How do I use a transformer as an inductor?
How do I obtain an inductor from the given transformer in the image? ... So that the inductance of the resulting inductor must be maximum.
Connect the undotted end of one winding to the dotted end of the other.
eg P2 to S1 (or P1 to S2) and use the pair as if they were a single winding.
(As per example in diagram below)Using just one winding does NOT produce the required maximum inductance result.
The resulting inductance is greater than the sum of the two individual inductances.
Call the resultant inductance Lt,- Lt > Lp
- Lt > Ls
- Lt > (Lp + Ls) !!! <- this may not be intuitive
- \$ L_t = ( \sqrt{L_p} + \sqrt{L_s}) ^ 2 \$ <- also unlikely to be intuitive.
- \$ \dots = L_p + L_s + 2 \times \sqrt{L_p} \times \sqrt{L_s} \$
Note that IF the windings were NOT magnetically linked (eg were on two separate cores) then the two inductances simply add and Lsepsum = Ls + Lp.
What will be the frequency behavior of the resulting inductor? Will it have a good performance at frequencies other than the original transformer was rated to run in.
"Frequency behavior" of the final inductor is not a meaningful term without further explanation of what is meant by the question and depends on how the inductor is to be used.
Note that "frequency behavior" is a good term as it can mean more than the normal term "frequency response" in this case.
For example, applying mains voltage to a primary and secondary in series, where the primary is rated for mains voltage use in normal operation will have various implications depending on how the inductor is to be used.Impedance is higher so magnetising current is lower so core is less heavily saturated. Implications then depend on application - so interesting. Will need discussing.
Connecting the two windings together so that their magnetic fields support each other will give you the maximum inductance.
When this is done
the field from current in winding P will now also affect winding S
and the field in winding S will now also affect winding P
so the resultant inductance will be greater than the linear sum of the two inductances.
The requirement to get the inductances to add where there 2 or more windings is that the current flows into (or out of) all dotted winding ends at the same time.
- \$ L_{effective} = L_{eff} = (\sqrt{L_p} + \sqrt{L_s})^2 \dots (1) \$
Because:
Where windings are mutually coupled on the same magnetic core so that all turns in either winding are linked by the same magnetic flux then when the windings are connected together they act like a single winding whose number of turns = the sum of the turns in the two windings.
ie \$ N_{total} = N_t = N_p + N_s \dots (2) \$
Now:
L is proportional to turns^2 = \$ N^2 \$
So for constant of proportionality k,
\$ L = k.N^2 \dots (3) \$
So \$ N = \sqrt{\frac{L}{k}} \dots (4) \$
k can be set to 1 for this purpose as we have no exact values for L.
So
From (2) above: \$ N_{total} = N_t = (N_p + N_s) \$
But : \$ N_p = \sqrt{k.L_p} = \sqrt{Lp} \dots (5) \$
And : \$ N_s = \sqrt{k.L_s} = \sqrt{L_s} \dots (6) \$
But \$ L_t = (k.N_p + k.N_s)^2 = (N_p + N_s)^2 \dots (7) \$
So
\$ \mathbf{L_t = (\sqrt{L_p} + \sqrt{L_s})^2} \dots (8) \$
Which expands to: \$ L_t = L_p + L_s + 2 \times \sqrt{L_p} \times \sqrt{L_s} \$
In words:
The inductance of the two windings in series is the square of the sum of the square roots of their individual inductances.
Lm is not relevant to this calculation as a separate value - it is part of the above workings and is the effective gain from crosslinking the two magnetic fields.
[[Unlike Ghost Busters - In this case you are allowed to cross the beams.]].
Just use the primary or the secondary with the other winding open-circuit. If you use the primary, the inductance will be \$L_P\$, and if you use the secondary it will be \$L_S\$ - by definition.
But I'm not sure what you are expecting to do with this (you say you don't want to use any other circuit elements .... ?).
The frequency response will depend on what other circuit elements you use. Assuming you are trying to implement an L/R or L/C low-pass filter, a mains transformer should give rejection up to a few tens of kHz before other factors (such as winding capacitance) have an effect.
Be aware though that the primary of a mains transformer will have higher inductance and will be rated for higher voltage and lower current than the secondary. You should also ensure that if you do not use one winding is well insulated, especially if you are using the secondary. This is because very high voltages could be induced in the primary if the secondary current changes rapidly.
EDIT
I see from your edits that you want to connect the windings together. The primary and secondary inductances can be calculated from their turns by the formulae ..
SECOND EDIT
I have rewritten this next part to make it less mathematical, more intuitive, and to distinguish it from other answers here.
The voltage induced across an inductor is proprrtional to the rate of change of current through it, and the constant of proportionality is the inductance L.
V1 = L * (rate of change of current through winding)
With coupled coils, the induced voltage has an extra factor due to the rate of change of current through the other winding, the constant being the mutual inductance Lm.
V2 = Lm * (rate of change of current through the other winding)
So in general, the voltage across the inductor is the sum of these:- (using your symbols)
Vp = Lp * (rate of change of primary current) + M * (rate of change of secondary current)
and for the secondary :-
Vs = Ls * (rate of change of secondary current) + M * (rate of change of primary current)
If we wire the primary and secondary in series, the currents are the same and the voltages will add or subtract,
depending on which way round we connect the windings together.
\$V_{total} = V_P \pm V_S = ( L_P \pm L_M + L_S \pm L_M )\$ * (rate of change of current)
SUMMARY
But this is just the same as if we had an inductor with inductance :-
\$L_t = L_p + L_s \pm 2L_m\$
If we connect the windings so that S1 is connected to P2, the current will flow the same way through both windings, the voltages will add and we maximize the inductance, so :-
\$L_t = L_p + L_s + 2L_m\$
If there is no coupling (for instance if the windings were on separate cores), the mutual inductance will be zero and the primary and secondary inductances will add as you might expect. If the coupling is less than perfect, a proportion k of the flux from one winding will couple into the other winding, with k varying from 0 to 1 as the coupling improves. The mutual inductance can then be expressed as :-
\$L_m = k\sqrt{L_pL_s}\$
and
\$L_t = L_p + L_s + 2k\sqrt{L_pL_s}\$
This is the same as Russell's answer if k=1 (perfect coupling) but I disagree that the mutual inductance is not relevant. It is.