to the young generation. The page covers mainly experiments from astronomy but some nice optics experiments (important for astronomy) are presented too.
EU-HOU, startpage
Four easy laser optics experiments can be found here:
EU-HOU, Laser Experiments
EU-HOU, home-made spectroscope
They handle of the:
- “Refraction , or bent light”
- “Determination of the index of refraction by a laser pointer”
- “Eureka, Light is a wave”
- "A home-made spectroscope"

All the pictures are taken from the EU-HOU page. Note that the EU-HOU page is addressed for teachers but every pupil (high school) can do it too. And please,
It can cause serious irreparable eye damage! Hence, take care even with a laser pointer. Enjoy the experiments!
Tuesday, December 8, 2009
Modelling an artificial eye with a CCD camera: see how they see!
Figure 1: Scheme of the eye
In the image an schematic view of an eye is represented; in a very simple model, we can consider the eye as a system formed by a refractive surface, the cornea, and the lens. In a normal eye, the light is focused at the fovea and the image is well-defined. When a person suffers from myopia, light is focused before the fovea; when a person suffers from long-sight, image is formed after the fovea.
Now, how can it be modelled with a web camera? Well, basically the webcam is a CCD sensor with a lens. If we replace this lens by a 35mm focal length lens (typical value for a human eye) and a diaphragm (which will act as a pupil), we can build an artificial eye.
Once, the webcam is ready you can try how people see. Ask for example for a pair of glasses and place them immediately before the webcam. If the person who has lent you the glasses suffers from myopia, you will see a blurred image: this is how this person sees without glasses (or better said, the opposite to the way this person sees: it corresponds to the vision of a long-sighted person with the same gradation):
Tuesday, April 14, 2009
Michelson interferometer

Let's explain how it works: coherent light emitted from a source (for example, a laser or a sodium lamp) travels up to a beamsplitter (BS), a device capable of dividing a beam into two beams (it is basically a glass with one of its surfaces partially reflective). From there, one of the beams goes to a first mirror (M1) where it is reflected; the same happens to the second beam. In the beamsplitter they meet again and travel together to the observation screen. Notice that there is an adittional glass (the blue one in the figure) to compensate the paths (the first beam goes twice through the beamsplitter and the second one just once).
In the following film from the Celtic Mad Scientist you can learn how to build your own Michelson interferometer, as well as applications and a detailed description of the setup:
For students of advanced levels, you should notice that if the interferometer was perfectly align you would get the interference of two plane waves with the same propagation vector (as they should be pararell) and thus there should not be interference fringes! Obviously, it is not the case here: since it is not perfectly aligned, there is a slighty angle between the two beams that allows you to see the fringes.
As curiosity you should know that, together with Edward Morley, Abraham Michelson tried to demonstrate with this system the existence of the "ether" in 1887. In the 19th century, it was believed that the Earth was surronded by a gas called ether. Michelson and Morley wanted to measure the speed of the Earth with respect to the ether. This movement will produce a wind and, since the light propagated through the ether, the speed of light would be different depending on the propagation direction. In one of the interferometer arms, the light would propagate in the same direction as the wind, but in the other one would propagate against the wind and thus more slowly.
However, they did not find any differences; the "failure" of the experiment showed the non-existance of ether and the propagation of light in vacuum.
In this link, you can find an interactive movie where you can reproduce the experiment and in the AIP Center for History of Physics you can download the original article.
Sunday, April 12, 2009
How to measure the speed of light with a liquorice stick
Can you guess why the value you have calculated is the speed of light?
First of all, let's explain how the microwave oven works.
The oven acts as a cavity for the waves; thus, the waves are no longer travelling waves, but standing waves.
As you can see in the video, the amplitude remains zero at some points which are separated half wavelenght. For this reason, the stick is not burnt at these points.
Since the speed of light is the product of the frequency (given by the oven specifications) by the wavelength, which can be deduced from the distance between two non-burnt points, it is easy to get a good approximation for it.This experiment has been adapted from "Cuaderno de bitácora estalar"

