Chapter 11 Gravity, Planetary Orbits, and the Hydrogen Atom.
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Transcript of Chapter 11 Gravity, Planetary Orbits, and the Hydrogen Atom.
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Chapter 11
Gravity, Planetary Orbits, and
the Hydrogen Atom
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Newton’s Law of Universal Gravitation Every particle in the Universe attracts every
other particle with a force that is directly proportional to the product of their masses and inversely proportional to the square of the distance between them
G is the universal gravitational constant and equals 6.673 x 10-11 Nm2 / kg2
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Law of Gravitation, cont This is an example of an inverse
square law The magnitude of the force varies as the
inverse square of the separation of the particles
The law can also be expressed in vector form
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Notation is the force exerted by particle 1 on
particle 2 The negative sign in the vector form of
the equation indicates that particle 2 is attracted toward particle 1
is the force exerted by particle 2 on particle 1
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More About Forces
The forces form a Newton’s
Third Law action-reaction pair Gravitation is a field force that
always exists between two particles, regardless of the medium between them
The force decreases rapidly as distance increases
A consequence of the inverse square law
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Active Figure AF_1101 gravitational force.swf
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G vs. g Always distinguish between G and g G is the universal gravitational constant
It is the same everywhere g is the acceleration due to gravity
g = 9.80 m/s2 at the surface of the Earth g will vary by location
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Gravitational Force Due to a Distribution of Mass The gravitational force exerted by a
finite-sized, spherically symmetric mass distribution on a particle outside the distribution is the same as if the entire mass of the distribution were concentrated at the center
For the Earth, this means
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Measuring G G was first measured
by Henry Cavendish in 1798
The apparatus shown here allowed the attractive force between two spheres to cause the rod to rotate
The mirror amplifies the motion
It was repeated for various masses
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Gravitational Field Use the mental representation of a field
A source mass creates a gravitational field throughout the space around it
A test mass located in the field experiences a gravitational force
The gravitational field is defined as
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Gravitational Field of the Earth Consider an object of mass m near the
earth’s surface The gravitational field at some point has
the value of the free fall acceleration
At the surface of the earth, r = RE and g = 9.80 m/s2
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Representations of the Gravitational Field
The gravitational field vectors in the vicinity of a uniform spherical mass
fig. a – the vectors vary in magnitude and direction The gravitational field vectors in a small region near the
earth’s surface fig. b – the vectors are uniform
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Structural Models In a structural model, we propose theoretical
structures in an attempt to understand the behavior of a system with which we cannot interact directly The system may be either much larger or much
smaller than our macroscopic world One early structural model was the Earth’s
place in the Universe The geocentric model and the heliocentric models
are both structural models
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Features of a Structural Model A description of the physical components of the
system A description of where the components are
located relative to one another and how they interact
A description of the time evolution of the system A description of the agreement between
predictions of the model and actual observations Possibly predictions of new effects, as well
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Kepler’s Laws, Introduction
Johannes Kepler was a German astronomer
He was Tycho Brahe’s assistant
Brahe was the last of the “naked eye” astronomers
Kepler analyzed Brahe’s data and formulated three laws of planetary motion
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Kepler’s Laws Kepler’s First Law
Each planet in the Solar System moves in an elliptical orbit with the Sun at one focus
Kepler’s Second Law The radius vector drawn from the Sun to a planet
sweeps out equal areas in equal time intervals Kepler’s Third Law
The square of the orbital period of any planet is proportional to the cube of the semimajor axis of the elliptical orbit
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Notes About Ellipses F1 and F2 are each a
focus of the ellipse They are located a
distance c from the center
The longest distance through the center is the major axis
a is the semimajor axis
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Notes About Ellipses, cont The shortest distance
through the center is the minor axis b is the semiminor axis
The eccentricity of the ellipse is defined as e = c /a For a circle, e = 0 The range of values of
the eccentricity for ellipses is 0 < e < 1
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Active Figure AF_1105 properties of ellipses.swf
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Notes About Ellipses, Planet Orbits The Sun is at one focus
Nothing is located at the other focus Aphelion is the point farthest away from the
Sun The distance for aphelion is a + c
For an orbit around the Earth, this point is called the apogee
Perihelion is the point nearest the Sun The distance for perihelion is a – c
For an orbit around the Earth, this point is called the perigee
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Kepler’s First Law A circular orbit is a special case of the
general elliptical orbits Is a direct result of the inverse square nature
of the gravitational force Elliptical (and circular) orbits are allowed for
bound objects A bound object repeatedly orbits the center An unbound object would pass by and not return
These objects could have paths that are parabolas and hyperbolas
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Orbit Examples Pluto has the
highest eccentricity of any planet (a) ePluto = 0.25
Halley’s comet has an orbit with high eccentricity (b) eHalley’s comet = 0.97
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Speed and Eccentricity AF_1107 elliptical orbits.swf
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Kepler’s Second Law
Is a consequence of conservation of angular momentum
The force produces no torque, so angular momentum is conserved
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Kepler’s Second Law, cont. Geometrically, in a
time dt, the radius vector r sweeps out the area dA, which is half the area of the parallelogram
Its displacement is given by
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Kepler’s Second Law, final Mathematically, we can say
The radius vector from the Sun to any planet sweeps out equal areas in equal times
The law applies to any central force, whether inverse-square or not
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Kepler’s Third Law Can be predicted
from the inverse square law
Start by assuming a circular orbit
The gravitational force supplies a centripetal force
Ks is a constant
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Kepler’s Third Law, cont This can be extended to an elliptical
orbit Replace r with a
Remember a is the semimajor axis
Ks is independent of the mass of the planet, and so is valid for any planet
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Kepler’s Third Law, final If an object is orbiting another object,
the value of K will depend on the object being orbited
For example, for the Moon around the Earth, KSun is replaced with KEarth
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Energy in Satellite Motion Consider an object of mass m moving
with a speed v in the vicinity of a massive object M M >> m We can assume M is at rest
The total energy of the two object system is E = K + Ug
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Energy, cont.
