courses:ast100:3
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| courses:ast100:3 [2024/11/22 07:16] – [Death of Stars] asad | courses:ast100:3 [2026/02/24 08:21] (current) – [3. Stars and humans: birth and death] asad | ||
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| ====== 3. Stellar Age ====== | ====== 3. Stellar Age ====== | ||
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| - | **Mars:** Peace will come after war. But for now, there’s no way without war. Look ahead — the massive Yarlung Tsangpo Gorge, the deepest and longest canyon on Earth. Its deafening roar will make it impossible for any of us to hear one another. | + | <div id=" |
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| - | **Hermes:** We can hear you clearly. Like the final scene in *Crouching Tiger, Hidden Dragon*, let’s leap from the summit of Namcha Barwa to the very bottom of the gorge. There, amidst all the sounds, we’ll let our words float. | + | # |
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| - | ===== - Birth and Death Rates ===== | + | /* Timeline Styling */ |
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| - | **Socrates:** I am confused about how the seven ages of the universe have been divided. I understand that the timeframes of the four ages from the Planetary Age to the Cultural Age are based on Earth and humanity. But why did we decide to begin the Stellar Age exactly ten billion years ago? The first stars were born at the same time as the first galaxies. So, why is the Stellar Age placed after the Galactic Age? | + | /* Vertical Line */ |
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| - | **Mars:** Knowing this question would arise, I prepared this figure in advance. It shows that the black and red curves have stayed very close to each other over the past twelve billion years. The black curve represents the **Star Formation Rate (SFR)**, and the red curve represents the **Black Hole Accretion Rate (BHAR)**. On the X-axis, time is shown at the top, and redshift is shown at the bottom. We already know from the Galactic Age that redshift serves as a proxy for time. The Y-axis displays the two rates. The formation rate is a type of birth rate, indicating the total mass of stars born per gigaparsec of cubic volume at any point in the universe' | + | # |
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| - | **Socrates:** I see. The figure is now readable, and I understand that both curves peaked ten billion years ago. | + | /* Timeline Dot */ |
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| - | **Mars:** That means ten billion years ago, stars were being formed from gas at the highest rate, while at the same time, the most stars and gas were being lost into black holes. When the birth rate is highest, the death rate is also at its peak—assuming we metaphorically consider falling into a black hole as a form of death. | + | # |
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| - | **Socrates:** This can be compared to human populations. Just as birth rates are high in Niger, Chad, and Congo, so are death rates. However, since human societies are far more complex than any physical system, the comparison isn't straightforward. | + | # |
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| - | **Mars:** True, it isn’t straightforward, | + | |
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| - | **Socrates:** Comparing humans to the universe is always fascinating. However, now it’s more important to compare stars to one another. To me, all stars look the same—large, | + | /* Mobile Optimization |
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| - | ===== - Stellar Classification ===== | + | <div class=" |
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| - | **Mars:** It seems your daemon informs you in advance about the next topic in our discussion. I was just about to talk about stellar classification. | + | <!-- Event 2 --> |
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| - | **Mars:** Galaxies are classified by their shape because there’s a lot of diversity | + | <!-- Event 5 --> |
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| - | **Mars:** Correct. These smaller stars are the most abundant | + | <!-- Event 7 --> |
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| - | **Mars:** You’d call it middle-class. The difference is also reflected in color. | + | ===== - Event details ===== |
| - | **Ishtar:** Yes, smaller stars are slightly red, and larger ones are bluish. But while crossing | + | Following the emergence of the spherical Galactic halo, the Milky Way's rotating gas and dust gradually flattened into a thin disk. While older, metal-poor Population II stars maintained random orbits in the ancient halo, the new disk became the primary site of star formation. This flattening coincided with the birth of metal-rich Population I stars, formed from interstellar material enriched by earlier generations. These younger stars inherited the disk's spin, moving in highly ordered, circular orbits around the Galactic center. |
