EE340_Manual_061
... In all of the measurements, make sure that the lines are fully extended (no loops). Also, avoid areas of electromagnetic interference inside the lab. 1. Measure the capacitance of the coaxial transmission line using the universal bridge. The far end of the line should be open-circuited. 2. Measure t ...
... In all of the measurements, make sure that the lines are fully extended (no loops). Also, avoid areas of electromagnetic interference inside the lab. 1. Measure the capacitance of the coaxial transmission line using the universal bridge. The far end of the line should be open-circuited. 2. Measure t ...
Solvable Examples of Drift and Diffusion of Ions in Non
... The factor [det(I + g)]1/2 ensures that ψ is normalized properly: Z ...
... The factor [det(I + g)]1/2 ensures that ψ is normalized properly: Z ...
Optics I - Department of Applied Physics
... permittivity constant (介电常数): 0 8.85 10 C /N m Note that this satisfies Newton's third law because it implies that exactly the same magnitude of force acts on q2 . Coulomb's law is a vector equation and includes the fact that the force acts along the line joining the charges. Like charges rep ...
... permittivity constant (介电常数): 0 8.85 10 C /N m Note that this satisfies Newton's third law because it implies that exactly the same magnitude of force acts on q2 . Coulomb's law is a vector equation and includes the fact that the force acts along the line joining the charges. Like charges rep ...
Final report - ECMI Modelling Week
... the torque for a given geometry of the rotor. To create this geometry we have limited ourselves to setting up just a quadrilateral in a first quarter of the rotor. We reflect the created shapes to the other quarters to obtain complete geometry. In order to setup the geometry we have created a Matlab ...
... the torque for a given geometry of the rotor. To create this geometry we have limited ourselves to setting up just a quadrilateral in a first quarter of the rotor. We reflect the created shapes to the other quarters to obtain complete geometry. In order to setup the geometry we have created a Matlab ...
Lecture Notes 04: Work and Electrostatic Energy
... charge distribution i.e. one which has finite spatial extent {with characteristic size ~ d}, far away from the localized charge distribution, if there is a net electric charge associated with the localized charge distribution, then V ( r d ) ~ 1 r and E ( r d ) = −∇V ( r d ) ~ 1 r 2 . If the localiz ...
... charge distribution i.e. one which has finite spatial extent {with characteristic size ~ d}, far away from the localized charge distribution, if there is a net electric charge associated with the localized charge distribution, then V ( r d ) ~ 1 r and E ( r d ) = −∇V ( r d ) ~ 1 r 2 . If the localiz ...
Quantum anomalous Hall effect with cold atoms trapped in a square
... frequencies for the lattice [19]. To break TR symmetry, we introduce a periodic adiabatic gauge potential in the simple form A(r) = h̄A0 sin[k0 (y − x)]ey , with A0 a constant, which can be generated by coupling atoms to two opposite-travelling standing-wave laser beams with Rabi-frequencies 1 = ...
... frequencies for the lattice [19]. To break TR symmetry, we introduce a periodic adiabatic gauge potential in the simple form A(r) = h̄A0 sin[k0 (y − x)]ey , with A0 a constant, which can be generated by coupling atoms to two opposite-travelling standing-wave laser beams with Rabi-frequencies 1 = ...
A critique of recent semi-classical spin-half quantum plasma theories
... orbit theory”. Specifically, if the time rate of change of the fields is measured by the frequency ω and the spatial scales are represented by the wave number k , drift orbit theory may be used when ρ∗ = Max[kρe , ωωce ] ≪ 1. Here, c⊥ is the “peculiar velocity” of the electron’s Larmor gyro motion. ...
... orbit theory”. Specifically, if the time rate of change of the fields is measured by the frequency ω and the spatial scales are represented by the wave number k , drift orbit theory may be used when ρ∗ = Max[kρe , ωωce ] ≪ 1. Here, c⊥ is the “peculiar velocity” of the electron’s Larmor gyro motion. ...
