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RegisterNow and claim your 100% FREE exclusive updates! You are about to proceed to “Confirm Your Email Address”. As a Thank You, We Will Send Your Cd Key For Crack User to Crack-Cd.com Premium Registration Page Now! the trace of the supercurrent dipole moment. Each superconductor will be located in contact with at least one normal metal. The charge Q of a superconducting wire with transition length l0 is nonzero, because in the limit l0 → 0 the wire cannot exist as it does not fulfil the boundary condition at l0; Q is a quantity of the order of l0. Charge Q is the only source term of the boundary condition equation (7); it appears as the source current term on the right-hand side. The differential equation (9) is a generalisation of the diffusion equation, and it has the following solution: (23) (24) (25) where is the space–charge screening length, which can be calculated from the solution to the potential equation (19), is the space–charge screening voltage, and is the time derivative of the electric potential (8). The solution (25) to the potential equation is found using the data: (26) Using the boundary condition (20), the solution to the potential equation (25) can be calculated. For the AC loss tensor ηN and ηS one obtains (27) (28) (29) (30) where is the frequency of the AC current at the boundary, is the DC voltage at the boundary, is the current at the boundary, is the transition length between the superconducting and normal metal, and is the length of the normal metal. Transition lengths below 0.1 µm The transition length between the superconducting and normal metal is approximately equal to the London penetration depth, (31) The characteristic lengths and can be measured experimentally, see Table 1. It is not possible to measure the diffusion length accurately on practice, and we use here for simplicity, the value 50 nm in all calculations. However, the London penetration depth does depend on the applied magnetic field and it can be calculated using, for example, the BCS model. Figure 5 shows results for transition lengths below

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