Chapter 19: Problem 36
A quasar has the same brightness as a galaxy that is seen in the foreground 2 Mpc distant. If the quasar is 1 million times more luminous than the galaxy, what is the distance of the quasar?
Short Answer
Expert verified
The distance of the quasar is 2,000 Mpc.
Step by step solution
01
Understand the Relationship between Brightness and Luminosity
Brightness decreases with the square of the distance from the source. That is, brightness (\text{B}) is proportional to luminosity (\text{L}) over distance squared (\text{D}^2): \[ B \rightarrow \frac{L}{D^2} \]
02
Write the Given Information
The galaxy's brightness and luminosity (\text{B}_\text{gal}, \text{L}_\text{gal}) are related through its distance: \[ B_\text{gal} = \frac{L_\text{gal}}{(2 \text{ Mpc})^2} \] The quasar is 1 million times more luminous than the galaxy but has the same brightness as the galaxy at 2 Mpc: \[ L_\text{quasar} = 10^6 \times L_\text{gal} \ B_\text{quasar} = B_\text{gal} \]
03
Equate the Brightness of Galaxy and Quasar
Since the brightness of the quasar and galaxy is the same, we have: \[ \frac{L_\text{quasar}}{D_\text{quasar}^2} = \frac{L_\text{gal}}{(2 \text{ Mpc})^2} \ \]
04
Plug in the Luminosity of the Quasar
Substitute the given luminosity for the quasar: \[ \frac{10^6 \times L_\text{gal}}{D_\text{quasar}^2} = \frac{L_\text{gal}}{(2 \text{ Mpc})^2} \]
05
Solve for the Distance of the Quasar
Cancel out \text{L}_\text{gal} from both sides of the equation and solve for \text{D}_\text{quasar}: \[ \frac{10^6}{D_\text{quasar}^2} = \frac{1}{4} \ \] Rearrange to solve for \text{D}_\text{quasar}: \[ D_\text{quasar}^2 = 4 \times 10^6 \text{ Mpc}^2\ D_\text{quasar} = \text{2,000 Mpc} \]
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Brightness and Luminosity Relationship
To understand how we determine the distance of a quasar using its brightness and luminosity, let's first define these two terms. Brightness is how much light from a celestial object reaches us on Earth. It's the perceived intensity of the light. Luminosity, on the other hand, is the total amount of energy emitted by the object per second in all directions.
Imagine holding a flashlight. The brightness you see depends on how far you are from it. The farther away, the dimmer it appears. Luminosity would be like knowing the bulb strength in the flashlight. A 100-watt bulb will always be a 100-watt bulb regardless of where you are in the room.
In astronomy, the relationship between brightness (\text{B}) and luminosity (\text{L}) is given by: \[ B \rightarrow \frac{L}{D^2} \] Here, \text{D} is the distance to the object. This equation tells us that brightness decreases as the square of the distance from the source increases. So, if you double the distance, the brightness decreases by a factor of four.
Imagine holding a flashlight. The brightness you see depends on how far you are from it. The farther away, the dimmer it appears. Luminosity would be like knowing the bulb strength in the flashlight. A 100-watt bulb will always be a 100-watt bulb regardless of where you are in the room.
In astronomy, the relationship between brightness (\text{B}) and luminosity (\text{L}) is given by: \[ B \rightarrow \frac{L}{D^2} \] Here, \text{D} is the distance to the object. This equation tells us that brightness decreases as the square of the distance from the source increases. So, if you double the distance, the brightness decreases by a factor of four.
Inverse Square Law
The inverse square law is a crucial concept in the calculation of astronomical distances. It states that a physical quantity (in this case, brightness) is inversely proportional to the square of the distance from the source.
Consider a light bulb: if you move twice as far away, the area over which its light spreads increases by four times, making it look four times dimmer. This is mathematically expressed as:
\[ B \rightarrow \frac{L}{D^2} \]
This principle applies to all sources of light in the universe, including quasars and galaxies. When comparing the brightness and luminosity of different astronomical objects, this law helps you determine how the observed brightness changes with distance.
Let's tie this back to our quasar and the foreground galaxy. The quasar is way more luminous (one million times more, in fact), but if both objects appear equally bright to us, it means the quasar must be much farther away. The inverse square law allows us to equate the brightness and adjust the luminosity to solve for the quasar's distance.
Consider a light bulb: if you move twice as far away, the area over which its light spreads increases by four times, making it look four times dimmer. This is mathematically expressed as:
\[ B \rightarrow \frac{L}{D^2} \]
This principle applies to all sources of light in the universe, including quasars and galaxies. When comparing the brightness and luminosity of different astronomical objects, this law helps you determine how the observed brightness changes with distance.
Let's tie this back to our quasar and the foreground galaxy. The quasar is way more luminous (one million times more, in fact), but if both objects appear equally bright to us, it means the quasar must be much farther away. The inverse square law allows us to equate the brightness and adjust the luminosity to solve for the quasar's distance.
Distance of Astronomical Objects
Determining the distance of astronomical objects like quasars is essential for understanding the scale of the universe. Various methods are used, but using brightness and luminosity relationship is one of the fundamental techniques.
In our exercise, we have a quasar and a galaxy with these key details:
Using the inverse square law, we know:
By substituting \( L_\text{quasar} = 10^6 \times L_\text{gal} \) in the above equation, we can then solve for \( D_\text{quasar} \). Simplifying, we find:
\[ D_\text{quasar}^2 = 4 \times 10^6 \text{ Mpc}^2 \]
Taking the square root to find \( D_\text{quasar} \), we get:
\[ D_\text{quasar} = 2,000 \text{ Mpc} \]
Thus, the quasar is 2,000 Megaparsecs away, illustrating how astronomers use these concepts to measure cosmic distances.
In our exercise, we have a quasar and a galaxy with these key details:
- The galaxy is 2 Megaparsecs (Mpc) away.
- The quasar is one million times more luminous than the galaxy.
- Their apparent brightness to us is the same.
Using the inverse square law, we know:
- \( B_\text{gal} = B_\text{quasar} \)
- \( \frac{L_\text{gal}}{(2 \text{ Mpc})^2} = \frac{L_\text{quasar}}{D_\text{quasar}^2} \)
By substituting \( L_\text{quasar} = 10^6 \times L_\text{gal} \) in the above equation, we can then solve for \( D_\text{quasar} \). Simplifying, we find:
\[ D_\text{quasar}^2 = 4 \times 10^6 \text{ Mpc}^2 \]
Taking the square root to find \( D_\text{quasar} \), we get:
\[ D_\text{quasar} = 2,000 \text{ Mpc} \]
Thus, the quasar is 2,000 Megaparsecs away, illustrating how astronomers use these concepts to measure cosmic distances.