| - | **Mars:** Stars generally look white. The colors in this illustration have been exaggerated to clarify | + | Roughly 10 billion years ago, the universe reached its peak rate of star formation as galaxies rapidly consumed their abundant gas. During |
| - | **Socrates: | + | Around 8 billion years ago, a " |
| - | **Mars:** As we learned during | + | Stellar nucleosynthesis (to be detailed in the Chemical Age) is the process by which stars forge the chemical complexity required for planets and life. Throughout their main-sequence lifetimes, |
| - | **Socrates: | + | Because fusing iron yields no energy, these massive cores inevitably collapse under their own gravity, triggering Type II supernovae. During these catastrophic explosions, temperatures soar to billions of degrees, allowing rapid neutron capture (the r-process) to synthesize elements heavier than iron, such as gold, silver, and uranium. The blasts scatter this enriched material into the interstellar medium, fertilizing galactic clouds with the stardust essential for forming rocky planets. |
| - | **Mars:** It’s not possible with the naked eye. But with spectrographs, like a prism at a telescope’s focal plane, light can be split into its various frequencies or colors. This allows us to identify which color is most prominent in a star's light. In fact, by analyzing a star’s spectrum, we can determine its temperature. | + | Although gravity initially slowed cosmic expansion, a fundamental transition occurred roughly 7 billion years after the Big Bang. The universe' |
| - | **Juno:** Oh, I see! That’s why you’re talking about a star’s **surface temperature**. The light used to measure temperature comes from the star’s surface, so it’s easier to determine the surface temperature. But is there no way to know the temperature inside | + | For our local cosmic neighborhood, the Stellar Age culminated 4.6 billion years ago when a chemically enriched |
| - | + | ===== - Stars and humans: birth and death ===== | |
| - | **Mars:** There is. Using equations of **stellar structure**, | + | {{: |
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| - | **Mars:** You’re forcing us to move on to the next topic. The simple answer is that the larger a star, the faster it burns through its fuel, and thus, it dies sooner. | + | |
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| - | ===== - Star Formation ===== | + | |
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| - | **Mars:** To understand why stars die quickly, we must first understand how they are born. This image shows the process of star formation. In the interstellar | + | |
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| - | **Juno:** At first, it was just a shapeless cloud, but now I see a red sphere in the center surrounded by a flat disk about half a light-year in size. How did the shapeless cloud transform into a spherical core and flat disk over these few million years? | + | |
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| - | **Mars:** To understand that, you need to grasp the difference between **gravity** and **rotation**. If I jump into the swift current of the Aungsui River from this rock, I will survive unscathed. However, I would die if I didn’t land in the water because gravity pulls me toward the Earth' | + | |
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| - | **Juno:** Is that why you tied a rock to the end of a rope to explain rotation? | + | |
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| - | **Mars:** Yes. If I swing this rock around me while holding the rope, I feel a centrifugal force on my hand. Now, let go of the rope. What happens to the rock? | + | |
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| - | **Juno:** The rock flies away and falls into the Aungsui River. | + | |
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| - | **Mars:** Exactly. Rotation opposes gravity | + | |
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| - | **Juno:** It went farther than the first one. | + | |
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| - | **Mars:** That means the centrifugal force was greater this time. The farther you go from the center of rotation, the stronger the rotational force becomes, opposing gravity. Near the center, gravity overcomes rotation, and since gravity pulls equally in all directions (spherical symmetry), the core becomes spherical. Outside the center, where gravity weakens, rotation dominates, forming a flat disk. Most of the material is pulled into the core by gravity, forming the star, while only about 1% remains in the disk. | + | |
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| - | **Juno:** So gravity has spherical symmetry, while rotation has circular symmetry? | + | |
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| - | **Mars:** Exactly, and well put! The circular symmetry of rotation works perpendicular to the axis of rotation. Imagine spinning a spherical pizza dough on your hand — it flattens | + | |
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| - | **Mars:** This video explains it better. It shows actual images of stars being born inside the massive **Orion Molecular Cloud Complex** in the Orion constellation. The process is as follows: when the spherical gas core grows large enough, it starts consuming gas and dust from the disk. Some of this material, | + | |
