https://www.physicsforums.com/showthread.php?t=195357
i would like to share some ideas.
i agree with ranger. increasing the cross-sectional area of the WIRE will decrease the DC resistance of the coil.
R = ρ*L/A
ρ = resistivity of the material used for the wire
L = length of the wire
A = cross-sectional area of the wire
and then the inductance of the coil will decrease when the cross-sectional area of the COIL is decreased or if the number of turns is decreased. this is in virtue of the equation
L = μ(N^2)A/s
A = cross-sectional area
s = length of the coil
N = number of turns
μ = permeability of free space
because the magnetic field would not be uniform if N is decreased, it is safer if you make the cross-sectional area of the COIL smaller. @tonytuong: maybe this may help for your problem.
the inductance will affect the AC resistance <the impedance> because the impedance of the ideal transformer <ignoring DC resistance of the wire> is jωL. this is the case for LONE COILS.
j = sqrt(-1)
ω= angular freq
L = inductance
we got this in class. the proving part for here is too long :(
the internal resistance of the wires used in the inductor can be modeled as a small resistance in series with an ideal inductor
about transformers:
actually the input impedance reflected at the primary is dependent on the LOAD connected to the secondary side.
using the equation (1) V2 = (n2/n1)*V1
V2 = voltage in secondary || n2 = turns at the secondary side
V1 = voltage in primary || n1 = turns at the primary
equation (2) I2 = (n1/n2)*I1
I2 = current through the secondary || n2 = turns at the secondary side
I1 = current through the primary || n1 = turns at the primary side
equation (2) should be agreeing with (1) because POWER IN = POWER OUT.
try to multiply these two equations to get V1*I1 = V2*I2!
and then try to DIVIDE equation (1) with (2) and you shall get:
V2/I2 = (n2/n1)^2*V1/I1 ===========> V1/I1 = (n1/n2)^2*V2/I2
V1/I1 = impedance when viewed from the primary side (Z1)
V2/I2 = impedance when viewed from the secondary side (Z2)
so from the above equations we can conclude that the input impedance of the TRANSFORMER when VIEWING FROM THE PRIMARY SIDE is DEPENDENT on the impedance on the secondary side, which is (n1/n2)^2*Z2!
this means that the transformer <along with the load on the secondary side> can be modeled ON THE PRIMARY SIDE as an impedance with Z = (n1/n2)^2*Z2 just to simplify calculations.
remember:
DC resistance α cross-sectional area of the WIRE
AC resistance α cross-sectional area of the COIL WINDINGplease correct me if something in my post is wrong. I am just a student. sorry =)