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An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics
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An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Dec 24, 2015

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Page 1: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

An Introduction to Astronomy

Part IX: The Sun, Our Star

Lambert E. Murray, Ph.D.

Professor of Physics

Page 2: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.
Page 3: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Our Sun

The Sun is a star – and as such, enables us to study stars up close (at least within 1 A.U.) Thus, understanding the Sun is the key to understanding the stars!

Our Sun is the principle energy source for our solar system. It supplies the energy on the Earth for our weather and for life itself. It also supplies the high-energy radiation which causes the aurora.

Page 4: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Size of the Sun

The Sun is roughly 100 times the diameter of the Earth – more than one million Earths could be dropped into the Sun, with room left over.

The density of the Sun is actually less than the Earth, about 1.4 g/cc, but

The mass of the Sun is about 700 times greater than the mass of all the rest of the solar system combined – about 333,000 times the Earth’s mass.

This mass basically controls the motion of all the other objects in the solar system.

Page 5: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

The Sun’s Atmosphere – That Part Visible to Us

The Sun’s atmosphere is divided into three separate parts:– Photosphere – the visible surface of the Sun.– Chromosphere – a pinkish surface layer of the

Sun’s atmosphere visible only during a total eclipse.

– Corona – the Sun’s outer atmosphere which extends great distances away from the Sun’s surface. This part of the Sun’s atmosphere is also only visible during a total eclipse.

Page 6: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

The Photosphere

This is the lowest of the three layers of the Sun’s atmosphere; it is the layer that determines the color of the Sun.

The limb of the Sun is the apparent edge of the Sun. (This term is applied to the edge of any object in space.)

A close-up of this surface shows features called granules.

Page 7: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Granulation Patterns on the Sun’s Surface

Page 8: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Granulation

The granulation patterns on the surface of the Sun are dynamic, changing in time like the boiling of water in a pan.

They are produced by convections currents in the Sun’s interior: heated areas rising from below the surface.– Doppler measurements confirm that the center of the

granules are rising, while the edges are falling.– Each granule is about 1000 km across, or about the size

of Texas.

Page 9: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Changing Granulation Patterns on the Sun: (The images were taken in 2 minutes intervals.)

Movie

Page 10: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Supergranulation

In addition to the smaller granules on the Sun’s surface, there appear to be large areas of the Sun’s surface (about the size of the Earth) which rise and fall together. These are called “supergranules”.

Page 11: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Convection in the surface layer of the Sun

Page 12: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

The Chromosphere

Page 13: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

The Chromosphere

The Chromosphere is visible only during a total eclipse of the Sun.

A close examination of the chromosphere at the limb of the Sun reveals “grass-like” features called spicules.

These spicules appear to encircle regions of supergranulation.

Page 14: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

The Limb

Page 15: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Spicules Outlining Supergranules

Page 16: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

The Corona

Page 17: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

The Corona

Visible only during a total eclipse, the corona is the nearly transparent outer atmosphere of the Sun.

It is composed of tenuous gases at extremely high temperatures (1-2 million Kelvin) – much hotter than the surface of the Sun.

The corona may extend millions of miles out into space.

Page 18: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Choronographs

For years, the only time scientists could study the chromosphere or the corona was during a total eclipse.

In recent years, the coronagraph has been developed. This instrument blocks out the disk of the Sun to allow the outer edge (the chromosphere) and the corona to be studied

The next several images were taken with a choronograph.

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The Dynamic Chorona

From these previous pictures, it should be clear that the corona is dynamic.

Coronal activity appears to be linked with the appearance of Sunspots.

The next image shows variations in coronal activity as correlated with sunspot activity.

Page 23: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

The Solar Corona During

Solar Maxima Solar Minima

Page 24: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Model of Sun’s Outer Atmosphere

Page 25: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

What causes the large temperature increase in the corona is not completely understood at present.

Some type of magnetic disturbance is the most likely explanation.

Page 26: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

The Corona and the Solar Wind

The Corona appears to be a continuous stream of particles being release from the Sun’s surface.

This “Solar Wind” is made up mostly of high-energy electrons and protons.

Millions of tons of matter each second is being spewed into interplanetary space.

This Solar Wind is also very dynamic and variable.

Page 27: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.
Page 28: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.
Page 29: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Sunspots and Solar Activity

During certain times the solar disk is completely devoid of apparent activity – this is the time of the quiet sun.

At other times, there appear to be magnetic “storms” that move across the Sun’s surface.

The severity and number of these storms varies greatly from time to time.

Page 30: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

The Solar Disk

Active Quiet

Page 31: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

The Solar Cycle

Sunspot activity has been monitored for several centuries.

The number of sunspots on the Sun’s surface appears to go through a cycle that has a period of approximately 11 years.

The Sunspot cycle is plotted in the next slide over a period of about 100 years and shows not only the number of sunspots, but their locations on the solar disk in the form of “butterfly” diagrams.

Page 32: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.
Page 33: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Long-Period Solar Cycles

• There appears to be another solar cycle superimposed upon the 11-year cycle, as seen on the next slide – notice the minimum every 100 years.

• The period from 1645 - 1715 when there were almost no visible sunspots and a dearth of any solar activity is known as the “Maunder minimum”.

• There is some evidence that there were very abnormal weather patterns during this time period – indicating a possible link between solar activity and the weather.

