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Essential Astrophysics

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Nguyễn Gia Hào

Academic year: 2023

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All example problems are solved to the approximate accuracy necessary to portray the basic result. It also includes discussions of stellar spectra, as well as the evolution of stars and their role in the origin of chemical elements.

Table 13.5 Physical properties of some novae . . . . . . . . . . . . . . . . . . 430 Table 13.6 Historical supernovae visible with the unaided eye
Table 13.5 Physical properties of some novae . . . . . . . . . . . . . . . . . . 430 Table 13.6 Historical supernovae visible with the unaided eye

What Do Astronomers and Astrophysicists Do?

Our Place on Earth

Longitude, denoted by the Greek letter k, of any point on the Earth's surface is the angle measured westward from the intersection of the prime meridian with the equator to the equatorial intersection of the longitude circle passing through the point (Figure 1.1). The length of the day and the period of rotation are the same for every place on Earth, and the speed of rotation around its axis depends on the location of the surface.

Location in the Sky

Precession results in a slow movement of the vernal equinox, producing a steady change in celestial coordinates. An observer can see only half of the celestial sphere—the half above the local horizon.

Fig. 1.2 Celestial coordinates Stars, galaxies, and other cosmic objects are placed on an imaginary celestial sphere
Fig. 1.2 Celestial coordinates Stars, galaxies, and other cosmic objects are placed on an imaginary celestial sphere

Measuring Angle and Size

The Sun's linear radius, denoted by R, can be determined from the Sun's angular diameter, denoted by h, using. By the way, the angular diameter of the Sun is about the same angle as that subtended by the thumb when viewed at arm's length.

The Locations of the Stars are Slowly Changing

The precessional movement of the Earth's axis of rotation is caused by the tidal action of the Moon and Sun on the rotating Earth. This movement of the Earth's rotation axis also causes a slow change in the celestial coordinates of any cosmic object.

Fig. 1.4 Precession The Earth’s rotation axis traces out a circle on the sky once every 26,000 years, sweeping out a cone with an angular radius of about 23.5°
Fig. 1.4 Precession The Earth’s rotation axis traces out a circle on the sky once every 26,000 years, sweeping out a cone with an angular radius of about 23.5°

What Time is It?

Terrestrial Time (TT) is the modern time standard used to measure the time of astronomical observations from the Earth's surface. This solar day is the interval between two consecutive passages of the Sun across the observer's meridian.

Telling Time by the Stars

The Prime Meridian is the local meridian of the old Royal Observatory in Greenwich, England. The local sidereal time is equal to zero when the vernal equinox or vernal equinox is on the local meridian.

Fig. 1.5 Sun time and star time The Sun reaches its highest point in the daytime sky, its culmination, at noon, and this happens every 24 h in a solar day
Fig. 1.5 Sun time and star time The Sun reaches its highest point in the daytime sky, its culmination, at noon, and this happens every 24 h in a solar day

Optical Telescopes Observe Visible Light

A second smaller lens called the eyepiece was used to magnify the image in the early refractors; later versions placed photographic or electronic detectors in the focal plane. The resolving power of a telescope operating at the wavelengths that we can see with our eyes, at a yellow wavelength of about 6910-7m, is about 0.124=DT00 when DT is in meters.

Fig. 1.6 Telescopes Light waves that fall on the Earth from a distant object are parallel to one another, and are focused to a point by the lens or mirror of a telescope
Fig. 1.6 Telescopes Light waves that fall on the Earth from a distant object are parallel to one another, and are focused to a point by the lens or mirror of a telescope

Telescopes that Detect Invisible Radiation

But an interferometer with radio telescopes placed on opposite sides of the Earth will have a datum out to twice the radius of the planet, or about 107 m. It is named after the English astronomer Sir William Herschel, the discoverer of the infrared spectrum and the planet Uranus, and his sister and colleague Caroline.

Fig. 1.7 Interferometer When incoming radiation approaches the Earth at an angle, the crests will arrive at two separated telescopes at slightly different times
Fig. 1.7 Interferometer When incoming radiation approaches the Earth at an angle, the crests will arrive at two separated telescopes at slightly different times

Units Used by Astronomers and Astrophysicists

This is the time it takes for radiation to travel from the Sun to the Earth. The orbital period of the Earth around the Sun is one year with a value.

Physical Constants

If the law of gravity is universal, applicable to all objects in the universe, then G must be independent of time, position, mass and nature of bodies. This constant appears in the description of thermal radiation (blackbody) and when describing the interaction of radiation with matter.

Electromagnetic Waves

Any electromagnetic wave, regardless of wavelength or frequency, travels through empty space at the speed of light, and this is the maximum speed possible (Focus 2.2). It is a change in the observed position of a star that depends on the ratio of the speed of the Earth and the speed of light.

