A white dwarf is the end stage of a star which started with a mass a few times that of our sun. It results from gravitational collapse after the outward pressure due to the heat of fusion has subsided. After collapse, the whole star is like one chunk of metal, all the electrons are free to move anywhere in the star and can be modeled with a simple particle in a well model. To do so, we will ignore nuclei and treat the electrons as particles in a 3d well. To refresh your memory, the energy levels in a well of width L with infinite potential walls are given by:
E = n2h2/8mL2
and the wavefunctions:
?=Asin(n?x/L).
To shift to three dimensions instead of one, we simply multiply the resulting wavefunctions and the energies will add. To see how this works, consider a 2-dimensional well of width L in both directions, x and y with the origin at one corner. The Schr?dinger equation for this well is
[a] Make the subtitutions for E and ? the Schr?dinger equation
[b] Split the equation into an x and a y equation
[c] Show that the x equation and y equation have the same solutions as the one-dimensional problem, that is show X(x) = Asin(nx?x/L) and Y(y) = Asin(ny?y/L) solve the equations and give the corresponding energies.
A white dwarf is the end stage of a star which started with a mass a...
C Question 5. The HF Moleoul C (time 3+3 3 +24-15 Minu C Question 12 Following Excit C Question 4. Time 6+514+5 2014pdf C Get Homework Help With C file:///C:Alsers/R3as0/Desktop/CHFM20020/Past %20paper/2014.pdf .. time 86 14 minutes Question 4. The Schrödinger equation for a particle in a one-dimensional box (length L) is: h2 d'y(x) 2m dx = Ey(x) (a) Show that nTx vlx)=2 sin n =1, 2, 3, .... are wavefunctions that satisfy the boundary conditions [y(0)= 0 and p(L) =...
8. The time independent Schrödinger equation (TISE) in one-dimension where m is the mass of the particle, E ita energy, (z) the potential (a) Consider a particle moving in a constant pote E> Vo, show that the following wave function is a solution of the TISE and determine the relationahip betwoen E an zero inside the well, ie. V(2)a 0foros L, and is infinite ou , ie, V(x)-w (4) Assuming (b) Consider an infinite square well with walls at 1-0...
TSD.1 In this problem, we will see (in outline) how we can calculate the multiplicity of a monatomic ideal gas This derivation involves concepts presented in chapter 17 Note that the task is to count the number of microstates that are compatible with a given gas macrostate, which we describe by specifying the gas's total energy u (within a tiny range of width dlu), the gas's volume V and the num- ber of molecules N in the gas. We will...