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The Ring Head and the Recording Gap
Volt

创建者

Volt

30. 八月 2026SE
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The Ring Head and the Recording Gap

Poulsen recorded on magnetised steel wire in 1898, running the wire past the pole of an electromagnet. It worked and it was crude: the pole's field spread along the wire, so every mark it wrote was long. Eduard Schüller at AEG patented the fix in 1933 and it is still in every drive built today. Bend the magnetic circuit into a RING, and cut one narrow non-magnetic slot in it. Almost all the flux now stays inside the high-permeability core, because that is the easy path, except at the slot, where it has to jump. The fringing field that bulges out of that slot is intense, and it is confined to roughly the slot's own width. The gap does not conduct the flux; it is the one place the flux is forced out into the world, and that is the entire trick. The same ring reads. A magnetised medium moving past the gap pushes flux through the core, and a coil around the core sees a voltage. So the gap length decides both halves at once: the shortest mark you can write, and the shortest wavelength you can read. When the recorded wavelength equals the gap length, the gap averages over exactly one full cycle and the output goes to zero. Every advance in magnetic storage since is, in large part, that slot getting narrower and the medium getting closer. This blueprint is fully buildable: wind a coil on a pair of ferrite U-cores, set the gap with a foil shim, and measure both the 6 dB per octave rise and the cliff it falls off.
中级
4 hours

说明

1

Wind the head and set the gap

Use a pair of ferrite U-cores: two halves that close into a rectangular ring, with mating faces already ground flat. Real ring heads are built the same way, from two halves, and it gives you two joints. One becomes the gap; the other must close as tightly as you can make it. (A ferrite toroid has no joint to open, and ferrite is too hard to cut cleanly without a diamond saw.) Wind 200 turns of 0.2 mm enamelled wire on one leg and scrape the enamel off the two ends. Close the halves with no shim and measure the inductance on the LCR meter; measure again once the gap is in. Ferrite is so permeable that even a few micrometres of non-magnetic gap in series with it lowers the inductance clearly, and that drop is your first proof the gap is there. Put the shim in ONE joint only, the one the tape will run over. It must be non-magnetic. Household aluminium foil is about 16 micrometres thick; measure yours with the micrometer, and stack layers for a wider gap. Never use a steel feeler gauge or a razor blade: steel is magnetic and would bridge the very gap it is meant to create. Close the other joint face to face with nothing between, and clamp or glue the halves so the faces stay parallel. The tape runs across the outside of the gapped leg. Smooth that face with 600-grit wet paper on a sheet of glass so the medium can pass within a hair of it. Spacing costs more than anything else you can get wrong here, and the notebook shows how much.

此步骤所需材料:

铁氧体 U 型磁芯(一对)铁氧体 U 型磁芯(一对)1 个
漆包铜线漆包铜线10 米
铝箔铝箔1 张

所需工具:

千分尺千分尺
LCR 测试仪 - 数字式LCR 测试仪 - 数字式
砂纸套装砂纸套装
6 英寸数显卡尺6 英寸数显卡尺
2

Build the read amplifier

A head winding delivers microvolts, so the first stage sets the noise floor and nothing after it can recover what that stage throws away. Bring the two leads to the amplifier as a twisted pair and amplify only their DIFFERENCE: U1A, an OPA1612 wired as a difference amplifier with a gain of 100. Hum from the motor arrives on both leads alike and cancels. In ngspice, 100 mV of 50 Hz hum on both leads left 1 mV at the output, with one of the four resistors deliberately 1 % off. A single-ended stage would have amplified the same hum 100 times and clipped. C_EQ and C_EQ2, 220 pF across the two 100k resistors, are the equalisation. Read-back rises 6 dB per octave on its own, so above 7.2 kHz the amplifier falls at the same rate and flattens the top of the band. Leave both out for the sweep in the next step, so the gain is a flat 100 and you measure the head, not the equaliser. The differentiator and comparator after it recover DATA rather than audio. A recorded bit is a flux REVERSAL, which shows up as a peak in the read voltage. U2A differentiates about a 2.43 V reference, so each peak becomes a zero crossing, and U3A, an LM393, turns each crossing into one edge. R_HYS sets its hysteresis window, which has to be right both ways. Simulated with 200 µV read pulses and 20 µV rms of noise: 330k gave one edge per transition in four of five noise runs and one extra edge in the fifth; with almost no hysteresis, 91 edges for 11 transitions; at 150k to 220k the window was too wide and transitions were lost. The edges came 25 to 35 µs after each peak. Power the op-amps from two 9 V batteries as +9 V and −9 V, and the LM393 from +9 V and ground. Its output is open collector, so return R_PU to the supply of whatever logic reads the pulses. The simulation used behavioural op-amp models, not the vendors' models.

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此步骤所需材料:

低噪声运算放大器(OPA1612)低噪声运算放大器(OPA1612)1 个
运算放大器集成电路运算放大器集成电路1 个
电阻套件电阻套件1 个
电容套件电容套件1 个
LM393 双比较器集成电路LM393 双比较器集成电路1 个
9V Li-ion Rechargeable Battery - 350mAh9V Li-ion Rechargeable Battery - 350mAh2 个
电池座电池座2 个

所需工具:

Breadboard - ClassicBreadboard - Classic
跳线套装跳线套装
数字示波器数字示波器
3

Sweep it and find your own gap

Glue a strip of cassette tape, coated side out, around the rim of a wheel on the geared motor, and hold the head against it on a sprung arm with the gapped face on the tape. Run the motor from the bench supply and measure the rim speed with the optical tachometer: a few tenths of a metre per second is plenty. Record first. Disconnect the amplifier and drive the head winding from the function generator through a 1 k resistor at its full output, one frequency at a time, for at least one turn of the wheel. Then disconnect the generator, reconnect the amplifier with C_EQ and C_EQ2 left out, and read the peak-to-peak amplitude at U1A's output. Step through the frequencies. The wavelength on the tape is the rim speed divided by the frequency. The output climbs at 6 dB per octave, peaks, then collapses. At the gap's first null it nearly vanishes: there the wavelength is about equal to the gap, a little longer in practice because the field fringes past the gap's edges. At 0.3 m/s, one layer of foil puts that null near 19 kHz. Cross-check it against the shim you measured. Then repeat one point with a sheet of paper between head and tape. That single measurement is the most important number in this blueprint.

此步骤所需材料:

盒式磁带盒式磁带1 个

所需工具:

函数发生器函数发生器
数字示波器数字示波器
数字转速表数字转速表
直流减速电机直流减速电机
台式电源台式电源
4

Gap loss, spacing loss, and the fit

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所需工具:

台式电脑台式电脑
5

Compendium: the head stores nothing

THE HEAD STORES NOTHING. A ferrite core stores its bit IN itself; the ring head has the same hysteresis loop and stores nothing at all. It is a transducer. Which is why a head is made of the SOFTEST magnetic material available — low coercivity, lets go instantly — and the medium of the hardest. Same physics, opposite ends. THE GAP IS A SPACER, NOT A HOLE. It is filled with glass or a hard non-magnetic alloy. It has to survive years of contact without the edges rounding over, because a rounded edge is a wider gap and a wider gap is a lower ceiling. IF IT DOES NOT WORK. No output: the gapped joint is not the one under the tape, or the other joint is not closed, so a second gap is wasting the winding's drive; butt it face to face. Output that does not change when you lift the head off the tape is not playback: it is hum or the motor's field reaching the winding, so twist the leads, move the motor away and screen the head. Double pulses per transition: too little comparator hysteresis. Missing pulses: too much.

材料

11

所需工具

12
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$11.28

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