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Electromagnetic Radiation (Light)

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Presentation on theme: "Electromagnetic Radiation (Light)"— Presentation transcript:

1 Electromagnetic Radiation (Light)
Chapter 5 Electromagnetic Radiation (Light)

2 Radiation is also known as...
Light pure energy Electromagnetic Waves energy-carrying waves emitted by vibrating electrons Photons particles of light

3 What is light? Light can act either like a wave or like a particle
Particles of light are called photons

4 Waves A wave is a pattern of motion that can carry energy without carrying matter along with it

5 wave speed = wavelength x frequency
Properties of Waves Wavelength is the distance between two wave peaks Frequency is the number of times per second that a wave vibrates up and down wave speed = wavelength x frequency

6 Wavelength (λ) and Frequency (f)
wavelength x frequency = speed of light ~ 300,000,000m/s λf=c

7 Light: Electromagnetic Waves
A light wave is a vibration of electric and magnetic fields Light interacts with charged particles through these electric and magnetic fields

8 The Electromagnetic Spectrum
A range of light waves extending in wavelength from radio waves to gamma rays

9 The Electromagnetic Spectrum
Radio Waves Microwaves Infrared Visible Light Ultraviolet X-rays Gamma Rays Raging Martians Invaded Venus (Roy G. Biv ) Using X-rays and Gamma Rays mnemonic

10 What is the electromagnetic spectrum?

11 Thought Question The higher the photon energy…
the longer its wavelength. the shorter its wavelength. energy is independent of wavelength.

12 Why be a physicist in late 1800s ?
One scientist lamented Newton and Maxwell had done it all. Nothing was left to discover. All that remained was to repeat the experiments with greater and greater precision. But there were some curious problems with “classical physics”

13 Problems of Classical Physics
Spectra from atoms, cold and hot Blackbody radiation Photoelectric effect What is the structure of matter ?

14 Problem:The structure of matter
Thompson model of matter had negative electrons stuck in positive pudding. Rutherford alpha scattering experiment proved positive nucleus had most of the mass in small area. Positive particles repel other positive particles. NUCLEI SHOULDN’T EXIST a new more powerful force is required. Led to planetary model of atoms. Positive nucleus (protons and neutrons) had negative electrons in orbits around them.

15 More on Structure Problem
Charged particles have an electric field around them. Motion of a charged particle causes a disturbance in the field, a wave, i.e. radiation Orbiting electrons should radiate energy, spiral into the nucleus.

16 Spectra from atoms:The Problem
Positive charges repel other positive charges with inverse square law. Electrons in classical orbits would emit continuous spectra as they spiral into the nucleus. Atoms shouldn’t exist.

17 Kirchhoff In 1859 long before atomic structure was understood, Gustav Kirchhoff formulated three rules that describe the three types of spectra. p. 99

18 Kirchoff’s Laws for Spectra
Law I: Solids, liquids or dense gases radiate at all wavelengths, a continuous spectrum. Law II : A low density gas excited to emit light will do so at specific wavelengths, a bright line or emission spectra. Law III : If light from a continuous spectrum passes through a cool low density gas a dark line spectra will result. Line spectra are unique for each element !

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20 Kirchoff’s Laws for spectra

21 Kirchhoff’s 1st Law: continuous spectra
1st law: Solids, liquids or dense gases radiate at all wavelengths… we now know the light is radiated by thermal radiation which is sometimes called blackbody radiation

22 Properties of Thermal/Blackbody Radiation
Hotter objects emit more light at all frequencies per unit area. Hotter objects emit photons with a higher average energy. Remind students that the intensity is per area; larger objects can emit more total light even if they are cooler.

23 Blackbody Radiation The Problem: Attempts to explain BB radiation failed. Classical physics leads to an equation that fits for long wavelengths but has a term that results in increasing intensity as the wavelengths get short. This was called the ultraviolet (uv) catastrophe. Figure 6.6: Black body radiation from three bodies at different temperatures demonstrates that a hot body radiates more total energy and that the wavelength of maximum intensity is shorter for hotter objects. The hotter object here will look blue to our eyes, whereas the cooler object will look red.