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| - | **Mars:** True, just as stellar systems are flat, so are these galaxies. Galactic disks also form in a similar way from rotating interstellar clouds, although the clouds in this case are much larger. While the clouds that form stars or stellar systems are a few hundred light-years in size, the clouds that form galaxies can be hundreds of thousands to millions of light-years across. | + | |
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| - | **Mars:** Yes, and when that happens, the gas sphere will complete its transformation from a protostar into an **adult star**. | + | |
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| - | **Mars:** To answer that, you need to understand the internal structure of a star like the Sun. This image shows such a structure. At the center | + | |
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| - | **Mars:** Exactly. The green arrow represents **inward gravitational force**. Gravity pulls all the star’s gas inward toward the center, trying to compress it. However, the smaller the star becomes, the hotter its gas gets. The hotter the gas, the more it exerts an **outward pressure**, represented by the red arrow. If gravity and gas pressure balance each other, the star neither contracts due to gravity nor expands due to gas pressure. However, gas pressure alone is slightly weaker than gravity. To achieve stability, another outward pressure is needed, called **nuclear pressure**, represented by the blue arrow from the core. | + | |
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| - | **Mars:** Exactly. As the protostar contracts under gravity, its gas gets hotter, especially near the core. When the core’s temperature reaches **15 million Kelvin**, | + | |
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| - | **Mars:** Since 76% of the universe’s matter is hydrogen, 75% of a star’s gas is hydrogen. At 15 million Kelvin, hydrogen nuclei fuse to form **helium nuclei**. Actually, it’s not helium atoms but their nuclei, because the high temperatures prevent electrons from sticking to nuclei. | + | |
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| - | **Socrates: | + | |
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| - | **Mars:** Nuclear fusion produces an enormous amount of energy in the form of light. As this light travels outward from the core to the surface, it generates **radiation pressure**. This is what we call nuclear pressure. Once fusion begins, nuclear pressure combines with gas pressure to counter gravity, stabilizing the star. That’s when we can call it an **adult star**. | + | |
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| - | ===== - Life of Stars ===== | + | |
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| - | **Hermes:** Now that we’re on the border between India and China, let’s sit in the famous Buddhist monastery of Bisheng village and hear the story of stellar life. Watching the dramatic performances of Indian and Chinese border guards during the storytelling wouldn’t be a bad addition either. | + | |
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| - | //[Everyone leaves the shores of Aungsui and sits in the Bisheng monastery, facing the snowy peaks.]// | + | |
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| - | **Mars:** To understand the life of a star, we need to understand this famous plot known as the **H-R Diagram**. This is literally the story of a star’s life. On the X-axis (horizontal), | + | |
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| - | **Socrates: | + | |
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| - | **Mars:** The band is called the **Main Sequence**, where all adult stars reside. The two colored lines represent the **life tracks** of two types of stars, showing changes in their temperature and luminosity from birth to death. The blue line is for massive stars that are 10–20 times heavier than the Sun, while the yellow line is for smaller stars like the Sun. | + | |
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| - | **Mars:** No. As the temperature (X) of a star increases, its luminosity (Y) also increases. That’s why the Main Sequence is diagonal. Being to the right would mean low temperature but high luminosity, and being to the left would mean high temperature but low luminosity—both cases indicate instability, | + | |
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| - | **Mars:** The yellow line on the H-R Diagram aligns with this image, making it easier to understand. This image shows every stage in the life of a small star like the Sun, from birth to death, while the yellow line gives an idea of the star’s temperature and luminosity at each stage. I’ll explain by comparing the two side-by-side. The yellow line shows that the cloud from which the protostar forms is initially cold. As the temperature of the cloud increases from 1,000 to 4,000 Kelvin (moving left), the line suddenly drops, indicating that the cloud is shrinking. Remember, moving downward means brightness (and size) is decreasing. After passing through the **protostar** and **bipolar outflow** phases, when the star shrinks further and nuclear fusion begins in its core, the yellow line reaches the Main Sequence, signifying the star’s stable, adult phase. A star like the Sun remains here for **10 billion years**, as it takes that long to convert all the hydrogen in its core into helium. What happens after the hydrogen is exhausted? | + | |
