The IEC & DIN groove specifications for 30cm LP are often quoted as under. These figures are arbitrary mixture from different standards/times and inconsistent or dubious as I remark in parentheses (italics).
|IEC Inmost Recorded Groove Radius 60.325mm=2 3/8inches（The metric number was expressed as diameter 120mm in IEC98-1958. Moreover its application for commercial record is questionable since it is defined originally for transcription records only.）|
|IEC Outmost Recorded Groove Radius 146.05mm=5 3/4 inches according to IEC98 1st edition 1958, but IEC adopted metric figure 146.3mm since 1964: In BS1928-1965 previous diameter 11.5inches is amended to read 11.52inches according to IEC95-1964 See Comparative Table of Standards for 30cm LP.|
|DIN Inmost Recorded Groove Radius 57.50mm (mentioned in DIN 45547: June 1981)|
|DIN Outmost Recorded Groove Radius 146.05mm (146.3mm as per DIN 45537-1962 & DIN 45547-1981. In DIN I could not find the source for 146.05 which seems simple metric conversion from 5 3/4 inches as quoted in IEC98-1958. I feel that generally before 1960 IEC followed BS/US record industry standards and since 1960 IEC followed DIN industry standards esp. their measuring methods.)|
Recently I read IEC60098(1987-still valid) as under:
Art.8.4 Lead-in groove. The pitch of lead-in groove shall be 1.2 plus-minus 0.4mm.
Art.8.5 Outer diameter of recorded surface. diameter 292.6 for 3033&3045(30cmLP33/45rpm) 241.8 for 2533 and 168.3 for 1733/1745 respectively.
Art.8.8 Lead-out groove. The pitch of lead-out groove shall be 6.4 plus-minus 3.2mm. The lead-out groove shall have at least one turn.
Art.8.9 Finishing groove. The diameter shall be 106.4 plus-minus 0.8mm for 3033/2533/3045 and 97.4 plus-minus 1.0mm for 1733/1745
Art.11.2 Tripping mechanism. When the pickup is in the playing position, the tripping mechanism of a record player shall not become operative at a diameter of more than 127mm. This is also corresponding to Art.8.7 Marker space between bands: marker spaces shall not be located inner than diameter 127mm.
Original documents are available from IEC in Switzerland
History of IEC 98:
First Edition-1958: Recommendations for lateral-cut commercial and transcription disk recordings. This original edition was using inch as unit! because "These Recommendations are based on proposals prepared by the British National Committee of the I.E.C., acting as Experts' Group No.2 of Technical Committee No.29, Electro-acoustics". It was noticeable that Union of Soviet Socialist Republics and Brazil as well as USA, European countries and UK jointly voted explicitly in favour of publication. These proposals were first discussed in September 1954. Hence only lateral-cut/monaural record was a subject for discussion at that time. The document contained two separate sections: commercial records (E) and professional (transcription) records (F).
Second Edition-1964: Processed Disk Records and Reproduction Equipment. Stereophonic fine groove records and channel orientation were introduced while transcription disk recordings were omitted from this edition. In 1972 IEC98A was issued as supplement.
Third and Final Edition-1987 (current coding 60098): Analogue audio disk records and reproducing equipment
JIS S8601-1981(abolished in 1994) stated:
JIS Inner Recorded Groove Radius: more than 57.6 (diameter 115.2mm)
JIS Outer Recorded Groove Radius: less than 146.5 (diameter 293mm)
JIS Finishing Groove Radius: 53.2mm (same as IEC&DIN).
NAB's inmost groove: 2.25inches=57.15mm? as per Audio Magazine 1980/Jan. I think NAB's 57.15mm was applicable for the records produced in USA for the decade of monaural LP records, i.e. from 1948 to early 50s until RIAA setting to normalize equalization curve. I heard that recommendation by RIAA was made in June 1953 to produce records based on RIAA equalization from 1954 onward. NAB indicated the diameter of innermost modulated groove shall not be less than 4 3/4inch for LP and not less than 4 1/4inch for EP (these are same as RIAA as per Bulletin No. E 4 around 1964). The writer of Audio Magazine misquoted NAB standards or quoted older NAB standard without specifying published year and the range of application (transcription or commercial record etc). Standards are apt to be changed by time and circumstance and also by group or party involved. Moreover the end (or replacement date) of a standard is usually neglected by us while one can remember the start of a standard. Very often one can assume specific practice or convention as a standard, but such is actually never confirmed nor accepted outside of a specific party or group.
Anyway I think the above figures are maximum or extreme (recordable) and not average values of the produced records.
First I search DIN office in net and find corresponding DIN standards there. Next I search amazon.co.jp and find the brochure DIN-Handbook 523 with title: PHONOTECHNIK (ISBN 3-410-12616-3) containing DIN standards (1966-87) and German translation from IEC98-1987 (analogue record) and IEC908-1987 (CD format). Now IEC98-1987(current coding 60098) is standard worldwide (BS7063-1989 is also equivalent English part) and to be revised around 2007 if vinyl format continues to be produced in sufficient scale – maybe impossible to my regret.
|General Dimensions of Disks||Standard Play (SP) 30cm||Extended Play (EP) 17.5cm||MP 25cm||LP 30cm(12inch)||Transcription 16inch Disks as specified in IEC98-1958|
|Type of groove||COARSE GROOVE||FINE (MICRO) GROOVE||MIXED GROOVES: FINE or COARSE|
|Innermost radius (mm) of music groove||47.6 RIAA(circa1963)||53 JIS(1973)||57.6 JIS||57.5 DIN(1981)/57.6 JIS(1973)/60.325 RIAA(1963)||60 for fine groove 33.3rpm*see remark, 47.5 for coarse groove 78rpm, 95 for coarse groove 33.3rpm|
|Outermost radius (mm) of music groove||146.3 IEC98(1964)/RIAA(1963)||84 JIS(1973)||121 JIS||146.3 IEC/146.5 JIS(1973)||196.85|
|Remark*: In the first edition of IEC98 (Section F5 Page 21) the "minimum diameter of recorded surface" 120mm (4 3/4inches) is quoted for transcription recordings (for broadcasting use) only. There is no corresponding description about minimum diameter for commercial disk records (Section E). However RIAA indicated 4 3/4inches(120.65mm) as minimum diameter of music groove for LP. Sometimes in actual records we find irregular disks which are not complying with any standard. These minimum diameters are determined historically for every format. I think the main factors are minimum groove speed and the applied tip radius of reproducing stylus. Minimum groove speed [=rpm*minimum recorded groove diameter*PI()/60] in my rough estimation: 20cm/s or 21cm/s for LP, 25cm/s for EP, 39cm/s for SP, 33cm/s for transcription coarse groove 33.3rpm. EP can sound better than LP when the same stylus is used.|
I note down interesting points (to me at least) from DIN-Handbook 523 as follows:
IEC60098: Analoge Schallplatten und -Abspielgeräte; Identisch mit IEC 60098:1987(Analogue audio disk records and reproducing equipment: same as IEC 60098:1987)
I was in doubt about my rapid reading of IEC60098 (original in French/English) and perused this German translation in 1989. I make following notes about the inner/outer groove radius.