Since Ug goes to zero as r goes to infinity, the total energy becomes
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Energy, Circular Orbits For a bound system, E < 0 Total energy becomes
This shows the total energy must be negative for circular orbits
This also shows the kinetic energy of an object in a circular orbit is one-half the magnitude of the potential energy of the system
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Energy, Elliptical Orbits The total mechanical energy is also
negative in the case of elliptical orbits The total energy is
r is replaced with a, the semimajor axis
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Escape Speed from Earth An object of mass m is
projected upward from the Earth’s surface with an initial speed, vi
Use energy considerations to find the minimum value of the initial speed needed to allow the object to move infinitely far away from the Earth
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Escape Speed From Earth, cont This minimum speed is called the escape
speed
Note, vesc is independent of the mass of the object
The result is independent of the direction of the velocity and ignores air resistance
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Escape Speed, General
The Earth’s result can be extended to any planet
The table at right gives some escape speeds from various objects
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Escape Speed, Implications This explains why some planets have
atmospheres and others do not Lighter molecules have higher average
speeds and are more likely to reach escape speeds
This also explains the composition of the atmosphere
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Black Holes A black hole is the remains of a star
that has collapsed under its own gravitational force
The escape speed for a black hole is very large due to the concentration of a large mass into a sphere of very small radius If the escape speed exceeds the speed of
light, radiation cannot escape and it appears black
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Black Holes, cont The critical radius at
which the escape speed equals c is called the Schwarzschild radius, RS
The imaginary surface of a sphere with this radius is called the event horizon
This is the limit of how close you can approach the black hole and still escape
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Black Holes and Accretion Disks Although light from a black hole cannot
escape, light from events taking place near the black hole should be visible
If a binary star system has a black hole and a normal star, the material from the normal star can be pulled into the black hole
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Black Holes and Accretion Disks, cont This material forms
an accretion disk around the black hole
Friction among the particles in the disk transforms mechanical energy into internal energy
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Black Holes and Accretion Disks, final The orbital height of the material above
the event horizon decreases and the temperature rises
The high-temperature material emits radiation, extending well into the x-ray region
These x-rays are characteristics of black holes
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Black Holes at Centers of Galaxies There is evidence
that supermassive black holes exist at the centers of galaxies
Theory predicts jets of materials should be evident along the rotational axis of the black hole
An HST image of the galaxy M87. The jet of material in the right frame is thought to be evidence of a supermassive black hole at the galaxy’s center.