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| - | **Mars:** And what happens when the star shrinks? | + | |
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| - | **Mars:** Because, Socrates, as the gas becomes hotter, hydrogen fusion begins in a shell around the core. Since the shell is closer to the surface compared to the core, the nuclear pressure in the shell causes the star to expand, turning it into a **Red Giant**. It’s red because its temperature is lower. After reaching a peak on the yellow line, the core becomes so hot that **helium fusion** starts in the core, where two helium nuclei fuse to form carbon. At this point, the yellow line drops again, stabilizing at a point where we call the star a **Yellow Giant**. What happens when the helium fuel is exhausted, i.e., when all helium is converted into carbon? | + | |
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| - | **Mars:** The carbon core doesn’t expand, but the surrounding | + | |
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| - | **Mars:** Exactly. Stellar life, like human life, is a cyclical process. Humans come from the Earth and return to it; stars come from gas and return to gas. By comparing this image of massive stars’ lives with the blue line in the H-R Diagram above, you’ll see the same cyclical process for larger stars as well. | + | |
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| - | **Mars:** Look at the blue line on the H-R Diagram. It starts from the bottom, rising to meet the Main Sequence. This means the gas gradually heats and expands, eventually forming an adult Main Sequence star through the same protostar and outflow phases. When the star nears the end of its life, the blue line exits the Main Sequence almost straight to the right, indicating a decrease in temperature and a slight increase in size. This phase is called the **Blue Giant**. It is followed by the **Pulsating Yellow Giant** phase, where the star’s size alternately increases and decreases. When it expands further, it becomes a **Red Supergiant**, | + | |
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| - | **Mars:** The iron core collapses further, becoming either a **neutron star** or a **black hole**. The core of a star that is 10–20 times more massive than the Sun typically becomes a neutron star, while heavier stars end their lives as black holes. | + | |
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| - | ===== - Death of Stars ===== | + | |
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| - | **Mars:** The remains of a star are no less fascinating than its life. To understand white dwarfs, we need to go back to **1604** | + | |
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| - | **Socrates:** Didn’t you say smaller stars only form white dwarfs, not supernovae? | + | |
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| - | **Hermes:** Patience! First, let’s travel to Prague in 1604. | + | |
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| - | //[With Hermes' | + | |
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| - | **Mars:** Stay invisible, everyone. Let me talk to Kepler. | + | |
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| - | //[Mars approaches the group Kepler was debating with, while the others remain invisible, observing and listening.]// | + | |
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| - | **Kepler:** I won’t believe it until I see it with my own eyes—a new star in the sky. I want to believe, though, because it would deliver another significant blow to Aristotle’s theories. | + | |
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| - | **Mars:** I saw it myself just last night. | + | |
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| - | **Kepler:** Where? | + | |
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| - | **Mars:** Look in that direction. It’s still visible. Check your charts to see if that star was supposed to be there. | + | |
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| - | **Kepler:** Incredible. It truly is a new star. It wasn’t supposed to be there. It’s been visible since last night. Aristotle said that nothing new happens in the heavens. He’s been proven wrong. My job now is to properly bury Aristotle’s theories by proving Copernicus’ heliocentric model. | + | |
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| - | **Mars:** Did you know that this new star is also a kind of burial? | + | |
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| - | **Kepler:** What do you mean? Who are you? A philosopher? | + | |