|From Art. 8.5: The outer recorded groove radius shall be less than 146.3mm.|
|From Art. 8.8/8.9: The inmost recorded groove radius for 30cm LP can be interpreted in various ways. No specific value, but I assume more than 59.6mm as intermediate value between 56-63.2mm where finishing groove radius (53.2mm±0.4mm) + one turn of lead-out groove pitch (6.4mm±3.2mm) = inmost recorded groove radius. Then minimum 57.5mm in DIN is covered by extreme minimum 56mm in this IEC because DIN/IEC adopted same specifications about finishing groove radius and lead out pitch.|
I find an interesting article about distance from the centre of mounting holes of cartridge to stylus tip. Fig.2 in connection to Art. 11.5 shows 9.5mm±1mm at recommended tracking force. This Art. 11.5 recommends: mounting screw M2.5 (or M2.6 where M2.5 is not available) and cartridge weight (mass) not exceeding 12g. I think the odd number 9.5mm as distance is derived from 3/8inches as often Shure cartridges have such value. In JIS C5503(1979) about Phonograph pick-ups, the value is indicated as 10mm±3mm (wide enough for almost all cartridges to fall in this range). There is no special reason to adopt inch instead of mm since IEC would adopt international metric unit generally. It is only a matter of conventional practice and depends on the products available or most popular at the time.
Direction of groove modulation: suitable vertical tracking angle (VTA) is 20degree +5/-0.
The resulting modulation shall be optimum for reproducing styli having a rake angle (SRA)
of between 0 and -5degrees.
I think effective vertical modulation angle (VMA) recorded in vinyl should match vertical tracking angle (VTA) for cartridge. Recommended VTA (and VMA) in 60's was about 15degrees and then in 70's it became 20degree +/-5 and from early 80's it became 20degree +5/-0. VMA is not equal to cutter head angle on lacquer. The cutter head should be more inclined than effective modulation angle due to the elasticity of lacquer. IEC98-1964 & BS1928-1965 have a following NOTE: "In practice, angles of between 0degree and 25degrees may be encountered" . VTA of cartridges in early '60 was ranging between 8degrees (Neumann DST1212) and 36degrees(Shure M77) -see VTA of old cartridges.
comparison with RIAA(3180/318/75μs, 50/500/2120Hz), this IEC (Art.10.2.1)
suggests an additional time constant 7950μs/20Hz in order to suppress subsonic
noise. It results in 3dB difference at 20Hz between recording and
reproduction as under. Art.10.2.2 Tolerance for reproduction chain: a) 2-20Hz
reproducing curve should be on or under the dotted line b)20Hz-20kHz no
tolerance is stipulated. In practice some preamplifiers are equipped with
subsonic filter 15Hz-12dB/Oct etc., for the same effect since IEC time constant
(and its curve 6dB/Oct) is an example. IMO: Historically speaking the bass
limit for phono amplifier is changing by time. Before 1950 low limit was often
not stipulated since there was natural bass limit in
microphone/amplifier/speaker. Later in Hi-Fi era after developing LP, the
handling frequency for microphone/amplifier/speaker has been much extended and
there arises a need for suppressing rumble noise (and low frequency resonance
between arm mass and cartridge compliance which has became lower than 20Hz).
"Nominal" low limit: year 1948 Columbia LP 100Hz>1954 RIAA
50Hz>1987 IEC additional 20Hz.
IEC 60098(IEC98-1987) is modifying or replacing DIN 45538(definitions of terms), 45539(guidelines for measuring method, specifications, connection, exchangeable pickup system, requirement on reproducing amplifier etc), 45546(StereoRecord 45rpm), 45547(StereoRecord 33rpm) and 45548(criteria for record reproducing equipment). The following are extracts mainly from DIN standards.
DIN 45500 T3 (1975):Heimstudio-Technik (Hi-Fi); Minderstanforderungen an Schallplatten-Abspielgeräte (Hi-Fi technics; requirements for disk record reproducing requirements)
standard is almost similar to IEC 60581-3(1978) defining minimum performance requirements. Both
standards mentioning: allowable deviation from rated speed +1.5%-1%/wow and flutter ±0.2%
maximum/Rumble ratio more than 35dB unweighted and 55dB weighted (in addition to
rumble IEC specified reference signal-to-hum ratio more than 50dB at reference
velocity 3.83cm/s rms and reference frequency 315Hz)/static VTF maximum 0.03N/channel unbalance less than 2dB at 1kHz/channel separation over 15dB between 500Hz (315Hz in IEC)
6300Hz: over 20dB at 1kHz/VTA 20±5degrees. This standard comments on compliance (static measured) for every
direction to be minimum 0.8cm/N (8x10^[-6]cm/dyne) corresponding to the
maximum braking force (resilience=Rückstellkraft) 7.5mN（0.75p) measured
at displacement 60μm. The compliance for lateral direction shall be bigger than that for
vertical direction. Further mentioning: rated output voltage of velocity
sensitive pick-ups (for example magnetic cartridges) to be 5 to 15mV at 1kHz with load 47kΩ
for peak velocity 10cm/s (channel sensitivity 0.7 to 2mV/cm/s as per
In case of displacement=amplitude sensitive pick-ups such as piezoelectric
cartridges: 0.5 to 1.5V with load 470kΩ for peak velocity 10cm/s. FIM (frequency intermodulation)
distortion at tracing -6dB reference tone shall be lower than 1%. Standard spherical stylus tip radius 15+3-0μm and
standard bi-radial tip radius 6μm and 18μm.