24 Wien’s Law for blackbody radiators

25 Wien’s Law Figure 6.6: Black body radiation from three bodies at different temperatures demonstrates that a hot body radiates more total energy and that the wavelength of maximum intensity is shorter for hotter objects. The hotter object here will look blue to our eyes, whereas the cooler object will look red. l max =

26 Star Colors Reddish  coolest star Orange-ish Yellowish White
Bluish  hottest star

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28 Star Temperatures 3000 K 4000 K 5000 K 6000 K 7000 K 10,000 K 15,000 K

29 Total Energy from BB The area under the curve is the total energy emitted by the blackbody. Stefan-Boltzmann Law: E = sAT4, E is the energy emitted per second σ is a constant 5.67 X 10-8 J/m2sec/K4 T is the Kelvin (absolute) temperature of the object A is the area the energy is passing through.

30 Emission Spectrum Something first has to excite the atoms. The surface of a star or near by hot stars mayexcite nebula out to great distances.

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32 Horsehead Nebula

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34 Absorption Spectra A continuous spectrum passing through a cooler gas will remove (absorb) the same lines the hot gas emits. These are called absorption or dark line spectra.

35 Lab Absorption

36 Stellar Atmospheric Absorption

37 Solar Spectra

38 Next Problem: Photoelectric effect

39 Photoelectric effect:Experimental

40 Photoelectric effect Results: KE of the ejected electrons

41 Photoelectric effect: The Problem
Classical physics would predict the brighter the light the more energy the emitted electrons would have. Increasing the intensity gives more electrons, but they all have the same kinetic energy. Each metal has a different threshold wavelength. Below this threshold no electrons are emitted regardless of the intensity of the light. The energy depends linearly on the frequency. E= hf = hc/λ

42 What can we find out from the light from a distant source? A.
Summary so far: Temperature from BB peak: Wien’s Law 2. Total energy from the BB temperature: Stefan-Boltzmann Law 3. Composition: Hot gases, emission nebula Cooler gases, stellar atmospheres, nebula All are descriptive only, not understood until …

43 Problems resolved Unexplained events are due to either poor experiments or standing on the edge of a great discovery. The Birth of Modern Physics Max Planck (c 1900) explained BB radiation by applying discrete energy levels to the oscillators in a BB cavity, Planck’s constant, h. Einstein took Planck’s idea a “quantum leap” forward by saying the energy itself was emitted in packets of specific energy, photons. Energy given by E = hf. Light has particle properties too. [ This won him the Nobel prize]. It also explains spectra as well.

44 Atoms are mostly empty Bohr , Schrodinger and others developed “quantum mechanics” to describe the structure of matter. We still use the idea of orbitals with associated energy levels, but it’s better to call these probability distributions. Take a chemistry class. Figure 6.2: Magnifying a hydrogen atom by 1012 makes the nucleus the size of a grape seed and the diameter of the electron cloud about 4.5 times longer than a football field. The electron itself is still too small to see. If hydrogen nucleus were the size if a grape seed the first electron orbital would be out 225 yards away. Fig. 6-2, p. 94

45 Spectra explained,1 Quantum mechanics, uses particle and wave properties to explain structure of atoms. Electrons in energy levels do not emit energy. Only photons with the exact energy to match differences in energy levels interact, going or coming, with atoms. The lowest energy level is called the ground state. Higher levels are called excited states.

46 Energy Level Transitions
I’m Free The only allowed changes in energy are those corresponding to a transition between energy levels Not Allowed Allowed

47 Photon absorption Figure 6.5: An atom can absorb a photon only if the photon has the correct amount of energy. The excited atom is unstable and within a fraction of a second returns to a lower energy level, reradiating the photon in a random direction. The excited atom is unstable and within a fraction of a second returns to a lower energy level, reradiating the photon in a random direction.