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| - | **Mars:** Who I am doesn’t matter. First, tell me—if, like Plato’s // | + | |
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| - | **Kepler:** I’m considering writing a story myself, called // | + | |
| - | ==== - White Dwarf ==== | + | |
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| - | **Mars:** Listen, then. This so-called “new star” was actually part of a **binary system**, meaning it had a companion star. Let’s call the new star **B** and its companion **C**. For about **10 billion years**, B and C orbited each other. However, since B was slightly larger and heavier than C, it died a million years ago, leaving behind a **white dwarf**—a very small but extremely hot remnant that appears white. After orbiting B’s corpse for a million years, C also neared the end of its life, swelling into a **red giant**, becoming enormous but cooler, thus appearing red. C grew so large that B (the white dwarf) began pulling gas from C’s outer layers. As a result, B’s mass gradually increased until, yesterday, it exceeded **1.4 times the Sun’s mass**. This caused B to collapse inward. However, since B’s core was extremely dense, the infalling gas couldn’t reach the center, bouncing off the solid core and exploding outward in a massive supernova. That’s why B is visible now. B isn’t a “new” star—it’s the fresh explosion of an old star’s corpse. | + | |
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| - | **Kepler:** Perhaps companion C was trying to revive B. | + | |
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| - | **Mars:** And it backfired. That’s why I always say: never attempt to revive the dead. If Orpheus couldn’t bring back Eurydice, how could C revive B? In reality, B’s massive explosion permanently flung C out of their mutual orbit. C is now a **runaway star**, a solitary wanderer. They’ll never again be gravitationally bound to each other. | + | |
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| - | **Kepler:** It’s not true that the dead can’t be revived. Plato revived Socrates. As much as I dislike Tycho Brahe, I must unearth the meaning of his observations, | + | |
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| - | //[Kepler turns back to find Mars gone, vanishing in an instant. Hermes takes everyone back to the confluence of the Siang and Brahmaputra rivers in India.]// | + | |
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| - | **Socrates: | + | |
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| - | **Mars:** Do you think I’d let Kepler catch me that easily? | + | |
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| - | **Mars:** A white dwarf is the highly compressed core of a star, so its density is incredibly high. So high, in fact, that the electrons within it can no longer maintain their usual positions and speeds. Under immense pressure, they are forced much closer together, and their speeds increase far beyond normal. These are known as **degenerate electrons**. Because they resist being forced closer, they collectively create an outward pressure called **degeneracy pressure**. This pressure counteracts gravity, allowing a white dwarf to remain stable for billions of years. | + | |
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| - | ==== - Neutron Stars ==== | + | |
| - | **Mars:** If the core mass of a star is less than 1.4 times the Sun’s mass, it becomes a white dwarf upon death. However, if it exceeds 1.4 times, it becomes a neutron star. For a core to reach this critical mass during a star's death, the star’s total mass must be at least 8 times the Sun’s mass. This is why only stars at least 8 times heavier than the Sun can leave behind a neutron star as their remnant. | + | |
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| - | **Mars:** Subrahmanyan Chandrasekhar (after whom the **Chandra X-ray Observatory** is named) discovered this famous limit in 1930 while traveling on a ship from Mumbai to Venice. Let me explain the **Chandrasekhar Limit** in simple terms, without math. Stars are primarily made of **hydrogen (74%)** and **helium (24%)**. Inside stars, the temperature is so high that electrons are stripped from atoms, leaving ions and free electrons. This creates a plasma—a gas of free protons (from hydrogen nuclei) and electrons. After passing through the red giant phase, the core of the star becomes small and dense. The electrons resist further compression by generating **electron degeneracy pressure**, stabilizing the star as a white dwarf. However, Chandrasekhar calculated that if the core’s mass exceeds **1.4 times the Sun’s mass**, gravity becomes so strong that electron degeneracy pressure can no longer counteract it. The core continues to collapse, breaking apart atomic nuclei, and converting protons into neutrons. These neutrons are packed extremely closely, and their motion generates a new type of pressure called **neutron degeneracy pressure**, which halts further collapse. Stars stabilized by neutron degeneracy pressure are called neutron stars. | + | |