This IEC specified separation of R from L and L from R respectively and made note: Separation and crosstalk are equivalent only if there is no unbalance output between R/L. In IEC98-1987: Separation precedes crosstalk because separation is independent of channel sensitivity. Hence playing back test record with R or L signal alternatively, the separation of channel L from channel R: 20log(L output voltage from L channel signal divided by L leakage voltage from R channel signal), the separation of channel R channel from channel L: 20log(R output voltage from R channel signal divided by R leakage voltage from L channel signal). And indicate smaller value of measured channel separations at 1kHz.
IMO: Allowable deviation from rated speed +1.5%-1% is too large. Provided the speed deviation +/-0.2% is allowed, drift of strobe-patterns shall be as following table. To get exact 45rpm at 50Hz, pattern should be drifting -15/minute. see also my EXCEL file for rpm & strobe pattern designs.
My note about the sensitivity of cartridge: The velocity of groove modulation is usually expressed as peak cm/s while output voltage is conventionally shown as mVrms in accordance with the indication of millivoltmeter. Relative output in this DIN (5 to 15mVrms for peak velocity 10cm/s) is equivalent to sensitivity in IEC expression (channel sensitivity 0.7 to 2mV/cm/s where output mV and velocity cm/s are both either effective [rms] or peak values). DIN45500 &45539 about cartridge output were often misused and outputs were expressed incorrectly as "mV/cm/s or mVs/cm" while original DIN indicated relative output in mVrms for peak recorded velocity. IEC 60581-3 was based on DIN, but maybe IEC people became aware of such misuse in practice so that they made remark: "output mV and velocity cm/s are both either effective [rms] or peak values" when expressing output in mV/cm/s. I will never know this fact unless I notice the difference of specific output numbers as described in DIN and IEC. See also the English part of "frequency record" (output test of 4 monaural cartridges). In German text, peak velocity is marked with symbol v^ while effective velocity is marked with veff. Accordingly all the velocities (cm/s) quoted hereunder shall mean peak values if not specified.
50Hz Power Supply (Mains)
60Hz Power Supply (Mains)
|RPM||number of stripes or dots on strobe disc||drift number per minute||RPM||number of stripes or dots on strobe disc||drift number per minute|
|77.92||77||-6 to +18||78.26||92||-38 to -10|
|45.11||133||-27 to -3||45.00||160||+/-14|
|33 1/3||180||+/-12||33 1/3||216||+/-14|
According to JIS C5521-1975 (phonomotor test method): 100/3 revolutions at groove radius 12cm and 45 revolutions at groove radius 8cm are measured with the usual stylus pressure on each plain groove. Because of stylus pressure (& drag force) influencing on turntable, rpm would be increasing a bit toward inner groove in most turntables other than Direct Drive turntables. Diameter of the conventional Strobe Disc (around 10cm) was made similar to the label size for checking rpm with record putting on turntable. We forget this reason and feel happy to have bigger strobe disc and measure rpm without loading of stylus pressure upon record.
DIN 45538 (1969):Begriffe für Schallplatten-Abspielgeräte (Definitions for disk record reproducing equipment)
This standard defined terms such as relative deviation from nominal RPM/Wow and flutter/Margin for rumble/pick-up system/cartridge/stylus/tracking force/resilience (Rückstellkraft)/compliance/channel separation/VTA/reproduced frequency/effective stylus mass etc. 'Rückstellkraft' is defined as a force which must be overcome by stress force so that stylus tip can be moved from set position. Tracking force/Resilience/Compliance can be measured at null frequency (static) or at specific frequency (dynamic). IMO: The term 'Rückstellkraft' is identical to stiffness as 1/compliance for example 2p/100micron=980*2dyne/0.01cm=196000dyne/cm stiffness which can be converted into static compliance about 5.1*10^(-6)cm/dyne.
DIN 45541 (1971):Frequenz-Mess-Schallplatten (Frequency test record St 33 and M33, Stereo and Mono)
St 33(Stereo:side A) contains Sweep from 31.5Hz to 20,000Hz(L/R), 16 spots Signals for same range. M33(Mono:side B) contains sweep from 31.5Hz to 20,000Hz, 16 spots signals for same range and sweep from 5 to 125Hz (flutter range). 8cm/s for stereophonic recording, 10cm/s for monophonic recording were selected each as reference recorded velocity 0dB in 70's. See also DIN 45543 which amended velocity 0dB for monaural recording: from conventional 10cm/s to correct 11.3cm/s as calculated.
DIN 45542 (1969):Verzerrungs-Messschallplatte (Distortion test record St 33 and St 45, Stereo)
St33: recorded vertically=hill and dale modulation Tiefenschrift, this side for
the measurement of
VTA is recorded at various vertical modulation angles from 6 to 30 degrees with
complex (Doppel) tones of 1850Hz+3150Hz & 370Hz+630Hz for measuring vertical
tracking angle of a cartridge.
Velocity of each frequency component is fixed at 3.8 cm/s. When the output of
total tone 5000Hz or 1000Hz is measured lowest, the ring shall indicate
tracking angle of a cartridge. Vertical tracking angle measured with total
tone 1000Hz shall be declared in data sheet.