48 Hydrogen Absorption Fig. 6-4, p. 96
Figure 6.4: A hydrogen atom can absorb only those photons that move the atom’s electron to one of the higher-energy orbits. Here three different photons are shown along with the change they would produce if they were absorbed. Fig. 6-4, p. 96

49 Spectra explained , 2

50 Hydrogen Energy levels
Transitions between levels lead to different series of spectra. To n=1 level Lyman series .. High energy we can’t see these. To n=2 Balmer series… These are what we see To n= 3 , Paschen series, in infrared. p. 100

51 Energy levels for different atoms
Increasing atomic number, more protons pulls the energy levels closer and we get more electrons too, Spectra become more complex. Figure 6.3: The electrons in atoms may occupy only certain, permitted orbits. Because different elements have different charges on their nuclei, the elements have different patterns of permitted orbits. Each element has its signature spectrum. Levels have limits on number of electrons in them (Pauli Exclusion Principle). Fig. 6-3, p. 95

52 Chemical Fingerprints
Each type of atom has a unique spectral fingerprint

53 Spectra,3 Bright line, emission spectra result from electron transitions to lower energy levels. Conservation of energy requires the energy to be carried away. Photons have energy E = DE =hf, DE is the energy difference between the levels in the atom. Dark line , absorption, spectra result when an electron is hit by a photon with energy matching a transition to a higher level. The electron jumps to a higher state. The energy is later emitted in either a single photon or a series of photons. Emission is in a random direction. This lowers the light intensity in the original direction.

54 Stellar Spectral Fig. 6-CO, p. 92

55 Solar Spectra Fraunhoffer in early 1800’s found 600 dark lines in solar spectra. We now know the source.

56 Doppler Effect The apparent change in wavelength or frequency of a wave when the source, observer, or both is in motion.

57 Everyday Doppler Effect : Sound
Figure 6.11: The Doppler effect. (b) The clanging bell on a moving fire truck produces sounds that move outward (black circles). An observer ahead of the truck hears the clangs closer together, while an observer behind the truck hears them farther apart. Figure 6.11: The Doppler effect. (b) The clanging bell on a moving fire truck produces sounds that move outward (black circles). An observer ahead of the truck hears the clangs closer together, while an observer behind the truck hears them farther apart.

58 Doppler Effect: Light Figure 6.11: The Doppler effect. (c) A moving source of light emits waves that move outward (black circles). An observer in front of the light source observes a shorter wavelength (a blue shift), and an observer behind the light source observes a longer wavelength (a red shift).

59 True Velocity Tangential Velocity Radar Radial Velocity

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61 Optical Doppler Shift Figure 6.11: The Doppler effect. (a) A blue shift appears in the spectrum of a star approaching Earth (top spectrum). A red shift appears in the spectrum of a star moving away from Earth (bottom spectrum). (The Observatories of the Carnegie Institution of Washington) Figure 6.11: The Doppler effect. (a) A blue shift appears in the spectrum of a star approaching Earth (top spectrum). A red shift appears in the spectrum of a star moving away from Earth (bottom spectrum). (The Observatories of the Carnegie Institution of Washington Fig. 6-11a, p. 106

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63 Radial Velocity from Doppler Data !!!!
= The ratio of the radial velocity to the speed of the wave is equal to the ratio of the shift in the wavelength to the original wavelength. Or Vr = Δλ c/ λ

64 What can we find out from the light from a distant source? B.
Summary so far: 1. Temperature from BB peak: Wien’s Law 2. Total energy from the BB temperature: Stefan-Boltzmann Law 3. Composition 4. Radial velocity Still more to come…..

65 How does light tell us the rotation rate of an object?
Different Doppler shifts from different sides of a rotating object spread out its spectral lines This figure from the book can give an introduction to the Doppler effect.

66 Spectrum of a Rotating Object
This figure from the book can give an introduction to the Doppler effect. Spectral lines are wider when an object rotates faster

67 Collisions cause shifts Higher pressure higher probability of a collision

68 Higher Temperatures also cause more broadening

69 Thin cool gas in nebula give sharp lines

70 Demonstrations for Lab
1.View light from a single slit or from a light bulb filament. Vary the voltage changing the temperature. Law I 2. Observe light from selected gas discharge tubes. Law II 3. Observe a solar spectrum by sunlight reflected off a cloud Law III

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