Page 34: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

The Maunder Minimum

Page 35: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

SunSpotRecord

Page 36: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Sunspots: A Closer Look

Sunspots look like dark blemishes on the solar disk. These areas are not really dark, however, they are just not as bright as the

surrounding areas.

Umbra

Penumbra

Page 37: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Groups of Sunspots

Sunspots often appear in groups – quite often in pairs.

These sunspot pairs appear to move on the Sun’s surface as the Sun rotates – gradually moving from higher latitudes toward the Solar equator.

Page 38: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.
Page 39: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Source of Sunspots

In 1908 George Hale discovered that sunspots were associated with intense magnetic fields – thousands of times larger than the average solar magnetic field.

These magnetic fields can be measured using the Zeeman effect – where spectral lines are split proportional to the strength of the magnetic field.

Page 40: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Zeeman Splitting at a Sunspot

Page 41: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Magnetic Polarization Studies The Zeeman effect also causes the light from these

strong magnetic field regions to be polarized. The polarization direction is associated with the

direction of the magnetic fields. A magnetogram, a photograph based upon this

polarization effect, is shown on the next page: – On this image one polarity is yellow, while the other is

purple.– The sunspots appear to occur in matching pairs of

opposite polarity– The polarity is reversed in opposite hemispheres and

remains the same over an 11-year cycle, then reverses!

Page 42: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

A Magnetogram of the Sun

Page 43: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

The 22-year Solar Cycle

Since the directions of the magnetic fields in the northern and southern hemisphere of the Sun reverse every 11-years, it appears that the 11-year sunspot cycle is actually a 22-year cycle.

The cycle of sunspot activity appears to be associated with a twisting of the Sun’s internal magnetic field lines.

Page 44: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Plages and Filaments

Associated with the Sunspots are other features on the Solar disk.

The next slide is an image of the Sun taken with an H-alpha filter (looking at the hydrogen emission line). You will see bright areas called plages, which are closely associated with sunspot activity, and dark snake-like features called filaments.

Page 45: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Filaments and Plages

Page 46: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Filaments and Prominences

The dark filament observed in the last slide is actually a stream of ionized gas trapped in the Sun’s magnetic field. These gases have been cooled, and are thus not as bright as the surface gases. When observed from above the Sun’s surface they appear darker than the rest of the surface. However, when observed from the side (above the edge of the Sun) they appear quite bright, and are called prominences.

Page 47: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Filament

Prominence

Page 48: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.
Page 49: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Solar Flares

Flares are the most violent events on the surface of the Sun.

They are usually associated with sunspot groups.

The material of a flare is heated to extremely high temperatures.

Large amounts of high-energy particles and radiation are emitted into space.

Page 50: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Active SUN 2/6/2000

large flare

Page 51: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Time Sequence of a Flare

Page 52: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Time sequence of eruptive prominence (~1½ hr intervals)

Page 53: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Large Flares can be Deadly

A Flare is a violent eruption from the surface which is usually over in about 20 minutes.

The x-rays and ultraviolet rays emitted from the flare arrive at the earth in about 8 minutes.

The highest energy particles streaming out from the Sun can reach the Earth within about 20 to 30 minutes but will reach a peak only after several hours or perhaps days.

An astronaut exposed in space to the high-energy particles from a large solar flare can literally be cooked.

Page 54: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Protection from Solar Events

Fortunately, the Earth is shielded from these high-energy events by the Earth’s magnetic field, which diverts the charged particles toward the poles, and by the atmosphere which absorbs much of the excess energy.

Page 55: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

The High-Energy Particles Follow the Sun’s Magnetic Field

Page 56: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Other Effects of Solar Flares

These high-energy bursts can disrupt radio communication on Earth

They increase auroral activity They may create power surges in electrical

power grids, burning out circuits.

Page 57: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

The Sun’s Interior

Page 58: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Solar Interior

Current solar models describe three regions inside the Sun– Core - where thermonuclear reactions power

the sun– Radiative zone - where photons carry energy

away from the core– Convective zone - where convection of gases

carries energy away from the core

Page 59: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Gravitational Attraction vs. Radiation Pressure

The material making up the Sun is being pulled toward the center by gravity.

Radiation pressure (the outward force of the photons and other elementary particles) is pushing the gases outward.

These two forces are in equilibrium inside the Sun.– If the radiation pressure were to decrease, the Sun

would collapse.– If the radiation pressure were to increase, the Sun would

expand.

Page 60: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Energy Source for Stars During the last 200 years, several different energy

sources for the Sun have been proposed. However, all fail to provide enough energy for the

Sun to have provided light to our solar system for the past 3-5 billion years except one: nuclear fusion.

Gravitational pressure of the Sun’s great mass causes the core to reach temperatures of 15 million Kelvins.

Under these conditions Hydrogen (H) can be fused together to make a heavier element Helium (He) liberating neutrinos and energy.

Page 61: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

Nuclear Fusion According to Einstein’s theory of relativity,

E = mc2

This equation indicates the possibility of converting mass into energy.

When hydrogen is converted into helium, only about 0.7% of the mass is converted into energy.

However, because c is so large, every gram of matter converted produces and amount of energy equivalent to that produced by 300,000 tons of coal.

The Sun must convert 600 million metric tons of hydrogen into helium every second to maintain its present luminosity.

However, there is enough hydrogen still in the Sun to provide energy for at least another 5 billion years!

Page 62: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.
Page 63: An Introduction to Astronomy Part IX: The Sun, Our Star Lambert E. Murray, Ph.D. Professor of Physics.

End of Part IX