photon

A photon is a scientific blog that deals with the various sciences and seeks a better world.

Sunday, February 2, 2020

How was the speed of light calculated?

please click subtitle icon below the video to turn on the English translation
This video is available in Arabic with English subtitles
How was the speed of light calculated?
What is the speed of light?
Galileo
Roemer’s Method
Fizeau’s Method
reference: PHYSICS for Scientists and Engineers with Modern Physics, Raymond A. Serway

Share:

Wednesday, January 29, 2020

where is the particle before the measurement?

where is the particle before the measurement?

Share:

Sunday, January 26, 2020

center of mass

center of mass

Share:

definition of rigid body

definition of rigid body
please click subtitle icon below the video to turn on the English translation

Share:

Thursday, July 25, 2019

Bohr's Principle of Complementarity

Bohr's Principle of Complementarity

Bohr was 'one of the intellectual giants of early quantum theory. His ideas and his personality were enormously influential. During the twenties and thirties, the Bohr Institute in Copenhagen (which was financially supported by the Carlsberg Brewery) became a haven for scientists who were developing the new physics. Bohr was not always receptive to quantum ideas; like many of his colleagues, he initially rejected Einstein's photons. But by 1925 the overwhelming experimental evidence that light actually has a dual nature had convinced him. So for the next several years, Bohr concentrated on the logical problem implied by this duality, which he considered the central mystery of the interpretation of quantum theory. Unlike many of his colleagues, Bohr emphasized the mathematical formalism of quantum mechanics. Like de Broglie, he considered it vital to reconcile the apparently contradictory aspects of quanta. Bohr's uneasy marriage of the wave and particle models was the Principle of Complementary. This principle entails two related ideas:
1-A complete description of the observed behavior of microscopic particles requires concepts and properties that are mutually exclusive .
2-The mutually exclusive aspects of quanta do not reveal themselves in the same observations.
The second point was Bohr's answer to the apparent paradox of wave-particle duality: There is no paradox. In a given observation, either quanta behave like waves or like particles.
How, you may wonder, could Bohr get away with this-eliminating a paradox by claiming that it does not exist because it cannot be observed? Well, he has slipped through a logical loophole provided by the limitation of quantum physics that quantum mechanics describes only observed phenomena. From this vantage point, the central question of wave-particle duality is not "can a thing be both a wave and a particle?" Rather, the question is "can a thing be observed behaving like a wave and a particle in the same measurement?" Bohr's answer is no: in a given observation, quantum particles exhibit either wave-like behavior (if we observe their propagation) or particle-like behavior (if we observe their interaction with matter). And, sure enough , no one has yet found an exception to this principle.
Notice that by restricting ourselves to observed phenomena, we are dodging the question, "what is the nature of the reality behind the phenomena?" Many quantum physicists answer, "there is no reality behind phenomena." But that is another story.

The source:
Michael A. Morrison - Understanding Quantum Physics.
By. Fady Tarek
Share:

De-Broglie's Law

De-Broglie's Law

If electromagnetic radiation consists of photons-localized clumps of energy-how can we explain phenomena such as diffraction and interference? If not, then why did Compton have to use classical collision theory to explain the scattering of x rays by metals? On the other hand, if electrons are particles, why do they produce an interference pattern at the detector in the double-slit experiment? The behavior of electrons and photons in these experiments seems provocatively similar---crazy, to be sure, but crazy in the same way. Are electrons and photons in some sense the same?
Einstein was deeply puzzled by this question until he noticed a possible answer in the doctoral thesis of a young French physicist. In 1924, Einstein wrote in a letter to his Dutch colleague Hendrik Lorentz (1853-1928) that the research of Prince Louis de Broglie (1892-1975) .....is the first feeble ray of light to illuminate this, the worst of our physical riddles." De Broglie's achievement was to synthesize the wave-like and particle-like aspects of microscopic matter. Although de Broglie seems to have only dimly understood the nature of quantum particles, and his rather nebulous physical models of quanta have since been superseded, the importance of his contribution has not diminished. It initiated the development of modem quantum mechanics.
In 1910 de Broglie began studying history at the University of Paris; soon, however, he switched to physics. His studies were interrupted in 1913 by a six-year stint in the French army, during which he and his brother Maurice worked on wireless telegraphy. Then in 1919 he returned to Paris for his doctoral research. From work on the x-ray spectra of heavy elements, de Broglie knew of photons and the Bohr model of atomic structure. And he was particularly intrigued by "Planck's mysterious quanta." So he set himself the task of "[uniting] the corpuscular and undulatory points of view and thus [penetrating] a bit into the real nature of quanta." In 1923, lightning struck. As de Broglie tells it:
As in my conversations with my brother we always arrived at the conclusion that in the case of x-rays one had [both] waves and corpuscles, thus suddenly-I cannot give the exact date when it happened, but it was certainly in the course of summer 1923-I got the idea that one had to extend this duality to the material particles, especially to electrons.
Thus did de Broglie come up with the idea of matter waves. This idea led him to the important notion that all microscopic material particles are characterized by a wavelength and a frequency, just like photons. Aesthetic considerations seem to have influenced de Broglie's thinking towards the idea of matter waves. He evidently felt that nature should be symmetrical, so if particles of light (photons) were to be associated with electromagnetic radiation, then so should waves of matter be associated with electrons. Simply stated, his hypothesis is this: There is associated with the motion of every material particle a "fictitious wave" that somehow guides the motion of its quantum of energy.
In spite of its rather vague character, this idea was remarkably successful. For example, using the methods of classical optics (such as Fermat's principle) to describe the propagation of quanta, de Broglie was able to explain how photons (and, for that matter, electrons) diffract and interfere: It is not the particles themselves but rather their "guide waves" that diffract and interfere. In de Broglie's words, "the fundamental bond which unites the two great principles of geometrical optics and of dynamics is thus fully brought to light." De Broglie proffered these ideas in his Ph.D. dissertation, which he wrote at age 31. His thesis did not fully convince his examiners, who were impressed but skeptical of the physical reality of de Broglie's matter waves. One examiner later wrote, "at the time of the defense of the thesis, I did not believe in the physical reality of the waves associated with the particles of matter. Rather, I regarded them as very interesting objects of imagination. Nevertheless, de Broglie passed.

