B Question about Hertzsprung-Russell-diagram

  • B
  • Thread starter Thread starter Meerio
  • Start date Start date
AI Thread Summary
The relationship between a star's temperature, luminosity, and radius is explained by the Stefan-Boltzmann equation, which quantifies the radiation emitted per unit area based on temperature. Total luminosity is derived by multiplying the radiation from the star's surface area, leading to the formula L = σT^4 * 4πR^2. By knowing a star's luminosity (L) and temperature (T), one can easily calculate its radius (R). This straightforward calculation highlights the interconnectedness of these stellar properties. Understanding this relationship is fundamental in astrophysics.
Meerio
Messages
16
Reaction score
1
Why can you read out the radii of the stars by knowing their temperature and luminosity?
Can't make sense out of it.
 

Attachments

  • images.jpg
    images.jpg
    10.7 KB · Views: 413
Physics news on Phys.org
The Stefan-Boltzmann equation tells you the amount of radiation emitted from a unit area of the star as a function of temperature. The total luminosity is then given by just summing this over the surface area of the star, so:

L = \sigma T^4 * 4 \pi R^2

So if you know L and T, you can calculate R.
 
wow that was easy thanks!
 
Thread 'Gauss' law seems to imply instantaneous electric field propagation'
Imagine a charged sphere at the origin connected through an open switch to a vertical grounded wire. We wish to find an expression for the horizontal component of the electric field at a distance ##\mathbf{r}## from the sphere as it discharges. By using the Lorenz gauge condition: $$\nabla \cdot \mathbf{A} + \frac{1}{c^2}\frac{\partial \phi}{\partial t}=0\tag{1}$$ we find the following retarded solutions to the Maxwell equations If we assume that...
Maxwell’s equations imply the following wave equation for the electric field $$\nabla^2\mathbf{E}-\frac{1}{c^2}\frac{\partial^2\mathbf{E}}{\partial t^2} = \frac{1}{\varepsilon_0}\nabla\rho+\mu_0\frac{\partial\mathbf J}{\partial t}.\tag{1}$$ I wonder if eqn.##(1)## can be split into the following transverse part $$\nabla^2\mathbf{E}_T-\frac{1}{c^2}\frac{\partial^2\mathbf{E}_T}{\partial t^2} = \mu_0\frac{\partial\mathbf{J}_T}{\partial t}\tag{2}$$ and longitudinal part...
Thread 'Recovering Hamilton's Equations from Poisson brackets'
The issue : Let me start by copying and pasting the relevant passage from the text, thanks to modern day methods of computing. The trouble is, in equation (4.79), it completely ignores the partial derivative of ##q_i## with respect to time, i.e. it puts ##\partial q_i/\partial t=0##. But ##q_i## is a dynamical variable of ##t##, or ##q_i(t)##. In the derivation of Hamilton's equations from the Hamiltonian, viz. ##H = p_i \dot q_i-L##, nowhere did we assume that ##\partial q_i/\partial...
Back
Top