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What is the Eddington limit? Explain how it can be used to set a limit on the mass of a supermassive black hole, and explain why this limit represents a minimum mass for the black hole.

Short Answer

Expert verified
The Eddington limit is a theoretical maximum condition of luminosity that can be maintained without having the mass of an object being blown away by the outward force of radiation pressure. For a supermassive black hole, the accretion rate is directly linked to its mass. Therefore, by measuring the accretion rate, a minimum limit on its mass can be determined.

Step by step solution

01

Definition of Eddington Limit

Eddington limit, named after astronomer Sir Arthur Eddington, defines the maximum luminosity a celestial body (like a star) can achieve while maintaining its stability. The light pressure outward is balanced by the gravitational force inward; beyond this limit, the object would shed mass at an increasing rate.
02

Application to Black Holes

In the context of black holes, the Eddington luminosity is used to determine the radiation pressure from the black hole's accretion disk. If a black hole accretes matter at a rate above the Eddington limit, the resulting radiation pressure would tend to push material away from the black hole.
03

Calculation of Minimum Mass

The Eddington limit can thus be used to derive a lower limit for the mass of a supermassive black hole. If we observe the radiation from an accreting black hole and measure its luminosity, we can infer the rate at which the black hole is accreting matter. By knowing this rate, we can apply the physics of the Eddington limit to conclude a minimum mass for the black hole. This is because the Eddington limit restricts the rate at which a supermassive black hole can accrete matter and hence grow in mass.
04

Explanation of the Limit as a Minimum

This limit represents a minimum mass because it is based on the balance of two forces - the gravitational pull of the black hole versus the outward push of radiation pressure. This balance determines the rate at which a supermassive black hole can accrete matter and grow in mass. Therefore, if we know the black hole's accretion rate, we can establish a minimum mass beneath which the black hole cannot fall without violating the principles that govern the Eddington Limit.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Supermassive Black Hole Mass
Supermassive black holes are cosmic giants, and their mass is one of the critical factors determining their interaction with the surrounding environment. The mass of a supermassive black hole can range from millions to billions of times the mass of our Sun. At this scale, their gravitational pull is immense, affecting stars, gas, and dust over vast distances. By observing the motions of stars near the center of galaxies, astronomers can estimate the mass of these gargantuan objects. However, the Eddington limit provides an additional method to assess their mass. Since there's a balance between gravity pulling material in and radiation pushing it away, measuring the amount of radiation allows us to infer the mass of the black hole indirectly. If we find a supermassive black hole with a luminosity at the Eddington limit, we know it must have a sizeable mass to produce that amount of energy without blowing itself apart.
Radiation Pressure
Radiation pressure is the force exerted by light on any surface it hits. In the cosmic scale, this pressure can influence the dynamics of gases and dust in space. Around a supermassive black hole, the intense radiation from the accretion disk heats the infalling material, creating a pressure that can counteract gravity. When the inward pull of gravity is just balanced by the outward push of radiation, we've reached the Eddington limit. The concept is akin to blowing up a balloon; too much air pressure and it will burst, too little and it won't inflate. For a supermassive black hole, if the radiation pressure becomes too strong due to excessive material falling in, it can prevent more matter from accreting by pushing it away, effectively setting a cap on the growth rate of the black hole.
Accretion Disk
An accretion disk is a structure often found around compact objects such as white dwarfs, neutron stars, and supermassive black holes. It's formed by material spiraling in towards the black hole, heated to extreme temperatures by friction and compression. This thermal energy is expelled as radiation, contributing to both the luminosity we observe and the radiation pressure we calculate. The accretion disk is a crucial element in studying black holes; it not only signals the presence of a black hole but also feeds it, allowing for growth in mass. The characteristics of the light emitted by the disk—its spectrum, intensity, and variability—provide valuable insights into the properties of the black hole, including its mass, spin, and the rate at which it's consuming material.
Gravitational Force
Gravitational force is the attractive force that acts between all masses in the Universe. For supermassive black holes, the gravitational force they exert is colossal due to their massive size. This force dictates how material accretes onto the black hole, as well as the orbit of nearby stars and the behavior of the galactic nucleus itself. It is the gravity of the black hole that competes with radiation pressure to establish the Eddington limit. The balance between the intense gravitational force pulling material inwards and the radiation pressure from the accreting material pushing outwards provides us with important information about the physical processes near a supermassive black hole, including the rate of growth and the emission of energy.
Luminosity
Luminosity is a measure of the total amount of energy emitted by an object per unit time. In the case of supermassive black holes, the luminosity primarily comes from the accretion disk's energy release as material spirals in and heats up. The Eddington limit is intimately related to luminosity: if the black hole accretes matter beyond this limit, the corresponding increase in luminosity would mean more radiation pressure, which could overcome gravitational attraction and stop further accretion. By measuring a supermassive black hole's luminosity, astronomers can work backwards to infer its accretion rate and, using the Eddington limit, set a lower bound on its mass. Stellar activity, background light, and other sources must be accounted for to ensure an accurate measurement of the black hole's true luminosity.

