$13.5.9^*.$ Large masses of matter in the Universe can focus light from distant objects, forming a "gravitational lens". Estimate the focal length of a spherical galaxy of radius $R \approx 20000 \text{ pc}$ and mass $M \approx 3 \cdot 10^{11} M_\odot$ (where $M_\odot$ is the mass of the Sun), assuming that the mass in the galaxy is distributed uniformly.
Since the light is coming from exceptionally distant astronomical objects, we can treat the incident light rays reaching our galaxy as practically parallel.
According to General Relativity, the deflection angle of a light ray passing a mass with an impact parameter $b$ is:
@@ -14,7 +14,7 @@Solution
$$\alpha = \frac{4GM_{enc}}{c^2 b}$$
Here, $M_{enc}$ is the effective mass responsible for the gravitational pull.
−
Let's consider paraxial rays ($b \ll R$) to determine the focal length. As the photon travels through the galaxy in a straight line, it forms a chord. The exact length of this path inside the spherical galaxy is $L = 2\sqrt{R^2 - b^2}$. Since $b$ is negligibly small compared to $R$, we can approximate the path length as the diameter of the galaxy: $L \approx 2R$.
+
Let's consider paraxial rays ($b \ll R$) to determine the focal length. As the photon travels through the galaxy in a straight line, it forms a chord. Since $b$ is negligibly small compared to $R$, we can approximate the path length as the diameter of the galaxy: $L \approx 2R$.
Why do we evaluate the mass inside a cylinder? As the photon travels along its straight trajectory at the speed of light, it experiences a transverse gravitational force. By symmetry, the components of the gravitational pull from the mass outside the photon's cylindrical path cancel each other out when integrated along the line of sight. Therefore, the net deflection is strictly caused by the matter enclosed within a cylinder of radius $b$ and length $L \approx 2R$.
The volume of this effective cylinder is:
$$ V_{cyl}\approx\pi b^2 \cdot 2R = 2\pi R b^2 $$
Since the density of matter in the galaxy is uniform ($\rho = \frac{M}{\frac{4}{3}\pi R^3}$), the enclosed mass within the cylinder is:
For small deflection angles, the geometry of a right triangle gives us the relationship $\tan\alpha\approx\alpha = \frac{b}{F}$.
Notice that our derived deflection angle $\alpha$ is directly proportional to the impact parameter $b$. This means the focal length $F$ is constant for all paraxial rays, proving that the central part of the uniform galaxy acts as an ideal thin lens:
$$\frac{1}{F} = \frac{6GM}{c^2 R^2}\quad\implies\quad F = \frac{c^2 R^2}{6GM}$$
Now, we estimate the numerical values in SI units:
$13.5.9^*.$ Large masses of matter in the Universe can focus light from distant objects, forming a "gravitational lens". Estimate the focal length of a spherical galaxy of radius $R \approx 20000 \text{ pc}$ and mass $M \approx 3 \cdot 10^{11} M_\odot$ (where $M_\odot$ is the mass of the Sun), assuming that the mass in the galaxy is distributed uniformly.
$13.5.9^*.$ Large masses of matter in the Universe can focus light from distant objects, forming a "gravitational lens". Estimate the focal length of a spherical galaxy of radius $R \approx 20000 \text{ pc}$ and mass $M \approx 3 \cdot 10^{11} M_\odot$ (where $M_\odot$ is the mass of the Sun), assuming that the mass in the galaxy is distributed uniformly.
Since the light is coming from exceptionally distant astronomical objects, we can treat the incident light rays reaching our galaxy as practically parallel.
Since the light is coming from exceptionally distant astronomical objects, we can treat the incident light rays reaching our galaxy as practically parallel.
According to General Relativity, the deflection angle of a light ray passing a mass with an impact parameter $b$ is:
According to General Relativity, the deflection angle of a light ray passing a mass with an impact parameter $b$ is:
@@ -14,7 +14,7 @@Solution
$$\alpha = \frac{4GM_{enc}}{c^2 b}$$
$$\alpha = \frac{4GM_{enc}}{c^2 b}$$
Here, $M_{enc}$ is the effective mass responsible for the gravitational pull.
Here, $M_{enc}$ is the effective mass responsible for the gravitational pull.
Let's consider paraxial rays ($b \ll R$) to determine the focal length. As the photon travels through the galaxy in a straight line, it forms a chord. The exact length of this path inside the spherical galaxy is $L = 2\sqrt{R^2 - b^2}$. Since $b$ is negligibly small compared to $R$, we can approximate the path length as the diameter of the galaxy: $L \approx 2R$.
Let's consider paraxial rays ($b \ll R$) to determine the focal length. As the photon travels through the galaxy in a straight line, it forms a chord. Since $b$ is negligibly small compared to $R$, we can approximate the path length as the diameter of the galaxy: $L \approx 2R$.
Why do we evaluate the mass inside a cylinder? As the photon travels along its straight trajectory at the speed of light, it experiences a transverse gravitational force. By symmetry, the components of the gravitational pull from the mass outside the photon's cylindrical path cancel each other out when integrated along the line of sight. Therefore, the net deflection is strictly caused by the matter enclosed within a cylinder of radius $b$ and length $L \approx 2R$.
Why do we evaluate the mass inside a cylinder? As the photon travels along its straight trajectory at the speed of light, it experiences a transverse gravitational force. By symmetry, the components of the gravitational pull from the mass outside the photon's cylindrical path cancel each other out when integrated along the line of sight. Therefore, the net deflection is strictly caused by the matter enclosed within a cylinder of radius $b$ and length $L \approx 2R$.
The volume of this effective cylinder is:
The volume of this effective cylinder is:
$$ V_{cyl}\approx\pi b^2 \cdot 2R = 2\pi R b^2 $$
$$ V_{cyl}\approx\pi b^2 \cdot 2R = 2\pi R b^2 $$
Since the density of matter in the galaxy is uniform ($\rho = \frac{M}{\frac{4}{3}\pi R^3}$), the enclosed mass within the cylinder is:
Since the density of matter in the galaxy is uniform ($\rho = \frac{M}{\frac{4}{3}\pi R^3}$), the enclosed mass within the cylinder is:
For small deflection angles, the geometry of a right triangle gives us the relationship $\tan\alpha\approx\alpha = \frac{b}{F}$.
For small deflection angles, the geometry of a right triangle gives us the relationship $\tan\alpha\approx\alpha = \frac{b}{F}$.
Notice that our derived deflection angle $\alpha$ is directly proportional to the impact parameter $b$. This means the focal length $F$ is constant for all paraxial rays, proving that the central part of the uniform galaxy acts as an ideal thin lens:
Notice that our derived deflection angle $\alpha$ is directly proportional to the impact parameter $b$. This means the focal length $F$ is constant for all paraxial rays, proving that the central part of the uniform galaxy acts as an ideal thin lens:
$$\frac{1}{F} = \frac{6GM}{c^2 R^2}\quad\implies\quad F = \frac{c^2 R^2}{6GM}$$
$$\frac{1}{F} = \frac{6GM}{c^2 R^2}\quad\implies\quad F = \frac{c^2 R^2}{6GM}$$
Now, we estimate the numerical values in SI units:
Now, we estimate the numerical values in SI units:
