International Conference on Teaching Physics Innovatively New Learning Environments and Methods in Physics Education ELTE University, Faculty of Science, Budapest, Hungary 17-19 August 2015.
The beautiful rainbow International Conference on Teaching Physics - - PowerPoint PPT Presentation
The beautiful rainbow International Conference on Teaching Physics - - PowerPoint PPT Presentation
Jzsef Cserti Etvs University, Faculty of Science, Department of Physics of Complex Systems The beautiful rainbow International Conference on Teaching Physics Innovatively New Learning Environments and Methods in Physics Education ELTE
Primary and secondary rainbow
Photograph: Ákos Horváth
Primary and secondary rainbow
Photograph: László Grób Photograph: Balázs Gyüre Photograph: J. Cs.
The house where Newton grew up
Woolsthorpe by Colsterworth, Woolsthorpe Manor, UK
More rainbows
Photograph: Géza Gáspárdy Triple Rainbows
Supernumerary arcs
Atmospheric Optics http://www.atoptics.co.uk/
Short history before Descartes
(not complete) Aristotle (384 – 322 BC): an unusual kind of reflection of sunlight from clouds Alexander of Aphrodisias (fl. 200 AD): Alexander's dark band Roger Bacon (1266): the first measurment of the angle, 42 degrees Theodoric of Freiberg (German monk, 1304): first experiment with a spherical flask filled with water Rene Descartes (1637): Geometrical optics
Descartes' 1637 treatise, Discourse on Method
Rene Descartes (1596- 1650)
Snell's law
(also known as the Snell–Descartes law
- r the law of refraction)
Willebrord Snellius (born Willebrord Snel van Royen) in Leiden (1580- 1626) plane of the interface
Snell's law
(also known as the Snell–Descartes law
- r the law of refraction)
Willebrord Snellius (born Willebrord Snel van Royen) in Leiden (1580- 1626) plane of the interface
Snell's law
(also known as the Snell–Descartes law
- r the law of refraction)
Willebrord Snellius (born Willebrord Snel van Royen) in Leiden (1580- 1626) plane of the interface
Classification of the rays inside the sphere
primary rainbow secondary rainbow p is the number of chords the ray makes inside the sphere
Incident light Incident light Incident light Incident light
p=0 p=1 p=2 p=3
Role of the impact parameter
impact parameter The impact parameter is the distance of an incident ray from the central axis of the droplet. incident light incident light incident light incident light
p=3 p=4 p=5 p=7
Dispersion
incident white light
Each color of light has its own rainbow angle. Each rainbows slightly displaced from the next.
The refractive index depends on the frequency (color) of the light.
incident white light
p=2 p=3
Role of the impact parameter and the dispersion
incident light incident light incident light
p=17 p=17 p=17
Primary rainbow
incident light
Parallel incident light, one reflection inside the droplet, p=2 p=2 p=2
Primary rainbow
incident light
Parallel incident light, one reflection inside the droplet, p=2 p=2 p=2 p=2
Secondary and higher order rainbow
p=3 or p>3
incident
light
secondary rainbow p=4 p=3
p=3
Descartes' Theory
Geometrical optics α α α β β β β R ρ P α−β 180 −2β
Descartes' Theory
Scattering angle as a function of the impact parameter Scattering angles have an extreme value as a function of the impact parameter Alexander's dark band
0.2 0.4 0.6 0.8 1 b 45 90 135 180
p=0 p=3 p=1 p=2
Cartesian ray
Caustics caustic
Cartesian ray for different colors
primary rainbow secondary rainbow
incident light incident light
Higher order rainbows
incident light Observer
- H. Moyses Nussenzveig: The Theory of the Rainbow, Scientific American, Vol. 236, p. 116 (1977)
Summary
(Geometrical Optics)
Beyond the Geometrical Optics
Rainbow and the wave nature of light Airy's theory, the supernumerary arcs
B
2
B
1
A
2
A
1
C
2
C
1
P B D D’ B’ A’ A
1
P
P’(u,v)
u v
O A’ B’ R Q
θd
- G. B. Airy: On the intensity of light in the neighbourhood of a caustics,
Transactions of the Cambridge Philosophical Society, 6 379 (1838)
The shape of the initial wavefront AB changes with time caustic
George Biddell Airy (1801-1892) Observer
Interference of light starting from the wavefront A' B'
Supernumerary arcs
Airy's theory
- G. B. Airy: On the intensity of light in the neighbourhood of a caustics,
Transactions of the Cambridge Philosophical Society, 6 379 (1838) George Biddell Airy (1801-1892)
- 2.5
- 2
- 1.5
- 1
- 0.5
0.5 1
- 2.5
- 2
- 1.5
- 1
- 0.5
0.5 1
D i r e c t i
- n
s
- f
t h e s u p e r n u m e r a r y a r c s
Computer simulation of the supernumerary arcs
Experiment
Supernumerary arcs Airy's theory
Andrásné Hunh, Eötvös University, Budapest 2005.