Side:B St45/33: recorded on flank(45 degrees)=Flankenschrift (vertical modulation angle fixed at 15degree) 300Hz+3000Hz for 33rpm or nearly 400Hz+4000Hz for 45rpm for the test of nonlinear distortions with stereo pick-ups. 0dB: f1=300Hz with velocity 8cm/s, f2=3000Hz with velocity 2cm/s, i.e. velocity rate is 4:1 for 300Hz/3000Hz (11cm/s:2.8cm/s for nearly 400Hz/4000Hz). Playing with 33.3rpm, frequency intermodulation distortion (FIM) can be measured by determining the degree of frequency modulation of f2 by f1 (FIM can be read as flutter component around 300Hz) - Ortofon often declares these data for their cartridges as FIM distortion at recommended tracking force, DIN 45542: < 1% etc. Wow-flutter/Drift meter in accordance with DIN 45507 can be applied with this frequency pair (300Hz+3000Hz). Instead of weighting filter, switch on RC HPF with time constant 1ms (=around 160Hz) enabling to suppress frequency modulation (FM) caused by wow-flutter of turntable. Playing with 45rpm, intermodulation distortions (IMD) in accordance with DIN 45403 can be measured. Search-tone-analyser (FFT?) is recommended since demodulation method (amplitude demodulation) may indicate false value of distortion arising at tracing (Phase modulation). Geometric distortion due to stylus tip shape is compensated upon recording except for two rings - cartridge with stylus tip radius 15μm and vertical tracking angle 15degree shall be used as standard for this test record (see my remark 1). The rate of nonlinear distortions arising at -6dB reference tone shall be declared in data sheet. See also DIN 45549 about FIM. My Personal Remarks: 1)By 1969 TELDEC [US Patent 3457374] etc already developed tracing simulator for compensating expected geometric distortion due to the spherical stylus tip tracking on groove. But then the respective designed curvature of spherical stylus tip should be used. 2)FIM & IMD. I am wondering how two different measuring methods in accordance with speeds are possible while the nature of recorded signals is essentially same? There have been various terms and different approaches to modulation distortion measurement: CCIF IMD/SMPTE IMD/DIM (dynamic intermodulation distortion) /Thiele IMD (total difference frequency distortion) and so on!!!
|Side A: Vertical Tracking Angle Test with complex (Doppel) tone in vertical modulation|
|Band||Vertical Modulation Angles||f1 (Hz)||f2 (Hz)||velocity for f1 (v1)=velocity for f2 (v2) (cm/s)||recorded time (second)||Sum tone f1+f2 (Hz)|
|A1||6/10/14/18/22/26/30 degrees (total 7 rings)||1850||2150||3.8||each 10||5000|
|A2||6/10/14/18/22/26/30 degrees (total 7 rings)||370||670||3.8||each 10||1000|
|Side B: Non-linear Distortions Test at 45degrees components|
|Band||Ring number within band||Channel||Relative level (dB)||recorded time St33 (second)||Remarks|
|B3||L||-6||35||Representative Level for FIM measurement|
|B4||R||-6||35||Representative Level for FIM measurement|
|B5||1/2/3/4/5/6/7||L||-12/-10/-8/-6/-4/-2/-6||each 12||Geometric tracing distortion is not compensated upon recording for ring No.7.|
|St45: rotation at 45rpm for side B||f1=400Hz||velocity 11 cm/s||0dB|
|f2=4000Hz||velocity 2.8 cm/s|
|St33: rotation at 100/3rpm for side B||f1=300Hz||velocity 8 cm/s||0dB|
|f2=3000Hz||velocity 2 cm/s|
DIN 45543 (1984):Meßschallplatte zur Messung des Frequenzganges und der Kanaltrennung (Frequency response and separation test record)
This record combines frequency test (sweep 20 to 20,000Hz Lateral), channel separation test (spot 20 to 20,000Hz Alternating L/R), and arm resonance test (3 to 500Hz Lateral and Vertical): thus replacing older test record DIN45541(Stereo and Mono) technically. This test record made in accordance with DIN45547-1981(Stereophonic disk record 33 1/3rpm) should have bottom groove radius smaller than 4micron and VMA 23degrees for stereophonic recordings. A test record based on this standard was produced by DGG.
|Band||Kind of Recording||Effective value cm/s||Peak value cm/s||REMARKS|
|Side A: signals are recorded with DIN/IEC/RIAA characteristic/time constants 3180-318-75microseconds.|
|A1||Lateral||8||11.3||Reference Tone Level = 0dB 1kHz 15seconds|
|A2||Vertical||8||11.3||Reference Tone Level = 0dB 1kHz 15seconds|
|A3||Left Channel||5.6||8||Reference Tone Level = 0dB 1kHz 15seconds|
|A4||Right Channel||5.6||8||Reference Tone Level = 0dB 1kHz 15seconds|
|A5||Left channel||-10dB level of band A3: sweep from 20Hz to 1kHz and -20dB sweep from 1kHz to 20kHz|
|A6||Right channel||-10dB level of band A4: sweep from 20Hz to 1kHz and -20dB sweep from 1kHz to 20kHz|
|A7||L/R alternative||-20dB 1kHz|
|A8-A18||L/R alternative||-20dB spot 20kHz/18kHz/16kHz/14kHz/12.5kHz/10kHz/8kHz/6.3kHz/4kHz/2kHz/1kHz|
|A19-A27||L/R alternative||-10dB spot 1000Hz/500Hz/250Hz/125Hz/80Hz/63Hz/40Hz/31.5Hz/20Hz|
|A28||L/R alternative||-10dB 1kHz|
|Side B: signals are recorded with time constants 3180-318microseconds (excluding top lift 75microsecond).|
|B1||Left channel||-10dB level of band B5: sweep 20Hz to 20kHz|
|B2||Right channel||-10dB level of band B6: sweep 20Hz to 20kHz|
|B3||Lateral||-10dB level of band B7: sweep 20Hz to 20kHz|
|B4||Vertical||-10dB level of band B8: sweep 20Hz to 20kHz|
|B5||Left channel||5.6||8||Reference Tone Level = 0dB 1kHz 15seconds|
|B6||Right channel||5.6||8||Reference Tone Level = 0dB 1kHz 15seconds|
|B7||Lateral||8||11.3||Reference Tone Level = 0dB 1kHz 15seconds|
|B8||Vertical||8||11.3||Reference Tone Level = 0dB 1kHz 15seconds|
|B9||Lateral||-22dB level of band B7 : sweep 3Hz to 500Hz|
|B10||Vertical||-22dB level of band B8 : sweep 3Hz to 500Hz|
the way 1) how about the relation between 0dB & recorded velocity?
According to Vinyl Lexikon by Frank Wonneburg published in year 2000: <following to RIAA/IEC 8cm/s for stereophonic records, 10cm/s for monophonic records and 12cm/s for MaxiSingle>.
