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... force within the conductor is equal to zero. Thus, the electric field inside of the conductor is zero. ...
Year 12 Physics Term 3 Unit 4 Plan
Year 12 Physics Term 3 Unit 4 Plan

... Accurate and successful completion of problems from the textbook. ...
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... 4. Why does electric discharge occur? due to the difference in charge. The build up of negative charges in an object is attracted to a positively charged object; therefore, the electrons move from negative to positive. Lightening is an example of electric discharge 5. What is a circuit? a complete p ...
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... magnetic flux changes by ∆B, and a voltage U will be induced in the wire coil given by A · ∆B U= ∆t With A = cross-sectional era of the torus This is of course nothing but the well-known effect of self-inductance - you cannot turn on a current very quickly that is flowing through a large inductance. ...
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... magnetic flux changes by ∆B, and a voltage U will be induced in the wire coil given by A · ∆B U= ∆t With A = cross-sectional era of the torus This is of course nothing but the well-known effect of self-inductance - you cannot turn on a current very quickly that is flowing through a large inductance. ...
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... substances that have high ___________________________________ – substances usually containing __________________________. ...
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... Magnet – Any material that attracts iron or materials containing iron Poles – The parts of the magnets where the magnetic effects are strongest Magnetic Force – The force of repulsion or attraction between the poles of magnets Electromagnetism – The interaction between electricity and magnetism Sole ...
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Transient responses due to various burial depths on a single long
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... 4). A slab of dielectric of relative permittivity ε is placed in a uniform external field E whose field lines make an angle θ with a normal to the surface of the slab. What is the density of polarisation charge on the surface of the slab? Hint: Consider the total field inside the slab, which is the ...
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... • Current carrying conductor of length l and crosssectional area A, having resistance R, with a potential difference across it of ΔV l Re member R   , I  j  A, & V  E  l A If V  I  R ...
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... We have seen that a conductor experiences a force when it carries current perpendicular to a magnetic field. This is the basis for the electric motor. What will happen if the same set up is utilised but with no supplied current & with an external force providing perpendicular motion to the wire? ...
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Skin effect



Skin effect is the tendency of an alternating electric current (AC) to become distributed within a conductor such that the current density is largest near the surface of the conductor, and decreases with greater depths in the conductor. The electric current flows mainly at the ""skin"" of the conductor, between the outer surface and a level called the skin depth. The skin effect causes the effective resistance of the conductor to increase at higher frequencies where the skin depth is smaller, thus reducing the effective cross-section of the conductor. The skin effect is due to opposing eddy currents induced by the changing magnetic field resulting from the alternating current. At 60 Hz in copper, the skin depth is about 8.5 mm. At high frequencies the skin depth becomes much smaller. Increased AC resistance due to the skin effect can be mitigated by using specially woven litz wire. Because the interior of a large conductor carries so little of the current, tubular conductors such as pipe can be used to save weight and cost.
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