1The Nature of LightChapter FiveGuiding Questions1. How fast does light travel? How can this speed be measured?2. Why do we think light is a wave? What kind of wave is it?3. How is the light from an ordinary light bulb different from the light emitted by a neon sign?4. How can astronomers measure the temperatures of the Sun and stars?5. What is a photon? How does an understanding of photons help explain why ultraviolet light causes sunburns?6. How can astronomers tell what distant celestial objects are made of?7. What are atoms made of?8. How does the structure of atoms explain what kind of light those atoms can emit or absorb?9. How can we tell if a star is approaching us or receding from us?Determining the Speed of Light• Galileo tried unsuccessfully to determine the speed of light using an assistant with a lantern on a distant hilltop2Light travels through empty space at a speedof 300,000 km/s• In 1676, Danish astronomer Olaus Rømer discovered that the exact time of eclipses of Jupiter’s moons depended on the distance of Jupiter to Earth • This happens because it takes varying times for light to travel the varying distance between Earth and Jupiter• Using d=rt with a known distance and a measured time gave the speed (rate) of the light• In 1850 Fizeau and Foucalt also experimented with light by bouncing it off a rotating mirror and measuring time• The light returned to its source at a slightly different position because the mirror has moved during the time light was traveling• d=rt again gave cLight is electromagnetic radiationand is characterized by its wavelength (λ)3Wavelength and FrequencyThe Nature of Light• In the 1860s, the Scottish mathematician and physicist James Clerk Maxwell succeeded in describing all the basic properties of electricity and magnetism in four equations• This mathematical achievement demonstrated that electric and magnetic forces are really two aspects of the same phenomenon, which we now call electromagnetism• Because of its electric and magnetic properties, light is also called electromagnetic radiation• Visible light falls in the 400 to 700 nm range• Stars, galaxies and other objects emit light in all wavelengths4Three Temperature ScalesAn opaque object emits electromagnetic radiationaccording to its temperatureA person in infrared-color coded image-red is hottest5Wien’s law and the Stefan-Boltzmann law are useful tools for analyzing glowing objects like stars• A blackbody is a hypothetical object that is a perfect absorber of electromagnetic radiation at all wavelengths• Stars closely approximate the behavior of blackbodies, as do other hot, dense objects• The intensities of radiation emitted at various wavelengths by a blackbody at a given temperature are shown by a blackbody curveWien’s LawWien’s law states that the dominant wavelength at which a blackbody emits electromagnetic radiation is inversely proportional to the Kelvin temperature of the object6Stefan-Boltzmann Law• The Stefan-Boltzmann law states that a blackbody radiates electromagnetic waves with a total energy flux E directly proportional to the fourth power of the Kelvin temperature T of the object:E = σT4Light has properties of both waves and particles• Newton thought light was in the form of little packets of energycalled photons and subsequent experiments with blackbody radiation indicate it has particle-like properties• Young’s Double-Slit Experiment indicated light behaved as a wave• Light has a dual personality; it behaves as a stream of particlelike photons, but each photon has wavelike properties7Light, Photons and Planck• Planck’s law relates the energy of a photon to its frequency or wavelengthE = energy of a photonh = Planck’s constantc = speed of lightλ = wavelength of light• The value of the constant h in this equation, called Planck’s constant, has been shown in laboratory experiments to beh = 6.625 x 10–34J sPrelude to the Bohr Model of the Atom• The Photoelectric Effect– experiment explained by Einstein, but performed by others• What caused this strange result?• This is what Einstein won the Nobel Prize forChemists’ Observations8Each chemical element produces its own unique set of spectral linesKirchhoff’s Laws9Kirchoff’s First Spectral Law• Any hot body produces a continuous spectrum– if it’s hot enough it looks something like this– digitally like thisWavelengthIntensityKirchoff’s Second Spectral Law• Any gas to which energy is applied, either as heat or a high voltage, will produce an emission line spectrum like this– or digitally like thisWavelengthIntensityKirchoff’s Third Spectral Law• Any gas placed between a continuous spectrum source and the observer will produce a absorption line spectrum like this– or digitally like thisWavelengthIntensity10Astronomers’ Observations11An atom consists of a small, dense nucleussurrounded by electrons• An atom has a small dense nucleus composed of protons and neutrons• Rutherford’s experiments with alpha particles shot at gold foil helped determine the structure• The number of protons in an atom’s nucleus is the atomic number for that particular element • The same element may have different numbers of neutrons in its nucleus• These slightly different kinds of the same elements are called isotopes12Spectral lines are produced when an electron jumps from one energy level to another within an atom• The nucleus of an atom is surrounded by electrons that occupy only certain orbits or energy levels• When an electron jumps from one energy level to another, it emits or absorbs a photon of appropriate energy (and hence of a specific wavelength).• The spectral lines of a particular element correspond to the various electron transitions between energy levels in atoms of that element.• Bohr’s model of the atom correctly predicts the wavelengths of hydrogen’s spectral lines.13Bohr’s formula for hydrogen wavelengths1/λ = R x [ 1/N2–1/n2 ]N = number of inner orbitn = number of outer orbitR = Rydberg constant (1.097 X 107m-1)λ = wavelength of emitted or absorbed photonBalmer Lines in Star Spectrum14The wavelength of a spectral line is affected by therelative motion between the source and the observerDoppler Shifts• Red Shift: The object is moving away from the observer• Blue Shift: The object is moving towards the observerΔλ/λo= v/cΔλ = wavelength shiftλo= wavelength if source is not movingv =