DIN 45537（1962）Monaural Records:peak 10cm/s at 1000Hz with the reservation that its value is to be approved internationally. I don't know whether international approval was gained or not.
DIN 45547（1981）Stereophonic Records: effective 5.6cm/s (=peak 8cm/s) at 1000Hz
Anyway pair of 10 & 8 was optional/stopgap because to get same output level from stereo & monaural grooves with stereo cartridge: stereo one channel recorded velocity towards 45degrees = monaural velocity/√2. Hence 8x√2＝11.3cm/s for monaural recording is indicated in the above table from DIN 45543. Of course these are again optional and another pair (Stereo 3.54cm/s and Mono 5cm/s) can be selected as reference 0dB as often applied on cartridge sensitivity test.
2) how to measure recorded velocity?
According to IEC98: the alternating velocity that a rotating disk would impart to the stylus of a pick-up having low mechanical impedance and negligible dimensions of stylus tip. Such perfect cartridge is not yet existing! Hence the recorded velocity of a sinusoidal groove modulation may be measured with an optical method (the Buchmann-Meyer light-band method measuring the width of reflected light patterns). G. Buchmann und E. Meyer, Eine neue optische Messmethode fuer Grammophonplatten. Electrische Nachr-Techn. 7(1930). Another method is based on the theoretical/geometrical value of velocity: Peak Velocity for sinusoidal modulation = amplitude or displacement of modulation from centre (0 to peaｋ)*2pi*frequency. For instance 3.14cm/s: 5micron amplitude for 1kHz, 50micron for 100Hz and so on.
|VARIOUS TEST RECORDS measuring output voltage or SN ratio or output difference between L/R||DENON XG-7001 & JVC TRS-1007 etc||JIS Monaural Standard Record JIS C-5507 & JIS Stereo Standard Record JIS C-5514*(see bottom explanation) etc||NAB Test Record||DIN Test record||CBS-Lab STR-100|
|1kHz reference level recorded in test record||Stereo (each channel i.e., L/R alternatively) 3.54cm/sec peak for 45 degrees||Lateral 5cm/sec peak||Lateral 7cm/sec peak||Stereo (each channel) 8cm/sec||Lateral 10cm/sec peak or 11.3cm/sec (DIN 45543)||Stereo (each channel i.e., L/R alternatively) 3.54cm/sec rms for 45 degrees|
|level of each one channel (45degrees peak) peak signal velocity conversion for stereophonic pickups||3.54cm/sec||3.54cm/sec||5cm/sec||8cm/sec||7cm/sec or 8cm/s (DIN 45543)||5cm/sec|
|Why lateral groove is used in JIS for measuring output voltage of stereo pickups. I think it is because of measuring output difference between L/R at a time. JIS C 5503-1979(Phonograph Pickups) explained clearly "lateral peak 50mm/sec should be converted to 35.4mm/sec peak 45degrees for stereo pickups". Please note the difference in definition between relative output (mVrms for certain velocity peak or rms) and absolute sensitivity (mV/velocity in IEC definition) as explained earlier.|
DIN 45544 (1971):Rumpel-Meß-Schallplatte (Rumble measurement test record St 33 and M 33, Stereo and Mono). The measuring method is based on DIN 45539.
Stereo L flank/R flank & Vertical/Lateral Recordings 315Hz with
peak velocity 5.42cm/s and long plain groove with normal
recording=dense pitch to test motor rumble.
Side B: Lateral=Monaural Recording 315Hz with peak velocity 0.54cm/s and long plain groove with recording pitch 0.54mm/turn =0.3mm/s to test rumble voltages (weighted and unweighted), acoustic feedback at plinth or the influence of auto-stop depending groove radius.
The rumble voltage ratio=20log10(output at 315Hz peak 5.42cm/sec divided by output at mute groove)
There is a reference to NAB-recommendation in March 1964. It is said that NAB's values (100Hz peak 1.4cm/s laterally recorded monaural) are lower than values measured with this DIN test record: about -4dB for monaural equipment and -7dB for stereo equipment because of velocity difference converted to 1kHz output and the nature of groove modulation (DIN/IEC=Stereo 315Hz while NAB=Monaural 100Hz). Moreover the measured value according to NAB is unweighted only. 315Hz is selected because it is the limit of weighted curve as well as linear section for evaluation. Peak velocity 5.42cm/s is selected because it is comparable with velocity 10cm/s at 1kHz after passing IEC/RIAA equalization (time constants 3180/318/75microseconds). But -5.32ｄB(=5.42/10) as recording difference between 315Hz and 1kHz was not exact! Hence accurate value 5.51cm/s for 315Hz based on recording difference -5.18dB is adopted later in IEC98(1987). Old IEC 60581-3(1978!) also indicated 3.83cm/s rms (5.42cm/s peak) based on old data from original RIAA and DIN etc before computer calculation based on time constants became easy - we find this kind of small deviations (0.1-0.2dB order) in old documents even though time constants 3180/318/75microseconds are unchanged. Interestingly the quality of a standard can be deteriorated by the indolent scripters who repeat old data without checking by themselves. IEC98(1964)&BS-1928(1965) indicated correct values for 20Hz-20kHz while the recording curve presented in DIN 45537-1962(Monaural LP record) had irregularity for 30Hz-200Hz (30Hz -17.5dB in DIN45537-1962 vs correct value -18.6dB in DIN45547-1981 for stereo LP) whereas time constants for these standards remain unchanged .