Fig. 2.1 Electromagnetic waves All forms of radiation consist of electrical and magnetic fields that oscillate at right angles to each other and to the direction of travel
Fig. 2.1 Electromagnetic waves All forms of radiation consist of electrical and magnetic fields that oscillate at right angles to each other and to the direction of travel

The Electromagnetic Spectrum

Most of the sun's ultraviolet radiation is absorbed by our air, but prolonged exposure to the amount that reaches the ground can burn the skin. The visible spectrum that we see with our eyes is a very small part of the entire range of wavelengths.

Fig. 2.2 Electromagnetic spectrum Radiation from cosmic objects can be emitted at wavelengths from less than 10 -12 m to greater than 10 4 m, where m denotes meters
Fig. 2.2 Electromagnetic spectrum Radiation from cosmic objects can be emitted at wavelengths from less than 10 -12 m to greater than 10 4 m, where m denotes meters

Moving Perspectives

The unchanging speed of light was first demonstrated in the late 19th century by the American physicist Albert A. However, Michelson and Morley found that there was no detectable difference in the speed of light measured in the direction of the earth's motion or perpendicular to it. (Michelson and Morley1887).

Thermal (Blackbody) Radiation

The constant of proportionality between the frequency and energy of the radiation is now known as Planck's constant, denoted by a lowercase letter. This results in the Stefan-Boltzmann law in which the luminosity increases with the square of the radius and the fourth power of the effective temperature.

Fig. 2.3 Blackbody radiation The spectral plot of blackbody radiation intensity as a function of wavelength depends on the temperature of the gas emitting the radiation
Fig. 2.3 Blackbody radiation The spectral plot of blackbody radiation intensity as a function of wavelength depends on the temperature of the gas emitting the radiation

How Far Away is the Sun, and How Bright, Big and Hot is it?and Hot is it?

  • Distance of the Sun
  • How Big is the Sun?
  • The Unit of Energy
  • The Sun’s Luminosity
  • Taking the Sun’s Temperature
  • How Hot are the Planets?

The solar parallax, denoted byp, is half of the Sun's angular displacement as seen from opposite sides of the Earth. The solar constant indicates the amount of the Sun's radiation that reaches our planet.

Fig. 2.5 Distance to the Sun Values of the solar parallax obtained from measurements of the parallaxes of Venus, Mars, and the asteroid Eros between 1850 and 1970
Fig. 2.5 Distance to the Sun Values of the solar parallax obtained from measurements of the parallaxes of Venus, Mars, and the asteroid Eros between 1850 and 1970

The Energy of Light

As Tyndall pointed out, our environment would be much colder at night in the absence of the greenhouse effect, and the Earth might otherwise be covered in frost. The low energies of the radio photons cannot easily excite the atoms of our atmosphere, therefore radio photons pass easily through the air.

Radiation Scattering and Transfer

  • Why is the Sky Blue and the Sunsets Red?
  • Rayleigh Scattering
  • Thomson and Compton Scattering
  • Radiation Transfer

The scattering of radiation by a particle depends on the size, a, of the particle and the wavelength, k, of the radiation. The scattering is described by the Thomson scattering cross section, which is independent of the wavelength, or frequency, of the incident radiation.

Fig. 2.6 Looking through a cloud When an interstellar cloud happens to lie along the line of sight to a star, the observed temperature, denoted T O , can differ from the star’s temperature, abbreviated T S
Fig. 2.6 Looking through a cloud When an interstellar cloud happens to lie along the line of sight to a star, the observed temperature, denoted T O , can differ from the star’s temperature, abbreviated T S

Ceaseless, Repetitive Paths Across the Sky

The distance between the perihelion and aphelion is the major axis of the orbital ellipse. The semi-major axis of the Earth's elliptical orbit around the Sun is called the astronomical unit, abbreviated AU.

Fig. 3.1 Kepler’s first and second laws The German astronomer Johannes Kepler (1571–1630) published his first two laws of planetary orbital motion in 1609
Fig. 3.1 Kepler’s first and second laws The German astronomer Johannes Kepler (1571–1630) published his first two laws of planetary orbital motion in 1609

Universal Gravitational Attraction

It depends on the height of the object, its mass and the strength of the gravitational field it is in. The effective gravity of the Earth is reduced by its rotation, and this reduction is greatest at the equator.

Mass of the Sun

Therefore, the Earth's effective gravity decreases with rotation, but at most by about 3% and near the equator. The ratio of the mass of the Earth, ME, to the mass of the Sun, M, which is independent of G, is given by.

