For a particle with energy E < U incident on the poten- tial energy step, use yo and y, from Eqs. 5.57, and eval- uate the constants B and D in terms of A by applying the boundary conditions at x = 0.
Q: Prove that, -2=kT2Cv, using the canonical ensemble in quantum statistical mechanics,
A: answer is in attachment.
Q: Problem #1 (Problem 5.3 in book). Come up with a function for A (the Helmholtz free energy) and…
A:
Q: Use the mapping function w = z2 to find the streamlines for the flow of wateraround the inside of a…
A: Consider the mapping function, w=z2 Differentiate with respect to z. dwdz=2z =0 When the real…
Q: Let V (r1→, ..., rM→) be the potential energy of a system of M massive particles which has the…
A: Given, Let V (r1→, ..., rM→) be the potential energy of a system of M massive particles which has…
Q: frequently interesting to know how a system behaves under some disturbance. These disturbances are…
A: Here the system is associated with 1D in potential well, The wave function related to this system is…
Q: Consider the dispersion relation of a linear spiral density wave perturbation (equation 4.45 in…
A: Step 1: Understanding the Toomre Q ParameterThe Toomre Q parameter is a unitless value that…
Q: We have a potential V = 1, where k is a constant and r is the distance to the potential focus, which…
A:
Q: Problem 2.14 In the ground state of the harmonic oscillator, what is the probability (correct to…
A: Understanding of this question is very easy because its just an small integral. But hardest point is…
Q: Problem 3.30 Derive the transformation from the position-space wave function to the “energy-space”…
A: In terms of states of eigen states, the identity operator is denoted as, ∑nEn><En=I The…
Q: Consider a system of two Einstein solids, A and B, each containing10 oscillators, sharing a total of…
A: The Einstein system is the one that can store any number of energy units of equal size. This system…
Q: Determine the transmission coefficient for a rectangular barrier (same as Equation 2.127, only with…
A: Solution:- E<V0 . ψ=Aeikx +Be-ikx(x<-a)Cekx +De-kx…
Q: Problem 1: Simple Harmonic oscillator (a) Find the expectation value of kinetic energy T for the nth…
A:
Q: 2.29 Consider a particle in one dimension bound to a fixed center by a 6-function potential of the…
A:
Q: 4.12-Consider a particle of dust orbiting a star in a circular orbit, with velocity v. This particle…
A:
Q: Evaluate the reflection and transmission coefficients for a potential barrier defined by Vo; 0; 0…
A: For simplicity we take potential 0 to "a" .
Q: Use a trial function of the form e(-ax^2)/2 to calculate the ground state energy of a quartic…
A:
Q: U = PV P = AT2 Find F0(U,V,N) and F1(U,V,N) After that use, Gibbs-Duhem to prove dF2=0 and…
A: We need to express F0 and F1 in terms of the extensive variables (U, V, and N) and the intensive…
Q: Problem 4.45. A simple partition function The partition function of a hypothetical system is given…
A:
Q: = (V2)1/2 K πGOO ' Consider the dispersion relation of a linear spiral density wave perturbation…
A:
Step by step
Solved in 3 steps with 2 images
- A. at pattern. Let's ssuming that the e angular spatial poral frequencies w, correspond to e is then W, 1) ir) [7.33] avelength of the quals the group eing amplitude- e waves of fre- of modulating and sum over is called the wer sideband. 7.19 Given the dispersion relation w = ak', compute both the phase and group velocities. -7.20* Using the relation 1/v = dk/dv. prove that 1 Vg I V₂ 7.21* In the case of lightwaves, show that V = 1 Ve v dv v² dv V 7.22 The speed of propagation of a surface wave in a liquid of depth much greater than λ is given by v dn c dv 11 -+- C solve 7.25 only where g = acceleration of gravity, λ = wavelength, p = density. Y = surface tension. Compute the group velocity of a pulse in the long wavelength limit (these are called gravity waves). 7.23* Show that the group velocity can be written as dv dλ 7.24 Show that the group velocity can be written as gλ 2πΥ + 2πT pλ Vg = V-A ( n + w(dn/dw) 7.25 With the previous problem in mind prove that dn (v) dv n₂ = n(v) + v.…Use a computer to reproduce the table and graph in Figure 2.4: two Einstein solids, each containing three harmonic oscillators, with a total of six units of energy. Then modify the table and graph to show the case where one Einstein solid contains six harmonic oscillators and the other contains four harmonic oscillators (with the total number of energy units still equal to six). Assuming that all microstates are equally likely, what is the most probable macrostate, and what is its probability? What is the least probable macrostate, and what is its probability?Calculate the period of oscillation of ?(x,t) for a particle of mass 1.67 × 10-27 kg in the first excited state of a box of width 1.68 × 10-15 m. Include a sketch of U(x) and ?(x).
