16  Analogue Recording and Reproduction

Formulae

Magnetomotive force, m.m.f is given by

m.m.f. = NI

where N is the number of coil turns and I is the current.

The units of m.m.f are ampere turns/meter (At/m)

The intensity or field strength is the total force acting per unit length I of the magnetic circuit. It is called the magnetizing force H.

H = m.m.f./l = NI/l(AT/m)

The magnetizing force causes a flux Ф in the magnetic circuit.

The flux density B is the flux per unit area. The unit is the tesla (= webers/m2).

Ф = m.m.f./S

where S is the reluctance of the circuit.

Figure 73 shows a typical BH loop (hysteresis loop).

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Figure 73  Hysteresis loop

Magnetic Tape – Typical Characteristics

Base material – Mylar

Base thickness – 25 to 40 μm

Coating, commonly ferric oxide (Fe2O3) in the form of needle-shaped particles roughly 0.6 to 1 μm in length and less than one-tenth of that in diameter.

Coating thickness – 10 to 15 μm.

Tape Transfer Characteristic

Figure 74 shows the distortion that would arise if corrective measures (bias) were not applied.

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Figure 74  Tape transfer characteristic

Tape Head Data

Typical head gaps for 38 cm/s (15 in/s) tape speeds:

Erase head: ~ 100 μm

Record head: ~ 20 μm

Replay head: ~ 5-10 μm or less

Recorded Wavelengths

The recorded wavelength is the length on the tape of one cycle of the recorded signal.

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Standard tape widths

  Tape width

Typical use

(mm)

(in.)

 

  3.8

5/32

Cassettes

  6.25

1/4

Mono full-track, 1 or 2 track, stereo

12.5

1/2

Stereo mastering, 4 track

25

  1

4-track mastering, 8 track

50

  2

16 track, 24 track

In the table below the recorded wavelengths are given in cm.

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Comparison of hysterisis loops for tape material and head cores

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Figure 75  Hysteresis loops for (a) ‘hard’ magnetic material – tape oxide; (b) ‘soft’ – head core material

Bias

Bias Frequency

This should be about 4–6 times the highest recorded signal – i.e. around 100 to 150 kHz. Lower bias frequencies may result in undesirable intermodulation products. For example, if the bias frequency were 30 kHz and the highest audio frequency were 18 kHz then there will be sum and difference intermodulation frequencies of 48 kHz and 12 kHz, the latter falling into the audible range.

Optimum Bias Setting

This is represented graphically in Figure 76.

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Figure 76  Illustrating optimum bias setting

Replay Amplifier Equalization

Used to compensate for losses caused by the gap length, the thickness of the tape coating and in the pole pieces, etc.

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Figure 77 (a)  Equivalent circuit of a standard replay response; (b) replay head and amplifier response for an ideal head; (c) real replay head and amplifier responses

Standard Equalizations in IEC and NAB Standards

These are given as the relevant time constants τ, where

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Tape speed

IEC1

IEC2 and NAB

9.5 cm/s; 3/75 in/s

-

50 Hz; 1800 Hz

 

 

3150 μs; 90 μs

 

 

(NAB only)

19 cm/s; 7.5 in/s

0 Hz; 2240 Hz

50 Hz; 3150 Hz

 

(∞, 70 μs)

(3150 μs; 50 μs)

38 cm/s; 15 in/s

0 Hz; 4500 Hz

50 Hz; 3150 Hz

 

(∞, 35 μs)

(3150 μs; 50 μs)

76 cm/s; 30 in/s

(IEC1 not used)

AES 1971

 

0 Hz; 4500 Hz

0 Hz; 9000 Hz

 

(∞, 35 μs)

(∞ μS; 17.5 μs)

Head Track Formats

See Figure 78.

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Figure 78  Head track formats

Cassettes

Track layout. See Figure 79.

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Figure 79  Audio cassette tape

Mechanical Adjustments of a Tape Head

See Figure 80.

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Figure 80  Illustration of azimuth and zenith adjustments

Level

The tone section of a tape is usually recorded at 700 Hz or 1 kHz. The exact frequency is not usually critical. The exact level is, however, important. It is taken as the 0 dB reference but if it is not the reference fluxivity required the example on page 121 shows how to make a correction.

Assume that the machine needs to be aligned to the NAB characteristic at 320 nWb/m for 0 VU = +4 dBm. The reference fluxivity on the tape is 200 nWb/m. The reference fluxivity difference is calculated from

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In the example given above:

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