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| - | **Mars:** Yes. If you compress a Sun-sized star (diameter ~1 million km) to the size of Earth (~10,000 km), you get a white dwarf. Compress it further to the size of Dhaka city (~10 km), and you get a neutron star. With no reduction in mass, the density increases drastically: | + | |
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| - | This means a **teaspoon** of neutron star material would weigh about **1 trillion kilograms**. | + | |
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| - | **Socrates: | + | |
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| - | **Mars:** The Sun and the Earth are both round, but how round are they? Due to rotation, no object can be perfectly spherical. The Earth, which rotates once every 24 hours, is slightly flattened at the poles. The difference between Earth’s equatorial and polar diameters is **0.3%**, while for the Sun, it’s only **0.0009%**, | + | |
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| - | **Socrates: | + | |
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| - | Here’s the response without bullet points: | + | |
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| - | **Mars:** You’re absolutely correct, Socrates. The gravity on a neutron star is immensely strong. Let me explain using weight as an analogy. A person weighing 100 kg on Earth would weigh 1,000 Newtons on Earth’s surface, 30,000 Newtons on the Sun’s surface, and 1 trillion Newtons on a neutron star’s surface. Despite this immense gravity, neutron stars remain as spherical as the Sun because they also spin very rapidly. Some neutron stars rotate up to 1,000 times per second. When a neutron star has a companion star or nearby gas, it can form an accretion disk, similar to protostars or active galaxies. As matter spirals into the neutron star, some of it is ejected along the poles as jets. These jets give rise to a type of neutron star called a **pulsar**. | + | |
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| - | Despite this immense gravity, neutron stars remain as spherical as the Sun because they also spin very rapidly. Some neutron stars rotate up to **1,000 times per second**. When a neutron star has a companion star or nearby gas, it can form an **accretion disk**, similar to protostars or active galaxies. As matter spirals into the neutron star, some of it is ejected along the poles as jets. These jets give rise to a type of neutron star called a **pulsar**. | + | |
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| - | **Socrates: | + | |
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| - | {{https:// | + | |
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| - | **Mars:** Yes, exactly like this image. The jet of a pulsar emits through a narrow beam, and we can only detect it when the beam is pointed directly at us. Each time the beam sweeps past Earth, telescopes detect a burst of high-energy radiation, creating a “pulse.” For pulsars that rotate 1,000 times per second, we detect 1,000 pulses per second. The first pulsar was discovered in **1967** by Jocelyn Bell Burnell at Cambridge University. Its regular pulses were so precise that some initially mistook them for signals from an alien civilization. | + | |
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| - | **Socrates: | + | |
| - | ==== - Black Hole ==== | + | |
| - | **Mars:** By now, you understand how a black hole forms. The fundamental challenge of a star’s life is resisting the relentless inward pull of gravity. The Sun does this through **nuclear pressure** and the pressure of hot gases, white dwarfs resist through **electron degeneracy pressure**, and neutron stars through **neutron degeneracy pressure**. However, if a star’s initial mass is **20 times or more** that of the Sun, its core will have a mass of at least **three times** the Sun’s mass at the time of its death. In such cases, even the degeneracy pressure of neutrons cannot counteract gravity. As the outer layers of the core collapse and bounce off the dense inner core, they cause a powerful supernova explosion, called a **hypernova**. After this explosion, the innermost core collapses under gravity into a near-point of infinite density—a **singularity**. | + | |
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| - | **Socrates: | + | |
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| - | **Mars:** Yes, it does. This image shows the structure surrounding a black hole, or at least its surroundings. The interior can’t be depicted, as nothing, not even light, can escape from within. | + | |
| - | **Socrates:** Is it gravity that prevents light from escaping? | + | This 2014 Madau & Dickinson diagram illustrates the cosmic history of star formation and black hole growth. The plot utilizes a dual x-axis: the bottom tracks cosmological redshift |
| - | **Mars:** Exactly. | + | The graph' |
| - | While all the energy and matter are concentrated in the **singularity**, | + | < |
| + | <iframe src=" | ||
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| - | Like protostars | + | We can draw a striking allegory between this cosmic timeline |
| - | **Socrates: | ||
courses/ast100/3.1732285004.txt.gz · Last modified: by asad
