Title: This Set of Slides
1This Set of Slides
- This set of slides deals with the nature of
light, how its created, some ways that its used
in astronomy. - Units covered 21, 22, 23, 24 and 25.
2Light
- In Astronomy, it is far too difficult to visit
stars and most planets in person. - Astronomers primary tool in learning about the
universe is from the electromagnetic radiation,
or light, that we can detect. - To understand how astronomers know what they
know, you must understand some things about
electromagnetic radiation - light.
3The Nature of Light
- Light is radiant energy.
- Travels very fast 300,000 km/sec,
- 186,000 miles/sec
- Has a dual nature - Can be described either as a
wave or as a particle traveling through space.
- As a wave
- A disturbance in an electric field creates a
magnetic field, which in turn creates an electric
field, and so on, a self-propagating
electromagnetic wave. - Light waves can constructively or destructively
interfere. - The color of light is determined by its
frequency. - The energy is also determined by frequency.
- As a particle
- Particles of light (photons) travel through
space. - These photons have very specific energies, that
is, light is quantized. - Photons strike your eye (or other sensors) like
very small, massless balls (maybe bbs), and
are detected.
4Light as a Wave Versus Mechanical Waves
- Wave transfer of energy without the transfer of
matter. - Wave phenomena refraction, diffraction,
constructive and destructive interference,
superpositioning, Doppler shift. - Measurable wave characteristics amplitude,
wavelength, frequency, period. - Mechanical Waves water, sound must have some
physical matter a medium in which to exist
and travel. - Light exhibits all wave phenomena and has all the
measurable wave characteristics (as a mechanical
wave). - BUT, light does not require any physical matter
for its transfer. Light can exist and travel
through the vacuum of space.
5Wavelength
- The colors we see are determined by the
wavelength of light. - Wavelength is the distance between successive
crests (or troughs) in an electromagnetic wave. - This is very similar to the distance between the
crests in ocean waves. - We denote the wavelength of light by the symbol ?.
- Wavelengths of visible light are very small.
- Red light has a wavelength of 7?10-7 meters, or
700 nanometers (nm). - Violet light has a wavelength of 4?10-7 meters,
or 400 nm. - Colors in between red and violet (remember ROY G
BIV?) have intermediate wavelengths.
6Frequency
- Sometimes it is more convenient to talk about
light in terms of frequency, or how fast
successive crests pass by a given point. - You can think of frequency as a measure of how
fast you bob up and down as the waves pass by. - Frequency has units of Hz (hertz), and is denoted
by the symbol ?. 1 Hz 1 cycle/sec. - Long wavelength light has a low frequency, and
short wavelength light has a high frequency.
- Frequency and wavelength are related by
Where c is the speed of light.
7White Light
- Light from the Sun arrives with nearly all
wavelengths, and we perceive this mixture of
colors as white. - Newton demonstrated that white light could be
split into its component colors with a prism, and
then recombined into white light with a lens.
8The Electromagnetic Spectrum I
- There is much more to light than just visible
light, the light that humans can see. - Radio waves have very long wavelengths, as much
as a meter and more. - Microwaves (like the ones we cook with) are at
the upper end of the radio part of the spectrum. - Infrared wavelengths are longer in wavelength
than visible light.
9The Electromagnetic Spectrum II
- Above the visible
- Ultraviolet waves are shorter in wavelength than
visible waves. These included the waves that tan
or burn us. - X-rays come mostly from stellar sources in
nature, and can penetrate many materials, like
skin, muscle and bone. - Gamma rays have the shortest wavelengths.
10Energy Carried by Photons
- A photon carries energy with it that is related
to its wavelength or frequency - From this we see that long wavelength (low
frequency) photons carry less energy than short
wavelength (high frequency) ones. This is why UV
waves give us a sunburn, and X-rays let us look
through skin and muscles.
11The Nature of Matter
- An atom has a nucleus at its center containing
protons and neutrons. - Outside of the nucleus, electrons move in
clouds called orbitals. - Electrons can also be described using wave or
particle models. - Electron orbitals are quantized that is, they
exist only at very specific energies. - The lowest energy orbital is called the ground
state.
- To move an electron from one orbital to the next
higher one, a specific amount of energy must be
added. Likewise, a specific amount of energy
must be released for an electron to move to a
lower orbital. - These are called electronic transitions.
12 Some Quantum versus Classical Mechanics
- An early (circa 1900) atomic model was equivalent
to a planetary model the nucleus was considered
to be like the Sun with the planet-like electrons
in orbits. - This model didnt last long.
- An object (planet, moon, artificial satellite,
space station) can be in orbit at any level as
long as the speed is right. - An electron in an atom can not be in any orbit
but only in very well-defined orbital levels. - An electron moves from one orbital to another
without actually passing anywhere in-between!
Another oddity of quantum mechanics!
13The Chemical Elements
- The number of protons (atomic number) in a
nucleus determines what element a substance is. - An atom that is neutrally charged has a number of
electrons equal to the number of protons. - The electron orbitals are different for each
element, and the energy differences between the
orbitals are unique as well. - This means that if we can detect the energy
emitted or absorbed by an atom during an
electronic transition, we can tell what element
the atom belongs to, even from millions of light
years away!
14Absorption
- If a photon of exactly the right energy (equal to
the energy difference between orbitals) strikes
an electron, that electron will absorb the photon
and move into the higher orbital. - The atom is now in an excited state.