Tidal Effects .1 The Ocean Tides.1 The Ocean Tides

  • Tidal Locking into Synchronous Rotation
  • The Days are Getting Longer
  • The Moon is Moving Away from the Earth
  • A Planet’s Differential Gravitational Attraction Accounts for Planetary RingsAccounts for Planetary Rings

The moon creates most of the ocean waves, but the sun also contributes to the size and rhythm of the waves. Paleontologists have made indirect historical measurements of the Earth's rotation through studies of fossil corals.

Fig. 3.4 Cause of the Earth’s ocean tides The Moon’s gravitational attraction causes two tidal bulges in the Earth’s ocean water, one on the closest side to the Moon and one on the farthest side
Fig. 3.4 Cause of the Earth’s ocean tides The Moon’s gravitational attraction causes two tidal bulges in the Earth’s ocean water, one on the closest side to the Moon and one on the farthest side

What Causes Gravity?

Natário (2011) provides a good description of general relativity without calculus, while Will (1993) has discussed the observational verification of the theory. The amount of bending and change in stellar position predicted by Einstein's general theory of relativity was first confirmed in 1929 during a total solar eclipse.

Fig. 3.9 Sun bending starlight As the Earth orbits the Sun, an observer’s line of sight to a star or other cosmic object can pass near to the Sun or far from it
Fig. 3.9 Sun bending starlight As the Earth orbits the Sun, an observer’s line of sight to a star or other cosmic object can pass near to the Sun or far from it

Motion Opposes Gravity .1 Everything Moves.1 Everything Moves

Escape Speed

The escape velocity is independent of the small mass m and depends only on the distance Dof of the small mass and the value of the large mass M. At larger distances, the escape velocity becomes less because the strength of the gravitational force exerted by the large mass is less.

Orbital Motion

This makes sense, since the orbital velocity will decrease as the inverse square root of the distance. Orbital velocity is independent of the planet's mass, so the planetary region known as the Solar System is dominated by the Sun.

The Moving Stars .1 Are the Stars Moving?.1 Are the Stars Moving?

  • Components of Stellar Velocity
  • Proper Motion
  • Radial Velocity
  • Observed Proper Motions of Stars
  • Motions in Star Clusters
  • Runaway Stars

This exciting star moves around the center of the Milky Way in the opposite direction of the other nearby stars. The motions of the stars oppose the combined gravitational pull of all the stars, preventing them from clumping together and collapsing to the center of the cluster.

Fig. 4.1 A star moves The space velocity, V S of a star relative to an observer can be resolved into two mutually perpendicular components: (1) the radial velocity, V r , directed along the line of sight; and (2) the tangential velocity, V \ , which is per
Fig. 4.1 A star moves The space velocity, V S of a star relative to an observer can be resolved into two mutually perpendicular components: (1) the radial velocity, V r , directed along the line of sight; and (2) the tangential velocity, V \ , which is per

Cosmic Rotation

Unexpected Planetary Rotation

The ratio of the centrifugal acceleration at the equator to the gravitational acceleration at the equator is. The rotation periods of some planets and stars, including the Sun, are given in Table 4.5.

Fig. 4.7 Radar probes of Mercury A radio signal spreads out as a spherical wave, and Mercury intercepts a small fraction of them
Fig. 4.7 Radar probes of Mercury A radio signal spreads out as a spherical wave, and Mercury intercepts a small fraction of them

The Sun’s Differential Rotation

Each rotation of the Sun is then given a unique number called the Carrington rotation number, with rotation 1 beginning on November 9, 1853. This differential rotation continues to the bottom of the convective zone at 28.7 percent of the way down to the center of the Sun.

Table 4.6 Differential rotation of the Sun a Solar latitude
Table 4.6 Differential rotation of the Sun a Solar latitude

Stellar Rotation and Age

Elementary Constituents of Matter

Protons and neutrons together are called nucleons, because they are the two components of the atomic nucleus. The enlarged nucleus of the helium atom consists of two protons and two neutrons bound together by the strong nuclear force.

Table 5.1 Physical properties of electrons, protons, neutrons, and atoms a Electron
Table 5.1 Physical properties of electrons, protons, neutrons, and atoms a Electron

Heat, Temperature, and Speed .1 Where Does Heat Come From?.1 Where Does Heat Come From?

Thermal Velocity

The magnitude of the thermal velocity, which is the thermal velocity, increases with the temperature of the gas and decreases with increasing particle mass. Earth's average surface temperature is about 281 K, not hot enough for hydrogen to immediately escape from the surface.

Collisions

The Distribution of Speeds

The most likely velocity is the velocity associated with the highest point in the Maxwell distribution, and it is the velocity most likely to be present for any particle of mass m at temperature T. In other words, the Maxwell distribution function broadens and its peak shifts to higher rates as the temperature rises.

Molecules in Planetary Atmospheres

If the gas is hot, the molecules move at a greater speed and are more likely to escape the planet's gravity. Lewis (1941–), the composition of the planets and their atmospheres is closely related to their distance from the Sun (Lewis1974, 2004).

