AWC Rad 30000 100
Q: 2. The Heisenberg uncertainty principle demonstrate the symmetry between the particles position and…
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Q: • What makes a set of objects a vector space? You will no doubt want to refer to notes and the text,…
A: A vector space is a collection of objects, called vectors, that can be added together and multiplied…
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A: State Diagram-
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Q: Derive the Lagrange's equations of a disk that is rolling down Plane without slipping motion for…
A: We can solve a classical mechanics problem using the concept of Lagrangian. This approach is useful…
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A: The quantum mechanics is a field of physics which deals with very small particles. It was started at…
Q: please answer and explain step by step
A: To create a 2-mode quantum program with an initialized state and a 2-mode squeezing gate followed by…
Q: Look for the results of the questions below whether they include convergent or divergent series…
A: (a) This is a divergent series.
Q: Rank, in increasing order, the derivatives of the function at each of the points marked A through D.…
A: Write the equation for the slope of the point. Slopem=Riserun =y2-y1x2-x1
Q: Knowing the connection between velocity and kinetic energy, make a sketch of the system below, and…
A: Answer: The velocity v and the kinetic energy KE are related to each other by the following…
Q: Consider a finite potential step as shown below, with V = V0 in the region x 0. Particles with…
A: The potential is given by,
Q: Calculate the relative error for your calculated for Trial #6 from the friction lab (the accepted…
A: The relative error (), is given by formula:
Q: e Newtons method for the case of roots.
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Q: How is the highlighted section the lagrangian? what about the kinetic energy?
A: The highlighted section (∫ y(x)√(y'(x)² + 1) dx) is not the Lagrangian itself, but it's a part of…
Q: The position of a ball, u(t), rolling on a bump is modelled using the ODE d²u du dt² = 3u-2=. dt (a)…
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Q: Problem 1 (multiple parts) The Dynamics Squad is at it again with more experiments. Thin disk C…
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Q: Explain in detail and with the aid of diagrams the absence of the C type Bravais lattice for the…
A: The base centered or c-centered cubic lattice system doesn't exist because it can be redrawn to a…
Q: In the case of a one-dimensional harmonic oscillator, state whether each of the following…
A: In the case of a one-dimensional harmonic oscillator,when measured, the total energy will always…
Q: The greenhouse-gas carbon dioxide molecule CO2 strongly absorbs infrared radiation when its…
A: Let, the CO2 molecule as a 3 body spring system. Now, the masses are connected by springs of spring…
Q: QUESTION 2 Hermite polynomials are useful for solving for the wave functions of a 3-dimensional…
A: The wave function of the three-dimensional harmonic oscillators is given in terms of the Hermite…
Q: (c) Of a room-temperature proton? (Ans: 0.147nm) (d) In what circumstances should each behave as a…
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Q: Question A3 A wavefunction takes the form = A sin(2x) in the interval -1 < x < 1, and is zero…
A: Step 1: Step 2: Step 3: Step 4:
Q: Problem 4. Consider the rigid rotor of problem 3 above. A measurement of Le is made which leaves the…
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Q: .In the 1-D problem shown below, a 5-MeV alpha particle is approaching a square potential barrier. a…
A: Quantum Tunneling
Q: For the logic diagram, write the Boolean expression. Show output of each gate in the Qiagram.…
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Q: Solve the beneath problems and give the right numeric response. Two balls with masses m1 and m2…
A: Applying the law of conservation of momentum and Kinetic energy;
Q: Find the optical and acoustical branches of the dispersion relation for a diatomic linear lattice,
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Find the phase velocity and group velocity for the diagram below at point A.


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- Calculate and plot the vibrational partition function of CSe2 between 500K and 1000K (with a step of 100K) given the wavenumbers 313 cm- (bend. two modes). 369 cm-1 ( symmetric stretch) and 1302 cm - (asymmetric stretch) assuming that each vibrational mode can be treated as a simple harmonic oscillator. Explain and discuss each step. (marks 10)Use your generic solution to the 2D box wavefunctions to demonstrate the following prop- erties of wavefunctions. 1. Show that if you independently normalize (x) and (y) that the product of (x) and (y) is also normalized. 2. Show that the wavefunctions for one dimension are orthogonal. Orthogonality means that f₁ Vndr = Smn, where the Kroenecker delta function means that the function is one for men and zero for m‡n. m 3. How many quantum numbers are needed to describe the energy of your system? 4. Show that the two dimensional wavefunctions are orthogonal by performing this test on the wavefunction for n = 1, ny = 2 and the wavefunction for nr = 2 and ny = 1. CLx Ly Mathematically the operations looks like f¹* f¹¹ V₁,2 (x, y) V2,1 (x, y) dxdy.Problem #2 Calculate the Legendre transform (F1) of y = x². For your answer, give the new function F1 and its derivative dF1. (a(f(x)) Note that dy = C dx, C, = f(x), and dC, = (0) dx. dx
- Part A Which particle can have its velocity known most precisely? Match the words in the left column to the appropriate blanks in the sentences on the right. Reset Help smallest position uncertainty The particle with the most precisely known velocity has the This can be observed for and the greatest wave function amplitude. smallest position uncertainty and wave function amplitude. greatest position uncertainty. The wave function amplitude does not play a role. greatest position uncertainty and the smallest wave function amplitude. Figure (x) (x) particle 1. AAAAA particle 2. particle 3. Particle 1 Particle 2 (x) particles 2 and 3. particles 1 and 2. Particle 3 Submit Previous Answers Request AnswerConsider a thin hoop of mass (1.420 ± 0.001) kg and radius (0.250 ± 0.002) m. The moment of inertia for a thin hoop rotating about an axis going through its center is MR2 . Calculate the moment of inertia of this hoop and its uncertainty using error propagation rules (see Appendix). Clearly show work. Please solve the uncertainty using the appendix I attachedEnumerate the constraints that restrict which functions can be viable wavefunctions.