My note: SN rates are actually differing by the radius of mute band to be tested - hence I think test on various radii of long mute bands is important though this point is often neglected in recent test data. In many cases SN ratio at inner groove is better than SN ratio at outer radius (maybe because the height variance due to warp might be small toward inner radius of record or because the rate of stylus friction on a groove might become small as per groove velocity in contradiction with the usual theory of kinetic friction? [a mystery to me]). Rumble due to mechanical imperfection at turntable together with Hum due to electric induction mainly at pick-up system can be measured as SN as a result. For example: Playback output of certain signal groove measured as 5mV, playback noise of plain groove measured as 10μV, then SN ratio is calculated as 54dB. I think rumble [more properly SN] ratio more than 35dB unweighted and 55dB weighted as demanded in DIN 45500(1975) &IEC 60581-3(1978) is practical enough as minimum performance target: it is in vain to seek extraordinary big numbers since the SN ratio of vinyl records [due to the lacquer material particle size under 50angstrom] is usually under 65dB at 1kHz weighted by hearing curve and under 50dB unweighted. I am astonished to read the technical leaflet attached to Denon test record XG-7001: "This band consists of non-modulated grooves that are provided for the purpose of measuring the signal-to-noise ratio of the sound system...If these grooves were to have been cut using a common cutting head, there would ensue noises such as hum, so a special non-modulated groove cutting head not equipped with any moving components was assembled and used to cut these grooves." I don't know how about the plain grooves in other test records for measuring SN ratio. Anyway an essentially rumble-free silent groove is required for SN measurement.
IMO: I. It is of no use to measure mechanical rumble alone. II. The "rumble" is an obsolete term since any modern turntable don't make audible rumble as in the early times.
Some methods to check mechanical imperfection or strength as the deflection of the revolving plate were presented in JIS C5521-1975 (Testing Method for Record Turntables)" as follows:
Each measurement is tested for turntable excluding record mat (i.e. bare platter). Measure with dial gauge (high sensitive type with measuring pressure requirement less than 30g).
(1) Static height variance: Without rotating a turntable, put 50g weight at the radius 125mm on turntable and then shift the weight to the opposite place (125mm). And check the height variance of turntable at radius 125mm. Weight 50g is selected in consideration of the current VTF less than 10g and safe rate as x 5.
(2) Revolving height variance: With rotating turntable, check the height variance at 10mm inside from the rim of a turntable.
(3) Revolving lateral variance: With rotating turntable, check the lateral variance at the rim of a turntable.
Each Evaluation of (1) & (2) : The deflection of turntable =height variance at testing point (mm) /testing point (mm) on a turntable.
Though these JIS methods can check mechanical imperfection or strength, the method (1) is not suitable for turntable with floating suspension. According to a Japanese test report around 1980 about first-class 11 turntables from the world (various drives: DD/BD/Idler and various suspension and construction), static height variance according to test (1) was maximum 0.04mm, revolving height variance according to test (2) was maximum 0.23mm and lateral variance according to test (3) was maximum 0.21.mm. These figures are negligible if compared with mat flatness and record warps.
Besides above JIS, in 1978 Thorens supplied a Rumpelmesskoppler (rumble test coupler maybe inspired by Rabinow's USP3653255-1972) to measure mechanical rumble noise arising from spindle (literal "rumble") - as a result generally 6dB to 10dB higher SN comparing to conventional method using test record could be indicated by this method (free from the quality of a test record). Hence I believe that any modern turntable is free from a mechanical rumble and its SN is mainly influenced by the electrical circumstances. SN is changing in accordance with actual arrangements and nominal SN indicates only potential under ideal (not hearing, only measuring) conditions - it is unreal for users who play records under non-ideal conditions (various acoustic feedback upon hearing).
|Band||Kind of Recording||Effective value cm/s||Peak value cm/s||REMARKS|
|Special remark*: current test records for the time being have 10seconds recording of each signal for side A and 3 seconds recording for side B. It should not be produced anew when new test record is arranged to be made.|
|Side A: Rumble Test Record as per DIN 45544|
|A1||Left Channel||3.83||5.42||315Hz for 15seconds*|
|A2||Right Channel||3.83||5.42||315Hz for 15seconds*|
|A3||Vertical||3.83||5.42||315Hz for 15seconds*|
|A4||Lateral||3.83||5.42||315Hz for 15seconds*|
|A5||Mute band||-||-||Long plain groove with normal recording=dense pitch for music up to radius 60mm at least.|
|Side B: Rumble Test Record as per DIN 45544|
|B1||Lateral||0.38||0.54||315Hz for 15seconds*|
|B2||Mute band||-||-||Long plain groove with recording pitch 0.54mm/turn (=0.3mm/s for synchronising paper recorder) up to radius 60mm at least.|
|Record for Rumble Test according to IEC98(1987)|
|Modulation||Frequency Hz||Effective value cm/s||Peak value cm/s||Time in second|
|Remarks: 315Hz is selected because it is located in the peak of weighted curve as well as in linear section of unweighted evaluation curve. Under the proposition that 1kHz reference signal velocity is 7.07cm/s eff. (10cm/s peak), the recorded velocity 3.90cm/s eff. (5.51cm/s peak) at 315Hz is equivalent with velocity 10cm/s at 1kHz in recording characteristic (time constants 3180/318/75microseconds). In the same way different frequency other than 315Hz can be selected for rumble test. For example: In JIS C5521-1975 (Testing Method for Record Turntables)" signal lateral 5cm/s peak at 1kHz is selected for both SN measurement and reference tone for checking the cartridge output though it is equivalent to diagonal velocity 3.54cm/s peak (2.5cm/s eff.). When measuring unweighted SN ratio about same turntable using IEC, DIN, JIS and NAB methods, indicated SN value is IEC>DIN>NAB>JIS because of the velocity difference of the recorded signals.|
45539(measuring method)&DIN 45544 (rumble test record) both March 1971 were
later accepted as international standards. Filter for unweighted curve was
modified a bit in IEC98-1987 since low frequency resonance between arm mass and
cartridge compliance might affect the unweighted measurement. Left from DIN
with my additional remark 6dB/Oct filter versus Right from DIN IEC 98 issued in 1989 as German
translation of IEC98-1987. It seems that the subsonic filter of rumble
measurement as per IEC98-1987 was made as a compromise between DIN 45539-1971
and JIS C5521-1975 (band-pass filter 300Hz-6ｄB/Oct & sharp subsonic
filter 30Hz-18dB/Oct or -40dB/Oct applying to the output for a plain groove at
radius 120mm for LP and at radius 80mm for EP). I make NAB bandpass
visualised with handwriting. I find a cool passage in this NAB(1964): "This
measurement is intended to give a measure of electrical effect of the
low-frequency noise output of a turntable pickup combination. Since the result
depends on the equalizer, pick-up and arm characteristics as much as on the
turntable itself, it is not feasible to standardize a turntable alone. The
measurement reflects the electrical effect, not the aural annoyance value, of
the low-frequency noise. It has been found that strong low-frequency noise at a
frequency and intensity below audibility may create severe intermodulation
distortion in an audio system, and that in modern systems with extended low
frequency response, this may be more serious than the audibility of the low
frequency. The reference level of 1.4cm/s peak velocity
approximates the expected program level at 100 cps and corresponds in amplitude
to 7cm/s peak velocity at 500 cps." I
prefer the term "SN for a whole
system" to "mechanical rumble". Usually weighted S/N only is
indicated since its number is around 20dB higher than unweighted S/N. I cannot
understand the meaning of weighted S/N since motor rumble & its acoustic
coupling to plinth/arm/mat is lower than
315Hz: mostly 10Hz-250Hz after passing hearing compensation filter
(-12dB/octave for 315Hz & up)-then what is the use of low cut filter
from 315Hz? Hence spectrum analysis method has been recommended by some testers
(Yamamoto in 1971 & Ladegaard in 1977 etc). There are two routes of acoustic
coupling or feedback within a turntable system: I. motor-driving
mechanism-platter-mat-record-cartridge-arm and II.