Gas Pressure

  • What Keeps Our Atmosphere Up?
  • The Ideal Gas Law
  • The Earth’s Sun-Layered Atmosphere
  • Pressure, Temperature, and Density Inside the Sun

That's because there is both a much higher temperature and a much higher particle density in the core of the sun. Beyond that, in the more tenuous outer parts of the sun, the temperature has dropped to 5,780 K.

Table 5.5 Range of cosmic pressures
Table 5.5 Range of cosmic pressures

Plasma .1 Ionized Gas.1 Ionized Gas

Plasma Oscillations and the Plasma Frequency

The plasma wavelength kP which corresponds to the plasma frequency mP in this layer of the ionosphere is. Radio transmissions from Earth at this long wavelength are reflected back to the ground, and cannot get through the ionosphere.

Atoms are Torn Apart into Plasma Within the Sun

We can infer the height and electron density of a particular layer in the ionosphere by sending radio signals up into the atmosphere at longer wavelengths or shorter frequencies. Longer wavelengths are used in radio communications around the Earth through reflection outside the ionosphere.

Sound Waves and Magnetic Waves .1 Sound Waves.1 Sound Waves

Magnetic Waves

The ion mass density provides the inertia of the oscillations and the magnetic field provides the restoring force. The ion motion and the magnetic field disturbances are in the same direction, both transverse to the direction of propagation.

Fig. 5.7 Alfvén waves The velocity amplitudes, or speeds, of Alfvén waves, expressed as transverse velocities of the oscillating magnetic field lines, versus distance, D, above the visible disk of the Sun or photosphere, given in units of the solar radius
Fig. 5.7 Alfvén waves The velocity amplitudes, or speeds, of Alfvén waves, expressed as transverse velocities of the oscillating magnetic field lines, versus distance, D, above the visible disk of the Sun or photosphere, given in units of the solar radius

What is the Sun Made Out Of?

The unique wavelengths of these lines coincide with the wavelengths of dark absorption lines in the Sun's spectrum. Earth is composed primarily of heavy elements that are relatively rare in the Sun and the rest of the universe.

Fig. 6.1 Absorption and emission lines The spectrum of a star or other cosmic object displays the intensity of its radiation as a function of wavelength, denoted by the Greek symbol lambda, k.
Fig. 6.1 Absorption and emission lines The spectrum of a star or other cosmic object displays the intensity of its radiation as a function of wavelength, denoted by the Greek symbol lambda, k.

Quantization of Atomic Systems

Bohr went a step further and quantized the energy of motion of electrons spinning in an atom. Both the energy and the orbital radius of an electron vary as the inverse square of the quantum number.

Fig. 6.6 Bohr atom In this model, proposed in 1913 by the Danish physicist Niels Bohr (1885–1962), a hydrogen atom’s one electron revolves around the hydrogen nucleus, a single proton, in well-defined orbits described by the integer n = 1, 2, 3, 4, 5, …
Fig. 6.6 Bohr atom In this model, proposed in 1913 by the Danish physicist Niels Bohr (1885–1962), a hydrogen atom’s one electron revolves around the hydrogen nucleus, a single proton, in well-defined orbits described by the integer n = 1, 2, 3, 4, 5, …

Some Atoms are Excited Out of Their Lowest-Energy Ground StateGround State

Under conditions of local thermodynamic equilibrium, the ratio of the number of atoms at two different energies depends on their energy difference divided by the temperature. The degeneracy of a level is the number of quantum states with the energy of that level.

Ionization and Element Abundance in the Sun and Other Starsand Other Stars

Fowler and Edward Milne then showed that the number of atoms or ions responsible for the formation of a spectral line can be estimated from the intensity of the line when Table 6.5 Ionization potentials for various degrees of ionization of the most common atoms in the cosmos is shown. Not even prominent astronomers of the time thought that hydrogen was the main component of the Sun and other stars.

Wavelengths and Shapes of Spectral Lines .1 Radial Motion Produces a Wavelength Shift.1 Radial Motion Produces a Wavelength Shift

Gambar

Fig. 1.4 Precession The Earth’s rotation axis traces out a circle on the sky once every 26,000 years, sweeping out a cone with an angular radius of about 23.5°
Fig. 1.5 Sun time and star time The Sun reaches its highest point in the daytime sky, its culmination, at noon, and this happens every 24 h in a solar day
Fig. 1.6 Telescopes Light waves that fall on the Earth from a distant object are parallel to one another, and are focused to a point by the lens or mirror of a telescope
Fig. 2.1 Electromagnetic waves All forms of radiation consist of electrical and magnetic fields that oscillate at right angles to each other and to the direction of travel
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