- Cosmology Tutorial
- Cosmology - Home
- The Expanding Universe
- Cepheid Variables
- Redshift and Recessional Velocity
- Redshift Vs. Kinematic Doppler Shift
- Cosmological Metric & Expansion
- Robertson-Walker Metric
- Hubble Parameter & Scale Factor
- Friedmann Equation & World Models
- Fluid Equation
- Matter Dominated Universe
- Radiation Dominated Universe
- The Dark Energy
- Spiral Galaxy Rotation Curves
- Velocity Dispersion Measurements of Galaxies
- Hubble & Density Parameter
- Age of The Universe
- Angular Diameter Distance
- Luminosity Distance
- Type 1A Supernovae
- Cosmic Microwave Background
- CMB - Temperature at Decoupling
- Anisotropy of CMB Radiation & Cobe
- Modelling the CMB Anisotropies
- Horizon Length at the Surface of Last Scattering
- Extrasolar Planet Detection
- Radial Velocity Method
- Transit Method
- Exoplanet Properties

- Cosmology Useful Resources
- Cosmology - Quick Guide
- Cosmology - Useful Resources
- Cosmology - Discussion

In this chapter, we will understand what the Angular Diameter Distance is and how it helps in Cosmology.

For the present universe −

$\Omega_{m,0} \: = \: 0.3$

$\Omega_{\wedge,0} \: = \: 0.69$

$\Omega_{rad,0} \: = \: 0.01$

$\Omega_{k,0} \: = \: 0$

We’ve studied two types of distances till now −

**Proper distance (lp)**− The distance that photons travel from the source to us, i.e., The**Instantaneous distance**.**Comoving distance (lc)**− Distance between objects in a space which doesn’t expand, i.e.,**distance in a comoving frame of reference**.

Consider a galaxy which radiates a photon at time **t _{1}** which is detected by the observer at

$$l_p = \int_{t_1}^{t_0} cdt$$

Let the galaxy’s redshift be **z**,

$$\Rightarrow \frac{\mathrm{d} z}{\mathrm{d} t} = -\frac{1}{a^2}\frac{\mathrm{d} a}{\mathrm{d} t}$$

$$\Rightarrow \frac{\mathrm{d} z}{\mathrm{d} t} = -\frac{\frac{\mathrm{d} a}{\mathrm{d} t}}{a}\frac{1}{a}$$

$$\therefore \frac{\mathrm{d} z}{\mathrm{d} t} = -\frac{H(z)}{a}$$

Now, comoving distance of the galaxy at any time **t** will be −

$$l_c = \frac{l_p}{a(t)}$$

$$l_c = \int_{t_1}^{t_0} \frac{cdt}{a(t)}$$

In terms of z,

$$l_c = \int_{t_0}^{t_1} \frac{cdz}{H(z)}$$

There are two ways to find distances, which are as follows −

$$F = \frac{L}{4\pi d^2}$$

where **d** is the distance at the source.

If we know a source’s size, its angular width will tell us its distance from the observer.

$$\theta = \frac{D}{l}$$

where **l** is the angular diameter distance of the source.

**θ**is the angular size of the source.**D**is the size of the source.

Consider a galaxy of size D and angular size **dθ**.

We know that,

$$d\theta = \frac{D}{d_A}$$

$$\therefore D^2 = a(t)^2(r^2 d\theta^2) \quad \because dr^2 = 0; \: d\phi ^2 \approx 0$$

$$\Rightarrow D = a(t)rd\theta$$

Changing **r** to **r _{c}**, the comoving distance of the galaxy, we have −

$$d\theta = \frac{D}{r_ca(t)}$$

Here, if we choose **t = t _{0}**, we end up measuring the present distance to the galaxy. But

$$\therefore d\theta = \frac{D}{r_ca(t_1)}$$

Comparing this with the previous result, we get −

$$d_\wedge = a(t_1)r_c$$

$$r_c = l_c = \frac{d_\wedge}{a(t_1)} = d_\wedge(1+z_1) \quad \because 1+z_1 = \frac{1}{a(t_1)}$$

Therefore,

$$d_\wedge = \frac{c}{1+z_1} \int_{0}^{z_1} \frac{dz}{H(z)}$$

**d _{A}** is the Angular Diameter Distance for the object.

If we know a source’s size, its angular width will tell us its distance from the observer.

Proper distance is the distance that photons travel from the source to us.

Comoving distance is the distance between objects in a space which doesn’t expand.

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