record-cartridge-arm-turntable board/plinth. I & II are in a loop. In my test using stethoscope during playing
record I could hear music clearly on arm-base while the noise at spindle was not
Sometimes electric transformer produces higher vibration than the
spindle of a revolving motor [transformer is suspended or damped
A or x curve to be applied on the output from a mute band: unweighted for 20Hz-315Hz for measuring Rumpel-Fremdspannung=Rumble interference voltage
B or y curve to be applied on the output from a mute band: weighted both high and low from 315Hz for measuring Rumpel-Geraeuschｓpannung=Rumble noise voltage
Hum measurement as per IEC98 (1987): Use the same record as the Rumble test (315Hz velocity 5.51cm/sec) and calculate The hum voltage ratio =20log10 (cartridge output at 315Hz peak 5.51cm/sec divided by hum induction output). When measuring hum voltage, the stylus point should be located in the range of radius 5-15cm from the centre of spindle, and the needle should be setting 2.5mm above revolving platter (maybe removing test record from turntable and locating the stylus point virtually at the same level of playing actual records - there is no mention on record mat). Check the left and right channel and indicate the minimum (= worst value). IMO: The various shielding states of cartridges influence this hum ratio in actual measurements so that hum rate is not specified in recent products. In JIS C5521-1975 (Testing Method for Record Turntables) definitive method for measuring hum induction level using spherical search coil instead of cartridge is presented, but I never know it is applied actually. SN measurement as the result of whole system is already enough though this SN ratio is also influenced by actual circumstances such as mat/cartridge/arm/cable/step-up transformer etc besides turntable.
DIN 45545 (1966):Gleichlauf-Meß-Schallplatten für 33 1/3 und 45 U/min (Wow and flutter test records for 33 1/3 and 45 rpm)
These records are applied for measuring wow and flutter based on DIN 45507(measuring equipment for frequency fluctuation) and DIN 45539(measuring method). Measuring frequency recorded horizontally is 3150Hz. Record itself shall be manufactured within ±0.06% (unweighted ±0.12%) fluctuation of frequency. And wavy height change hindering optimal centering shall not exceed 0.3mm. The test record based on this standard was assigned to DGG.
W&F evaluation curves: left as per DIN & right as per old JIS before 1972 for example. By early 1970s, NAB & JIS C5521-1975 adopted DIN/IEC evaluation curve though there remained(?) difference in expression among peak/rms/mean. Anyway usual W&F analog meter will rectify the signal (with a special slow-quasi-peak full-wave rectifier designed to register any brief speed excursions) so that they have essentially same meaning relatively, only showing different numbers: theoretical rate 1/0.707/0.636 for peak/rms/mean respectively in case of sinusoidal modulating frequency. For example JIS 0.25%rms is equivalent to DIN/IEC 0.35%peak. We cannot compare the measured specifications of equipments without knowing the measuring method and its evaluation curve. Though this measuring method with W&F meter is established and accepted widely, one can doubt its efficiency because it is based on "slow-quasi-peak full-wave rectifier". Also there is the battle among measuring methods. J.Mcknight (Ampex) mentioned in IEEEM (1972) (here the term "flutter" covers wow and flutter): "The old IEEE/ANSI flutter measurement standard did not predict subjective flutter; it also failed to specify several important characteristics of the meter. Comerci proposed a "flutter index" method but it was never adopted. Results of several workers were incorporated in 1962 in a German Standard (DIN) Weighted Peak Flutter measurement. The NAB flutter measurement of 1965 incorporates the frequency weighting of the DIN Standard, and the volume indicator of Comerci. CCIR adopted the DIN method in 1966. Experiments in the U.S.A. comparing the DIN and NAB methods showed the DIN method to be more satisfactory, and this method is incorporated in the new IEEE Standard 193-1971, based on an IEC draft. Circuits to achieve the desired time and frequency responses are given, as well as suppliers of commercial flutter meters and test records to the new standard."
