Recent content by Toby_phys

  1. Toby_phys

    Using Noether's Theorem to get conserved quantities

    Homework Statement N point particles of mass mα, α = 1,...,N move in their mutual gravitational field. Write down the Lagrangian for this system. Use Noether’s theorem to derive six constants of motion for the system, none of which is the energy Homework Equations Noethers Theorem: If a...
  2. Toby_phys

    Energy of a solenoid with a partially removed core

    Homework Statement A solenoid of volume V, current I and n turns per unit length has an LIH core, relative permitivity is \mu_r. This core is then slid out so that a fraction f of the solenoid's length is filled with air/vacuum (and 1-f is filled with the core). Neglecting hysteresis, what...
  3. Toby_phys

    Effusing gas onto the interior of an evacuated sphere

    Homework Statement A gas effuses into a vacuum though a small hole of area A. Show that if the particles effused into an evacuated sphere and the particles condensed where they collided that there would be a uniform coating. (7.6 of Blundell and Blundell) Homework Equations Angular...
  4. Toby_phys

    Adiabatic stretching of a rubber band

    There was a part A that was to show this is the case $$dU=C_vdT+\left[f-T\left(\frac{\partial f}{\partial T}\right)_L\right]dL$$ The second term drops out
  5. Toby_phys

    Adiabatic stretching of a rubber band

    Homework Statement For a stretched rubber band, it is observed experimentally that the tension ##f## is proportional to the temperature ##T## if the length ##L## is held constant. Prove that: (b) adiabatic stretching of the band results in an increase in temperature; (c) the band will...
  6. Toby_phys

    Efficiency of a Simple 3-Stage Ideal Gas Cycle: Analyzing Thermal Efficiency η

    A possible ideal-gas cycle operates as follows: 1. From an initial state (##p_1##, ##V_1##) the gas is cooled at constant pressure to (##p_1##, ##V_2##); Let's call the start and end temperature ##T_1## and ##T_2## 2.The gas is heated at constant volume to (##p_2##, ##V_2##);Lets call the...
  7. Toby_phys

    Quantum - infinite chain of wells

    An electron can tunnel between potential wells. Its state can be written as: $$ |\psi\rangle=\sum^\infty_{-\infty}a_n|n\rangle $$ Where $|n \rangle$ is the state at which it is in the $n$th potential well, n increases from left to right. $$...
  8. Toby_phys

    Boltzmann vs Maxwell distribution?

    Why are the states counted in momentum space?? I haven't seen a derivation where this is necessary
  9. Toby_phys

    Boltzmann vs Maxwell distribution?

    So I worked through the Boltzmann distribution and got: $$ P\propto e^{\frac{-E}{k_BT}} $$ Where $E$ is the energy. So surely this means the kinetic energy (and therefore speed) of particles is distributed over a Boltzmann distribution. Or in equation: $$ P\propto e^{\frac{-mv^2}{2k_BT}} $$...
  10. Toby_phys

    Lorentz force - particle in an odd magnetic field

    Homework Statement Particles of mass ##m## and charge ##q## are initially traveling in a beam along the ##z## direction with speed ##v## when they enter a long magnetic quadrupole lens, where there is no E-field and the magnetic flux density is ##B = Ay\hat{i} + Ax\hat{j}##, and where A is a...
  11. Toby_phys

    Line Integrals around a Square on the x-y Plane

    Homework Statement Evaluate the following line integrals, showing your working. The path of integration in each case is anticlockwise around the four sides of the square OABC in the x−y plane whose edges are aligned with the coordinate axes. The length of each side of the square is a and one...
  12. Toby_phys

    The slowing down of a Farady disc

    Yes, I think :) $$\frac{dE}{dt}=\frac{15Ba^2}{32}^2\frac{\dot{\theta}^2}{R_l+R_d}=\frac{15Ba^2}{32}^2\frac{4E}{ma^2(R_l+R_d)}$$ Which is seperable.Edit - I have worked through it all and it works, thank you
  13. Toby_phys

    The slowing down of a Farady disc

    I thought about that but I couldn't see how to do it
  14. Toby_phys

    The slowing down of a Farady disc

    Mechanical energy is lost at the same rate that energy is dissipated through the resistances. I could go into forces and go right back to first principles but I feel that would be far too long
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