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Gravity Waves Gravity waves are ripples in space-time
caused by changes in a gravitational system The ripples may be caused by a black hole
forming from a collapsing star or other black holes
The Laser Interferometer Gravitational Wave Observatory (LIGO) is being built to try to detect gravitational waves
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Importance of the Hydrogen Atom A structural model can also be used to
describe a very small-scale system, the atom The hydrogen atom is the only atomic system
that can be solved exactly Much of what was learned about the
hydrogen atom, with its single electron, can be extended to such single-electron ions as He+ and Li2+
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Light From an Atom The electromagnetic waves emitted
from the atom can be used to investigate its structure and properties Our eyes are sensitive to visible light We can use the simplification model of a
wave to describe these emissions
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Wave Characteristics
The wavelength, , is the distance between two consecutive crests
A crest is where a maximum displacement occurs
The frequency, ƒ, is the number of waves in a second
The speed of the wave is c = ƒ
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Atomic Spectra A discrete line spectrum is observed
when a low-pressure gas is subjected to an electric discharge
Observation and analysis of these spectral lines is called emission spectroscopy
The simplest line spectrum is that for atomic hydrogen
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Uniqueness of Atomic Spectra Other atoms exhibit completely different
line spectra Because no two elements have the
same line spectrum, the phenomena represents a practical and sensitive technique for identifying the elements present in unknown samples
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Emission Spectra Examples
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Absorption Spectroscopy An absorption spectrum is obtained
by passing white light from a continuous source through a gas or a dilute solution of the element being analyzed
The absorption spectrum consists of a series of dark lines superimposed on the continuous spectrum of the light source
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Absorption Spectrum, Example
A practical example is the continuous spectrum emitted by the sun
The radiation must pass through the cooler gases of the solar atmosphere and through the Earth’s atmosphere
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Balmer Series
In 1885, Johann Balmer found an empirical equation that correctly predicted the four visible emission lines of hydrogen H is red, = 656.3 nm
H is green, = 486.1 nm
H is blue, = 434.1 nm
H is violet, = 410.2 nm
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Emission Spectrum of Hydrogen – Equation
The wavelengths of hydrogen’s spectral lines can be found from
RH is the Rydberg constant RH = 1.097 373 2 x 107 m-1
n is an integer, n = 3, 4, 5,… The spectral lines correspond to different values of n
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Niels Bohr 1885 – 1962 An active participant in
the early development of quantum mechanics
Headed the Institute for Advanced Studies in Copenhagen
Awarded the 1922 Nobel Prize in physics
For structure of atoms and the radiation emanating from them
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The Bohr Theory of Hydrogen In 1913 Bohr provided an explanation of
atomic spectra that includes some features of the currently accepted theory
His model includes both classical and non-classical ideas
He applied Planck’s ideas of quantized energy levels to orbiting electrons
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Bohr’s Assumptions for Hydrogen, 1
The electron moves in circular orbits around the proton under the electric force of attraction The force produces
the centripetal acceleration
Similar to the structural model of the Solar System
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Bohr’s Assumptions, 2 Only certain electron orbits are stable and these
are the only orbits in which the electron is found These are the orbits in which the atom does not emit
energy in the form of electromagnetic radiation Therefore, the energy of the atom remains constant
and classical mechanics can be used to describe the electron’s motion
This representation claims the centripetally accelerated electron does not emit energy and eventually spirals into the nucleus
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Bohr’s Assumptions, 3 Radiation is emitted by the atom when the
electron makes a transition from a more energetic initial state to a lower-energy orbit The transition cannot be treated classically The frequency emitted in the transition is related to the
change in the atom’s energy The frequency is independent of the frequency of the
electron’s orbital motion The frequency of the emitted radiation is given by Ei – Ef = hƒ h is Planck’s constant and equals 6.63 x 10-34 Js
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Bohr’s Assumptions, 4 The size of the allowed electron orbits is
determined by a condition imposed on the electron’s orbital angular momentum
The allowed orbits are those for which the electron’s orbital angular momentum about the nucleus is quantized and equal to an integral multiple of h h = h / 2
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Mathematics of Bohr’s Assumptions and Results Electron’s orbital angular momentum
mevr = nh where n = 1, 2, 3,… The total energy of the atom is
The total energy can also be expressed as
Note, the total energy is negative, indicating a bound electron-proton system
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Bohr Radius The radii of the Bohr orbits are quantized
This shows that the radii of the allowed orbits have discrete values—they are quantized
When n = 1, the orbit has the smallest radius, called the Bohr radius, ao
ao = 0.0529 nm
n is called a quantum number
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Radii and Energy of Orbits A general expression
for the radius of any orbit in a hydrogen atom is rn = n2ao
The energy of any orbit is
This becomes
En = - 13.606 eV/ n2
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Specific Energy Levels Only energies satisfying the previous
equation are allowed The lowest energy state is called the ground
state This corresponds to n = 1 with E = –13.606 eV
The ionization energy is the energy needed to completely remove the electron from the ground state in the atom The ionization energy for hydrogen is 13.6 eV
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Energy Level Diagram
Quantum numbers are given on the left and energies on the right
The uppermost level,
E = 0, represents the state for which the electron is removed from the atom
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Frequency of Emitted Photons The frequency of the photon emitted
when the electron makes a transition from an outer orbit to an inner orbit is
It is convenient to look at the wavelength instead
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Wavelength of Emitted Photons The wavelengths are found by
The value of RH from Bohr’s analysis is in excellent agreement with the experimental value
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Extension to Other Atoms Bohr extended his model for hydrogen
to other elements in which all but one electron had been removed
Bohr showed many lines observed in the Sun and several other stars could not be due to hydrogen They were correctly predicted by his theory
if attributed to singly ionized helium
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Orbits As a spacecraft fires its
engines, the exhausted fuel can be seen as doing work on the spacecraft-Earth orbit
Therefore, the system will have a higher energy
The spacecraft cannot be in a higher circular orbit, so it must have an elliptical orbit
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Orbits, cont. Larger amounts of energy will move the
spacecraft into orbits with larger semimajor axes
If the energy becomes positive, the spacecraft will escape from the earth
It will go into a hyperbolic path that will not bring it back to the earth
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Orbits, Final The spacecraft in orbit
around the earth can be considered to be in a circular orbit around the sun
Small perturbations will occur
These correspond to its motion around the earth
These are small compared with the radius of the orbit