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Sriman Dutta

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About Sriman Dutta

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  • Birthday 12/18/2000

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  • Location
    Kolkata, India
  • Interests
    Books and paintings take my free time. Love to listen to music, capture moments and travel.
  • College Major/Degree
    Indian Institute of Engineering Science and Technology, Shibpur
  • Favorite Area of Science
  • Biography
    Exploring life...
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  1. Hi! I was trying to analyse the RC series circuit for a sinusoidal AC input. I fed the input with an AC voltage V1sin(wt), and found the differential equation for the voltage across the capacitance Vo. RC dVo/dt +Vo = V1sin(wt) I assumed the capacitor was chargeless, so Vo = 0 at t=0. Next I tried to solve for Vo using two methods. I used Laplace transform and brute-force solving the differential equation itself. However I arrived at two different results, considering the same initial condition. Please see if I'm missing something. Or do give an explana
  2. I agree. I personally followed Griffiths Quantum Mechanics and McGraw Hill's Demystifying Quantum Mechanics as introductory textbooks, later supplemented by JJ Sakurai's Modern Quantum Mechanics as I got interested in the concepts of angular momentum.
  3. I actually meant to say that modern QM begins with Hilbert space definition. However in introductory college lessons, they first teach you the phenomenon that raised doubt in classical physics. As an example, I told about my first sem lectures in QM. on a side note, can you tell me the name of the book? It looks intriguing.
  4. Yaa. There were three main postulates: the constant speed of light for all observers, the same laws of physics for all inertial observers and the homogeneity of space. Well, Heisenberg's uncertainty principle is a special case of a nore general result in mathematics, which is the uncertainty principle for two Fourier conjugate variables. If g(t) be a function of t, and it's Fourier transform be G(f) in the conjugate domain f, then the uncertainty principle is equally valid for them. In QM x and p are conjugate variables and gence there exists an uncertainty principle betw
  5. Okay. So pretty much the fundamentals are a guesswork. And yet the entire formulation that relies heavily on those axioms works out so well. Hence there isn't any independent deduction of the Planck-Einstein relations, as I infer. This is unlike other branches. In relativity the main postulate that speed of light is constant for all observers has a well-reasoned deduction feom Mawell equations solutions on the form of plane waves. The rest part of relativity like length contraction, time dilation, Lorentz transformation can be deduced mathematically from that postulate.
  6. Then these are the basic or the most fundamental equations ? I might say then that they are axioms.
  7. Hi, Planck while explaining the black-body radiation postulated that photon energy is quantised, that is, E=hf, f is frequency. Similarly to explain the matter waves, de Brogile proposed that p=h/y, y is wavelength. Using this two relations, the whole theory of QM has been developed. Is there any derivation of these results ? Or are they accepted to be fundamental relations of nature? Thanks !
  8. You seem not to understand what is meant by bases. I will be trying to explain it in simpler terms. Any quantitative thing is a number. We use 10 characters 1,2,3,4,5,6,7,8,9,0 to represent them. Count how many characters we use? It's ten characters. Therefore our standard base of calculation is ten. Now imagine a civilisation living in a far off galaxy (don't ask questions like where are they bla bla, I'm just trying to explain). They evolved just like us. However unlike us, they are familiar to calculate numbers in base 4. They use the characters @,#,$ and & to represent
  9. I see. Thanks a lot for the information!
  10. I see. Is the approach to the mathematical proof requires group theory? Also imagine if there are two particles are in positions 1 and 2, then their exchange in positions is equivalent to rotation of the world around them keeping them constant. But how can that change the wavefunction ? Like I can view the two particles are seen one side, and from other side, their wavefunction values are different (a minus sign pops up!) ?
  11. Hi everyone, While reading Quantum Mechanics from Griffiths, I came upon a point where the author writes that the relationship between spin of a particle and its characteristic statistical behavior is explained by relativity. I'm in complete darkness regarding this. Can someone please explain how this is explained? And also it will be great if someone can cite some source or mathematically explain the phenomenon. Thanks in advance!
  12. From a realist's point of view, you cannot altogether discard military. You cannot absolutely disarm and channel all your military funds to other sectors. Because there are threats. Because there is fundamentalism and violence. A recent knife-attack and inhumane beheading of a teacher in France remains the solid evidence that there exists a vast populace whose sentiment is fragile enough to be hurt by caricrature of religious figures. In essence they are arrogant, orthodox and deeply fundamentalist, lashing and attacking all the elements of modernity, viewing them vile and obstructing the prog
  13. What did you do to the equation? Your entire passage sounded me to like: here's positive, negative, both direction, negative direction, E=mc squared, E=0+mcsquared, blah blah... Wish to learn before you theorise? Follow the textbooks.
  14. yes, to be strictly speaking, this is not formally tunnelling. A better example of it can be the delta potential. However, even in this finite potential well, the wavefunction behaves like that. I am actually trying to draw the analogy here between the probability of finding the particle on the other side of potential barrier and the probability of finding in the regions outside (-a,a) where E<V0, yet still it manages to get there.
  15. Assumin V=0 when -a<x<a V=V0 elsewhere (V0>0) There are two cases: Case 1: E < V0 (bound state) In this case, the wavefunction has certain discrete energy levels, the number of which depends on the strength (aka shallowness) of the potential. The discrete states can be obtained after some numerical calculus, as there is no direct analytical method. Also the wavefunction is not zero outside (-a,a). This is the striking feature of quantum tunneling. If you integrate the square modulus of the wavefunction in
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