154 154.2 154.4 0.2 0.4 0.6 0.8 1 int water droplet Laser Computer Mirror Detector stepper motor
Intensity
Experiment Airy's theory
primary rainbow Supernumerary arcs
Glass (n=1.467), R = 5.25 mm laser ( = 650 nm), kR = 50749
Exact description: the Mie's theory
Gustav Mie: Beitrage zur Optik trüber Medien, speziell kolloidaler Metallösungen,
- Ann. Phys., Leipzig 25, 377-445 (1908).
- M. Born and E. Wolf: Principles of Optics, Pergamon Press, New York, 1989 (6th eds.).
Ludwig V. Lorenz, 1890 Peter J. W. Debey, 1909
James Clerk Maxwell: On the Physical Lines of Force (1862)
Light = Electromagnetic field as a solution of the Maxwell's equations Rainbow = Scattering of an electromagnetic plane wave by a homogeneous dielectric sphere Helmholtz's equation:
E or the B field
Solution: Infinite series, can be treated efficiently only numerically Quantum mechanics: Scattering by potential well
Experiment and the Mie's theory
Andrásné Hunh, Eötvös University, Budapest 2005.
137 137.5 138 138.5 0.2 0.4 0.6 0.8 1
int.
θ
primary rainbow
Experiment Mie's theory
Supernumerary arcs Intensity Descartes' theory
Water (n=1.33), R = 1.82 mm laser ( = 650 nm), kR = 17583
Rainbow related optical phenomena: Corona
Corona = diffraction of light by small particles
http://www.atoptics.co.uk/droplets/corona.htm
Rings around the Sun
(black spot: shield the sun not to damage eyesight
Ring around the Sun due to volcanic ash The Eruption of Krakatoa 1883 Corona around the Moon
Imaged by Richard Fleet (Glows, Bows & Haloes) in Wiltshire, England during the summer of 2003
Rainbow related optical phenomena: Glory
Glory = a large angle (close to 180º ) scattering of light by a water droplet
http://www.atoptics.co.uk/droplets/glory.htm Photograph: Péter Vankó Photograph: Géza Király
Glories can be seen on mountains and hillsides, from aircraft, and is directly opposite the Sun
Photograph: Imre Derényi incident light back scattered light surface wave
Some references
Atmospheric Optics: http://www.atoptics.co.uk/ http://www.phy.ntnu.edu.tw/java/Rainbow/rainbow.html Raymond L. Lee, Jr., and Alistair B. Fraser: The Rainbow Bridge, Rainbows in Art, Myth, and Science, Penn State University Press; 1st edition (July 2001) http://www.usna.edu/Users/oceano/raylee/RainbowBridge/Chapter_8.html
- H. Moyses Nussenzveig: The Theory of the Rainbow, Scientific American,
- Vol. 236, p. 116 (1977)
John A. Adam: The mathematical physics of rainbows and glories, Physics Reports 356, 229–365 (2002) Philip Laven, Geneva, Switzerland: Freely available MiePlot computer program (Microsoft Windows) for Mie theory, http://www.philiplaven.com/
My works (Hungarian): A szivárvány fizikája, Fizikai Szemle 2005. év szeptemberi, októberi és decemberi számában Fizikus szemmel a szivárványról, Fizikai Szemle 2006. év szeptemberi számában a Mindentudás az Iskolában rovatában A szivárvány fizikai alapjai, T ermészet Világa 2007. év májusi és júniusi számában,
- 202. és 258. oldal
Acknowledgement
Gyula Dávid, T amás Geszti, Péter Gnädig, Ottó Haiman, Gábor Horváth, Andrásné Huhn, Krisztián Kis-Szabó, András Pályi, Péter Pollner, Géza Tichy, T amás Weidinger, and Philip Laven
Waterfall at Jajce by Tivadar Kosztka Csontváry