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Most popular questions from this chapter

. Figure 25-22 shows ionized gas streaming away from the "central engine" of the radio galaxy Cygnus A. Instead of spreading outward equally in all directions, the gas appears to be funneled into two oppositely directed cones. Discuss how this could be caused by a dusty torus surrounding a supermassive black hole at the center of Cygnus A.

Search the World Wide Web for information about "microquasars." These are objects that are found within the Milky Way Galaxy. How are they detected? What are the similari ties and differences between these objects and true quasars? Are they long-lasting or short-lived?

When we observe a quasar with redshift \(z=0.75\), how far into its past are we looking? If we could see that quasar as it really is right now (that is, if the light from the quasar could somehow reach us instantaneously), would it still look like a quasar? Explain why or why not.

Use the Starry Night Enthusiast \({ }^{\mathrm{TM}}\) program to examine the vicinity of the galaxy M87, shown in Figure 25-8. Select Favourites \(>\) Deep Space \(>\) Virgo Cluster to display this large cluster of galaxies. (a) You can use the upward and downward pointing triangles in the Viewing Location panel of the toolbar to move toward or away from the cluster. You can also rotate the Virgo Cluster by putting the mouse cursor over the image and, while holding down both the Shift key and the mouse button, move the mouse. (On a two-button mouse, hold down the left mouse button.) Use these controls to get a sense of the extent of the Virgo Cluster. Use the Viewing Location controls to move to a distance of about 30 Mly from the Sun. Open the Find pane and enter Virgo A. Click the menu button associated with Virgo A in the Find pane and select Highlight "GA Virgo Cluster" Filament to highlight the members of this cluster in yellow to see the extent of this huge grouping of galaxies. Describe where this active galaxy, also known as M87, is located in the cluster. (b) Discuss how the position of M87 in the Virgo Cluster might relate to its being an active galaxy.

If the Milky Way had an active galactic nucleus, with an accretion disk around its central black hole, there might be a pair of relativistic jets emanating from its center. Use the Starry Night Enthusiast \({ }^{\text {TM }}\) program to investigate how these jets might appear from Earth. On the toolbar, set the date and time to June 15 of this year at 12:00:00 A.M. (midnight), when the center of the Milky Way is prominent in the sky. Open the Find pane and center the field of view on the star HIP86919. The position of this star on the celestial sphere is less than \(1^{\circ}\) from the black hole at the center of the Milky Way. Select View > Stars and ensure that Milky Way is being displayed. Select Options > Stars > Milky Way to open the Milky Way Options dialog window, move the slidebar to the right to brighten the galaxy, and click the OK button. Close any open panes to ensure that that the entire window is again devoted to a view of the sky. Make a sketch of the Milky Way Galaxy and attempt to show how the night sky might appear on June 15 at 12:00:00 A.M. if our Galaxy had an active galactic nucleus. Label the Milky Way, the jets, the central black hole, and the accretion disk. Assume that the plane of the accretion disk is aligned with the plane of the Milky Way. Zoom in to a field of view of about \(6^{\circ}\). An X-ray image of the Milky Way center is superimposed upon the galaxy. (If not, select View \(>\) Deep Space and click on Chandra Images to display this image.) Open the object contextual menu over this image and click on Magnify to enlarge this image to see the high temperature features of this violently active region of our galaxy.

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