De-Broglie's equation

De Broglie's equations for the wavelength and frequency of his matter waves are elegant and simple. Even their derivations are not complicated. In his seminal paper of 1923,
de Broglie began with light quanta-photons-so I'll first recap the derivation of the equation relating the wavelength and momentum of a photon and then press on to material particles.
The photon is a relativistic particle of rest mass mo = O. Hence the momentum p of a photon is related to its total energy E through the speed of light C as
To introduce the frequency v of the photon, we use Einstein's equation for the photon energy
to write Eq. (2.10) as
For a wave in free space, the wavelength is , so Eq. (2.12) becomes

The source:
Michael A. Morrison - Understanding Quantum Physics.
By. Fady Tarek
Share:

Wednesday, July 24, 2019

interference experiment of electrons

interference experiment of electrons

Our strategy in the double-slit experiment is to send electrons through a double-slit diaphragm and see how the intensity measured by the detector differs from the interference pattern formed by light. To implement this strategy, we must make a few modifications in the apparatus Young used when he performed this experiment with light. First we replace the light source with an electron gun-a device that produces a (nearly monoenergetic) beam of electrons of energy E. A heated tungsten wire, for example, produces a stream of electrons that we can accelerate to the desired velocity. Second, we replace the photographic plate with an electron detector: a device that counts the number of electrons that arrive in each square meter of unit area per sec. (Like the photographic plate used in Young's experiment, our electron detector measures the rate at which energy arrives at each point on the detector.) A screen covered with phosphor will do; when an electron arrives at the screen, it produces a spot.
What would we expect to see at the detector if the electrons were particles, subject to the same physical laws as, say, marbles? Imagine for a moment that we block one slit-say, the lower slit in Fig. 2.3-so that all electrons must come through the other, open slit. Most electrons that make it through the diaphragm will go straight through this slit, "piling up" at the detector directly opposite it. We therefore expect to see a maximum in the measured intensity opposite the upper slit. But some particles will scatter from the edges of this slit, so we expect some amount of spread in the pattern. A reasonable guess for the intensity for a beam of particles passing through this apparatus with only the upper slit open is the curve  sketched in Fig. 2.6a. The curve  should be obtained if only the lower slit is open.
What should happen when both slits are open? Well, if the electrons are indeed particles, then the measured intensity should be simply . This rather featureless curve is sketched in Fig. 2.6b. (Were you to scale the apparatus to macroscopic size and send through it a uniform beam of marbles-with, of course, a suitable detector this is what you would see.) But what we actually see when we run the experiment with electrons is altogether different.
The measured intensities in Fig. 2.7 clearly exhibit bands of alternating high and low intensity: an interference pattern, like the one formed by light (see Fig. 2.4). This observation seems to imply that the electrons are diffracted by the slits at the diaphragm and then interfere in the region between the diaphragm and the detector. We can even fit the measured intensity of the scattered electrons to the double-slit function  of Eq. (2.6) provided we assign to each electron (of mass m and energy E) a wavelength
But to a classical physicist, steeped in the idea that electrons are particles, Eq. (2.9) is nonsense!


The source:
Michael A. Morrison - Understanding Quantum Physics.
By. Fady Tarek
Share:

BTemplates.com