- It says (in blue highlighted) that I will be of constant motion if I and H poisson commute. Please show that this is true in detail.Problem 2.21 Suppose a free particle, which is initially localized in the range -a < x < a, is released at time t = 0: А, if -a < х <а, otherwise, (x, 0) = where A and a are positive real constants. 50 Chap. 2 The Time-Independent Schrödinger Equation (a) Determine A, by normalizing V. (b) Determine (k) (Equation 2.86). (c) Comment on the behavior of (k) for very small and very large values of a. How does this relate to the uncertainty principle? *Problem 2.22 A free particle has the initial wave function (x, 0) = Ae ax where A and a are constants (a is real and positive). (a) Normalize (x, 0). (b) Find V(x, t). Hint: Integrals of the form e-(ax?+bx) dx can be handled by "completing the square." Let y = Ja[x+(b/2a)], and note that (ax? + bx) = y? – (b²/4a). Answer: 1/4 e-ax?/[1+(2ihat/m)] 2a Y (x, t) = VI+ (2iħat/m) (c) Find |4(x, t)2. Express your answer in terms of the quantity w Va/[1+ (2hat/m)²]. Sketch |V|? (as a function of x) at t = 0, and again for some very large t.…Expand the equation K = m(γ−1) in aTaylor series, and find the first two nonvanishingterms. Explain why the vanishing terms are theones that should vanish physically. Show thatthe first term is the nonrelativistic expression forkinetic energy.
- Problem 2.34 Consider the "step" potential:53 V (x) = [0, x ≤0, Vo, x > 0. (a) Calculate the reflection coefficient, for the case E VoFind a formula for the temperature of an Einstein solid in the limit q « N . Solve for the energy as a function of temperature to obtain U = N€e-€/kT (where € is the size of an energy unit).Problem 4.25 If electron, radius [4.138] 4πεmc2 What would be the velocity of a point on the "equator" in m /s if it were a classical solid sphere with a given angular momentum of (1/2) h? (The classical electron radius, re, is obtained by assuming that the mass of the electron can be attributed to the energy stored in its electric field with the help of Einstein's formula E = mc2). Does this model make sense? (In fact, the experimentally determined radius of the electron is much smaller than re, making this problem worse).
- 2.4. A particle moves in an infinite cubic potential well described by: V (x1, x2) = {00 12= if 0 ≤ x1, x2 a otherwise 1/2(+1) (a) Write down the exact energy and wave-function of the ground state. (2) (b) Write down the exact energy and wavefunction of the first excited states and specify their degeneracies. Now add the following perturbation to the infinite cubic well: H' = 18(x₁-x2) (c) Calculate the ground state energy to the first order correction. (5) (d) Calculate the energy of the first order correction to the first excited degenerated state. (3) (e) Calculate the energy of the first order correction to the second non-degenerate excited state. (3) (f) Use degenerate perturbation theory to determine the first-order correction to the two initially degenerate eigenvalues (energies). (3)6I need the answer as soon as possible