1 Lecture 13 How Stars Work 2 The Sun’s Magnetic Field • Magnetic fields apply a force on charged particles that pushes them along the direction of the field lines. • The charged particles in the ionized gas also push back on the magnetic field, altering its shape. • Magnetic fields appear to play an important role in the “storms” we see on the Sun’s surface. Chapter 15 (Sun) Chapter 16 OWL #3 is open Due 4/3/08 3 Twisting Magnetic Fields 4 PRS: Sunspots Sunspots are dark because 1. They are cool relative to the gas around them. 2. They contain 10 times as much iron as surrounding regions. 3. Nuclear reactions occur in them more slowly than in the surrounding gas. 4. Clouds in the cool corona block our view of the hot photosphere. 5. The gas within them is too hot to emit any light. The Sun’s differential rotation “winds up” the magnetic field, like twisting a rubber band 5 Sunspots • Cooler regions in Sun’s photosphere—still hot! • Magnetic fields alter atomic energy levels slightly • Magnetic fields in sunspots can be measured spectroscopically. Zeeman splitting 6 Sunspot Structure • The strong magnetic field should push the sunspot apart. • Like a storm on Earth, the cool region draws in gas, which drags along magnetic field. • The strong, tangled magnetic field blocks gas from rising from below 1 7 The Solar Cycle Magnetic Waves near Sunspot 8 • The number of sunspots goes up and down about once every 11 years on average. • After each sunspot maximum, the Sun’s magnetic field reverses. • Geologists find that the Earth’s magnetic field reverses once every ~250,000 years In this filtered movie from the Big Bear Solar Observatory, you can see magnetohydrodynamic waves emanating from the center of the sunspot. 9 Solar Flares In regions of strong magnetic fields, sudden bursts of gas may occur, and intense X-rays and visible light can be generated by electrons and charged particles impacting the surface. 11 More Solar Flares 10 After and during the flare, material moves in the confined magnetic tubes above the surface. Prominence 12 Solar Prominences In X-Rays we can observe hot gas directly from telescopes in space. The plasma moves along the magnetic field lines. 2 Magnetic Loops 13 Coronal Mass Ejections 14 Occasionally, a large blob of ionized gas is ejected from the Sun’s corona, leading some weeks later to auroras and interference with satellites here on Earth. Ionized plasma is confined by magnetic field lines looping out of the solar surface. 15 16 Long Term Changes in the Sun • When Sun is more active it generates more power overall. • This may affect Earth’s climate. Solar Wind Aurora on Earth: Excited O, N, H atoms (4+ days after CME) 17 PRS: Sunspots How do strong magnetic fields make sunspots dark? 1) They repel hydrogen atoms so the nuclear fusion is less intense. 2) They stop convection in the plasma so heat can’t rise through them. 3) They attract iron particles that block the light coming from below. 18 Calculating the Sun’s Luminosity Imagine completely surrounding the Sun with a sphere of radius 1 AU (1.5 x 1011 m), to capture all of its power output. Each square meter would receive 1300 Watts because the Sun’s radiation is the same in all directions. The Sun’s luminosity is therefore: L = B × 4 π d2 = (1300 watts/m2 ) × 4 π (1.5 x 1011 m)2 ~ 1.3 x 103 W/m2 × 2.6 × 1023 m2 ~ 4 x 1026 Watts 3 19 Human Energy Consumption The Sun from the Inside Out 20 Core Humans worldwide use ~4 x 1020 Joules of energy per year. (U.S. 25% of this.) How many years worth of energy does the Sun generate in one second? • This is where the Sun’s energy is generated. 1) 10-26 2) 10-20 3) 10-6 • Energy is transported by photons Radiation Zone 4) 106 5) 1014 6) 1026 Convection Zone time = 4x1026 Joules / 4x1020 Joules/year = 106 years The amount of sunlight that strikes the Earth is ~ 5 x 1024 Joules per year. • Energy is transported by upwelling gas (we see the top as granulation) 21 E=m PRS: Size of Sun’s Core If the Sun’s core has ¼ the Sun’s radius, how big is its volume compared to the volume of the whole Sun? 1) 2) 3) 4) 5) 6) 22 1/4 1/12 1/16 1/32 1/64 1/256 c2 • Einstein’s relationship between mass and energy implies that the Sun must be turning m = E / c2 = 4 x 1026 Joules / (3 x 108 m/sec) 2 ~ 4 x 109 kg = 4 million tons of matter into energy every second! • The Sun’s mass is so large that this is negligible. • What’s providing all of this power? 23 Nuclear Fusion • One of the only processes which is known to convert a significant fraction of mass into energy is nuclear fusion. • In the combining four hydrogen nuclei into a helium nucleus, almost 1% of the mass is released as energy. • If the Sun fuses all of the hydrogen in its core, it could burn for ~10 billion years at its current luminosity. 24 CPS: H, He, C burning Fusing atomic nuclei are stripped of all of their electrons in a plasma in the stellar core. Therefore, the order of easiest to hardest to fuse would be (1) H, C, He (3) He, C, H (2) H, He, C (4) C, He, H 4 25 26 Fission vs. Fusion Hydrogen Fusion The P-P chain is made possible by the extremely high temperature and density pressure at the Sun’s core. Net reaction: P+P+P+P = He + neutrinos + E Nuclei lower in mass than iron can combine to release energy. Higher mass nuclei can split to release energy. If the mass of the starting atoms is greater than that of the products, energy is released. 5