184_notes:examples:week14_step_down_transformer

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Recall the discussion on voltage transformers. We designed a step-up transformer in the notes, which is used to convert small voltages from a generator into high voltages, which get carried long distances to residential areas. High-voltage power lines are dangerous, though, because the potential difference between the power lines and the ground is so enormous. Before the lines enter a residential area, they are sent to a transformer, from which low-voltage lines carry power to the residential area. How can you design a step-down transformer to convert a line that has a $240 \text{ kV}$ potential difference to ground, into a power line that has a $120 \text{ V}$ potential difference to ground?

Facts

  • The high-voltage line carries $240 \text{ kV}$.
  • We want the low-voltage line to carry $120 \text{ V}$.
  • We know the step-up transformer was created by wrapping two solenoids around an iron torus, and connected the high-voltage line to one solenoid, and the low-voltage line to the other. The low-voltage solenoid had fewer turns. A more detailed representation is shown below.

Lacking

  • We need a design for the step-down transformer.

Approximations & Assumptions

  • We have access to the same materials as we did for the step-up transformer.
  • The step-down transformer we are building will have a similar design to the step-up transformer.

Representations

  • We represent magnetic flux as $$\Phi_B = \int \vec{B} \bullet \text{d}\vec{A}$$
  • We can represent induced voltage as $$V_{ind} = -\frac{\text{d}\Phi}{\text{d}t}$$
  • We represent the step-up transformer, as described in the Facts, with the following visual:

Step-up Transformer

It makes sense intuitively to just flip the step-up transformer for our design. If the step-up transformer brings voltage down, we could just reverse it to bring the voltage up. Our design is shown below, where the number of turns in the primary solenoid is much greater than the number of turns in the secondary solenoid – it's just the flipped step-up transformer, as described.

Step-down Transformer

As with the step-up transformer, the two solenoids are wrapped around the same iron torus. When current exists in the primary solenoid, it creates a magnetic field inside the solenoid, aligned along the torus. The magnetic field from the solenoid will cause all of the atoms within the iron to align with the magnetic field from the primary solenoid. Because iron atoms are very responsive to magnetic fields, even the atoms that are outside the primary solenoid will align with this magnetic field (largely because they are feeling the effects of their neighboring iron atoms). Because the magnetic field in the primary solenoid is oscillating (due to the alternating current), this means that the magnetic field in all of the iron ring is also constantly changing. For snapshot in time, the field may look like this:

Step-down Transformer with B-field

The iron is able to align its atoms with the magnetic field much faster than the current alternates between directions, which is why we draw the magnetic field the same everywhere. The iron also greatly amplifies the magnetic field that the primary solenoid would produce in air, so even though $B_P$ contains magnetic field contributions from the primary solenoid and from the iron, the contribution from the iron is far greater. For this reason, we approximate the magnetic field as the same at all locations in the iron. By this approximation, $B_P = B_S$.

Since the magnetic field is changing with the alternating current, (in the primary solenoid), this will induce a voltage ($V_S$) in the secondary solenoid. We can use Faraday's Law to write this as: $$-V_{S}=\frac{d\Phi_{B_{S}}}{dt}$$

The rest of our calculation follows just as it would for the analysis of the step-up transformer. We can then rewrite the flux $\Phi_{B2}$ using the flux definition: $$\Phi_{B_{S}}=\int \vec{B}_S \bullet \vec{dA}_S$$ where the area here would be the cross-sectional area of the iron ring (since this is where the magnetic field is). The direction of the magnetic field would always be perpendicular to the area of the cylinder - so the flux would simplfy to: $$\Phi_{B_{S}}=B_S A_S$$ But this is the magnetic flux through one loop in the secondary solenoid - if we want the total flux through all the loops then we have to multiply by the number of loops: $$\Phi_{B_{S}}=B_S A_S N_S$$ We can then plug this into the voltage equation we wrote above: $$-V_{S}=\frac{d}{dt}\biggl(B_S A_S N_S\biggr)$$

Since $N_S$ and $A_S$ are constant with respect to time (not add/taking away loops or increasing/decreasing the area), these terms can come out of the derivative: $$-V_{S}=N_S A_S \frac{d}{dt}\biggl(B_S\biggr)$$ If we assume that the ring has a constant cross-sectional area, then $A_P=A_S$ and we already said that $B_P=B_S$. This means we can rewrite the flux through the secondary solenoid in terms of the magnetic field and area of the primary solenoid. $$-V_{S}=N_S A_P \frac{d}{dt}\biggl(B_P\biggr)$$

If we look at the $A_P\frac{d}{dt}\biggl(B_P\biggr)$ term, this looks very much like the changing magnetic flux (or induced voltage) through a single loop of the primary solenoid: $$\frac{d\Phi_{B_{P}}}{dt}=\frac{d}{dt}\biggl(B_P A_P\biggr)$$ If we use Faraday's Law, we can rewrite the flux through a single loop of the primary solenoid in terms of the number of coils and the induced voltage in the whole solenoid: $$-V_P=N_P \frac{d}{dt}\biggl(B_P A_P\biggr)$$ $$\frac{d}{dt}\biggl(B_P A_P\biggr)=\frac{-V_P}{N_P}$$

Finally, We can plug this result into the $V_S$ equation above to get the potential in the secondary solenoid as it relates to the potential in the primary solenoid: $$-V_S = N_S \frac{-V_P}{N_P}$$ $$V_S=V_P \frac{N_S}{N_P}$$

This equation then tells us that that if we want the voltage in the secondary solenoid to be 100 times greater than the voltage in the primary solenoid, the secondary solenoid must have 100 times as many loops as the primary solenoid! Remember that even though there are not explicit sines or cosines in our equation, this whole process hinges on the fact that the current, and thus magnetic field and voltage, are oscillating. You would not be able to make a voltage transformer in the same way using a direct current because there would no longer be a changing magnetic flux. (This was one of the biggest arguments made back in the 1880s for using alternating current in the power grid rather than direct current.)

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  • Last modified: 2017/11/29 16:49
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