- If the photon energy doesnt match any of the
orbital-energy differences it can not be
absorbed it will pass through. We say the
element is transparent to those frequencies or
colors.
- This process is called absorption.
- If the electron gains enough energy to leave the
atom entirely, we say the atom is now ionized, or
is an ion.
15Emission
- If an electron drops from one orbital to a lower
one, it must emit a photon with the same amount
of energy as the orbital-energy difference. - This is called emission.
16Emission Spectra
- Imagine that we have hot hydrogen gas.
- Collisions among the hydrogen atoms cause
electrons to jump up to higher orbitals, or
energy levels. - Electrons can jump back to lower levels, and emit
a photon of energy h x f. - If the electron falls from orbital 3 to orbital
2, the emitted photon will have a wavelength of
656 nm. - If the electron falls from orbital 4 to orbital
2, the emitted photon will have a wavelength of
486 nm.
- We can monitor the light emitted, and measure the
amount of light of each wavelength we see. If we
graph this data, well see an emission spectrum.
17Seeing Spectra
- Seeing the Suns spectrum is not difficult.
- A narrow slit only lets a little light pass.
- Either a grating or a prism splits the light into
its component colors. - If we look closely at the spectrum, we can see
dark lines. These correspond to wavelengths of
light that were absorbed.
18Emission spectrum of hydrogen
- This spectrum is unique to hydrogen.
- If we were looking at a hot cloud of interstellar
gas in space, and saw these lines, we would know
the cloud contained hydrogen.
19Different atom, different spectrum!
- Every element has its own spectrum. Note the
differences between hydrogen and helium spectra
below.
A spectrum is like a chemical fingerprint!
20Absorption Spectra
- What if we had a cloud of cool hydrogen gas
between us and a star? - Photons of energies that correspond to the
electronic transitions in hydrogen will be
absorbed by electrons in the gas. - The light from those photons is effectively
removed from the spectrum. - The spectrum will have dark lines where the
missing light would be. - This is an absorption spectrum.
- Also unique for each element.
21Types of Spectra - Summary
- If the source emits light that is continuous,
and all colors are present, we say that this is a
continuous spectrum. - If the molecules in the gas are well-separated
and moving rapidly (have a high temperature), the
atoms will emit characteristic frequencies of
light. This is an emission-line spectrum. - If the molecules of gas are well-separated, but
cool, they will absorb light of a characteristic
frequency as it passes through. This is an
absorption line spectrum.
22Spectra of Astronomical Objects
23Measuring Temperature
- It is useful to think of temperature in a
slightly different way than we are accustomed to. - Temperature is a measure of the motion of atoms
in an object. - Objects with low temperatures have atoms that are
not moving much. - Objects with high temperatures have atoms that
are moving around very rapidly. - The Kelvin temperature scale was designed to
reflect this - 0 ? K is absolute zero the atoms in an object
are not moving at all.
24The Blackbody Spectrum
- As an object (piece of iron for example, or the
gas in a star) is heated, the atoms in it start
to move faster and faster. - When they collide, they emit photons with energy
proportional to how hard they hit - Some collide lightly, and produce long-wavelength
radiation. - Some collide very hard, and produce
short-wavelength radiation. - Most are somewhere in between.
- As the body gets hotter, the number of collisions
increase, and the number of hard collisions
increase.
Gentle collisions
Hard collisions
25Results of More Collisions
- Additional collisions mean that more photons are
emitted, so the object gets brighter. - Additional hard collisions means that more
photons of higher energy are emitted, so the
object appears to shift in color from red, to
orange, to yellow, and so on. - Of course we have physical laws to describe these
effects.
26Wiens Law and the Stefan-Boltzmann Law
- Wiens Law
- Hotter bodies emit more strongly at shorter
wavelengths. The hotter it is, the shorter the
wavelengths.
- SB Law
- The luminosity of a hot body rises rapidly with
temperature.
27Taking the Temperature of Astronomical Objects
- Wiens Law lets us estimate the temperatures of
stars easily and fairly accurately. - We just need to measure the wavelength (?max) at
which the star emits the most photons. - Then,
28The Stefan-Boltzmann Law
- If we know an objects temperature (T), we can
calculate how much energy the object is emitting
using the SB law - ? is the Stefan-Boltzmann constant, and is equal
to 5.67?10-8 Watts/m2/K4 - The Sun puts out 64 million watts per square
meter lots of energy!
29The Effect of Distance on Light
- Light from a distant source seems very dim. Why?
- Is it because the photons are losing energy?
- No the light is simply spreading out as it
travels from its source to its destination. - The farther from the source you are, the dimmer
the light seems. - The objects brightness, or the amount of light
received from a source, decreases with increased
distance. The relationship is mathematical.
30Doppler Shift in Sound
- As the car passes, the sound shifts to lower
pitch due to the longer wavelengths. - Police radar guns work on the same principle.
The waves reflected off the car will be shifted
by an amount that corresponds to the cars speed.
- You have experienced the Doppler shift in sound.
- Standing on the sidewalk, listening as cars go
past. - As a car approaches, the sound from the car seems
to have a higher pitch this is due to shorter
wavelengths.
31Doppler Shift in Light
- If an object emitting light is moving toward you,
the light you see will be shifted to shorter
wavelengths toward the blue end of the
spectrum. We say the light is blue-shifted. - Likewise, if the object is moving away from you,
the light will be red-shifted. - If we detect a wavelength shift of ?? away from
the expected wavelength ?, the radial
(line-of-sight) velocity of the object is