1056 Chapter 28
(28-5)
where,
x is 2 S× thickness/wavelength.
Although this expression yields a drop of 6 dB per
octave, as shown in Fig. 28-18, this curve is not the
same shape as the response of a low-pass filter made
from a resistor and capacitor. The response in Fig.
28-18 is down 4 dB at the intersection of the asymptotes
rather than the typical 3 dB for a single pole RC filter.
This difference in shapes means that a simple RC boost
circuit will not properly correct for the thickness loss.
Depending on the choice of RC boost frequencies, the
difference in shape will produce an error of 0.5–1.0 dB
in the midband response.
28.3.2.1 Equalization Boosts
This thickness loss of Fig. 28-22, must be corrected by
applying compensating boosts in either the record or
reproduce circuitry. Although this loss is a playback
deficiency, the choice of whether to correct the loss
during record or playback is somewhat arbitrary. The
amount of record boost is limited by the magnetic satu-
ration characteristics of the tape; playback boost is
limited by the high-frequency noise characteristics of
the tape and the reproduce head and associated circuitry.
The minimum amount of boosting required to
achieve flat response can be considered to be a neces-
sary equalization. The industry has developed a set of
internationally recognized standards to promote
compatibility of tapes. Each standard deals with the
necessary and discretionary equalizations to define the
exact characteristics of the recorded tape. Using the tape
flux characteristics as a standard implicitly specifies the
partitioning of equalizations between the recording and
reproducing functions. Table 28-4 lists the commonly
encountered standards.
Unlike the absolute nature of the reproduce charac-
teristics, the record characteristics of the recorder must
have enough flexibility to accommodate a number of
different tape sensitivities and frequency characteristics.
Once the reproduce section has been calibrated to the
standard with a standard alignment tape, all further
adjustments are to produce a recorded tape on the
machine that accurately matches the standard tape.
The amount of thickness loss can always be reduced
by utilizing thinner coatings, but any decrease in thick-
ness also causes an equal drop in low- and midfrequency
output and SNR. To preserve the existing standards, the
tendency has been to adjust the coating thickness of new
tapes to emulate the high-frequency losses of the older
tape types while trying to achieve maximum low- fre-
quency output. This somewhat self-defeating strategy
has been overcome in recent thin-coat high-energy tapes
Figure 28-18. Loss due to ratio of coating thickness to
wavelength.
Coating thickness lossdB 20 x
1 – e–x
= log----------------
0
10
20
30
.01 0.1 1.0 10
T/L—Thickness/wavelength
Output in dB
A. 15 kHz 30 in/s T = 0.65 mil ( 7.4 dB)
B. 15 kHz 15 in/s T = 0.65 mil ( 12.4 dB)
C. 15 kHz 1^7 / 8 in/s T = 0.2 mil ( 20.0 dB)
D. 15 kHz 1^7 / 8 in/s T = 0.65 mil ( 30.3 dB)
E. Digital 30 kbit/in T = 0.2 mil ( 31.5 dB)
A
B
C
D
E
20log^2 P × T/L
1 e^2 P4/L
Table 28-4. Common Tape Record-Playback Equipment Equalization Standards.
Transition Frequencies and Time Constants
Standard Type Tape 1 ips 3 ¾ ips 7½ ips 15 ips 30 ips
IEC Fe 2 O 3 100/1326 Hz 50/1768 Hz 0/2274 Hz 0/4547 Hz
1590/120 μs 3180/90 μs /70 μs /35 μs
Metal 100/2274 Hz
1590/70 μs
NAB 50/1768 Hz 50/1768 Hz 50/3180 Hz 50/3180 Hz
3180/90 μs 3180/90 μs 3180/50 μs 3180/50 μs
AES 0/9095 Hz /17.5 μs
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