Sample of unweighted & weighted filters (Leader LFM-39A manufactured in 1979 so that filters are same as DIN):
|Specifications of wow-flutter meter for example||Band-pass Filters : Unweighted|
My note on conventional W&F meter. Why fundamental 3kHz or 3.15kHz is selected? It is said that the sensibility peak of human ears is located around 2kHz-3kHz. Moreover if fundamental frequency is nearer to modulating frequency, then more sharp LPF is required otherwise W&F 0.1% (-60B) cannot be measured. The reason why modulating frequency upto 200Hz is enough might be another story (acoustic psychology). The acoustic psychology (tests carried out by NHK-1955 and Eberhard Zwicker etc) tells us that human ears are most sensitive to wow (modulating frequency) 3-6Hz so that weighted curve for hearing compensation is decided. Upon my hearing of FM waves generated experimentally, even through PC speakers I can hear clearly WOW of 3-6Hz upto -50dB=0.3% as something like beating echo sound while I could not discern W&F of any frequency at less than 0.1% - thus I can reconfirm conventional theory: "there is no real problem in sound quality as far as continuous W&F (excluding any peaked thrust from groove irregularity) is lower than 0.1%". I suppose this is the reason why IEC recommends groove eccentricity to be within 0.2mm. Wow caused by 0.2mm eccentric groove 0.14-0.33% can be reduced to less than 0.1% if weighted with hearing compensation=1/3(-10dB at 0.55Hz). The minor frequency difference between 3kHz and 3.15kHz is negligible because the filter band of W&F meter can handle centre frequency +/- 10% as input. Usually the measured figures weighted with hearing compensation (evaluation curve) is indicated as representative value. When the frequency counter is mounted with W&F meter, counter shows centre frequency so that it works as drift meter (indicating average frequency in certain time scale: drift between playing outmost groove and inmost groove) : to know actual rapid frequency variation, frequency counter with smallest "gate time" is required. Some W&F meters can indicate W&F unweighted/W&F weighted/Wow/Flutter separately in combination of indication JIS/DIN/NAB etc. 0Hz-6Hz as wow and 6-200Hz as flutter in many conventional W&F meters (when modulated with threshold frequency 6Hz and 1% amplitude, meter shows 0.7% each for wow and flutter). Meanwhile current IEC calls 0.1Hz-10Hz as wow range and over 10Hz as flutter range. Now IEC standard based on DIN remains valid while JIS etc is abolished as standard. Nobody care about the end of standards: almost all JIS standards about analog records and equipments were stamped as "abolished" with specific dates while some old standards are walking alone as living ghosts without knowing their death. IEC would adopt 20 years rule from last revision then IEC98(1987) too becomes such living ghost.
DIN 45549 (1980):Abtastfähigkeits-Meßschallplatte (Tracking ability-test-record)
In the first place this test record shall be applied for trackability test at
315Hz and 10kHz. It covers supplementary tests for trackability in mid
frequencies for FIM measurements, sensitivity and rectangular modulation. Vertical
modulation angle is 23degree for stereo recorded bands except B9-B16 monaural
bands which are recorded laterally/sidewise=Seitenschrift. Bands A1-A2: 1kHz
effective velocity 5.6cm/sec(=peak 8cm/sec) as reference tone, Bands
A3-A7: pulse 10kHz with a 250Hz repetition, peak velocity 8-20cm/s interchanging between L/R for
pulse test. Bands A8-12: 300Hz/3000Hz (4:1),
300Hz component peak velocity 4-10cm/s interchanging between L/R for frequency intermodulation
test (each 2.5dB up for 400/4000Hz when playing at 45RPM instead of 33.3RPM)-
see DIN 45542. Bands B1-B2: 1kHz effective velocity
5.6cm/sec(=peak 8cm/sec) as reference tone. B3: Rectangular wave 1kHz cut as triangle
with amplitude 11μm. B4-B8: complex (Doppel) tone of 1.8kHz+2.2kHz (1:1)
momentary peak velocity 10-25cm/s interchanging between L/R. Bands B9-16: 315Hz peak signal
amplitude 50μm-120μm. Distortion rate in high frequency is measured
with pulse 10kHz/250Hz while trackability in low frequency is measured with high
amplitude horizontal recording of 315Hz. The distortion for high frequency
after passing special filter shall be
Dh=U(250)/U(10000) x 100 in %. I saw similar equation in leaflet attached
to Shure Test-record TTR-103 (10.8kHz pulsed high frequency test with a 270Hz
repetition). In low-frequency test Shure TTR-103
indicated Amplitude Intermodulation Distortion with 400+4kHz at 45rpm based on SMPTE (Society of Motion Picture
& Television Engineers) method. Quite different measuring methods are imaginable:
record Pink Noise excluding certain bandwidth and compare it with
reproduced output range to measure distortion fallen in the band.
Current IEC 60098 Article 14.9 Trackability is suggesting to use three kinds of test signals:
-A. Trackability at low-frequency with 315Hz/Horizontal Modulation. Its performance is indicated by max. amplitude in mm up to which a cartridge at recommended tracking force can trace without apparent distortion and tracking problem . The smaller rate of amplitude shall be adopted when the performance differs between channels.
-B. Trackability at low-mid frequency with sweep from 1kHz to 20Hz/Horizontal Modulation. The output of these frequencies are equalised with IEC/RIAA reproduction characteristics so that the output voltage is stable within these frequencies. Hence velocity shall be indicated along with respective frequency measured. Its performance is indicated by max. velocity in cm/s up to which a cartridge at recommended tracking force can trace without apparent distortion and tracking problem. The smaller rate of velocity shall be adopted when the performance differs between channels.
-C. Trackability at high-frequency with pulse 10kHz (with repetition at 250Hz) LRLRLRLRLR. The output is amplified linearly and then filtered into components. Its performance is indicated by max. velocity in cm/s up to which a cartridge at recommended tracking force can trace without excessive distortion and tracking problem. The smaller rate of velocity shall be adopted when the performance under the specified distortion rate differs between channels. Also distortion rate in high frequency shall be indicated. Why impulse instead of continuous 10kHz recording? I suspect that continuous 10kHz recording at very high velocity can burn out driving coils of cutterhead as specified by Neumann SX-74 with cutter drive logic SAL74 as under. Lateral 28.5cm/s peak can be converted to stereo (45 direction) around 20cm/s peak. Even if juvenile cutting engineers fumbled with Neumann and try to record continuous 10kHz 20cm/s, the cutting system can remain undamaged as far as cooling equipment is added.
|Band||Kind of Recording||Effective value cm/s||Peak value cm/s||REMARKS|
|How to use this test record: linear flat amplifier (without RIAA/IEC reproducing characteristics) should be used.|
|Side A: Tracking Ability Test Record as per DIN 45549: A test record based on this standard was produced by DGG.|
|A1||Left Channel||5.6||8||Reference Tone Level = 0dB 1kHz 15seconds|
|A2||Right Channel||5.6||8||Reference Tone Level = 0dB 1kHz 15seconds|
|A3||L/R||5.6||8||Impulse Test 10kHz
with repetition at 250Hz: (every packet of impulse:
L/R interchanging every 20 seconds
intermodulation) Test 300/3000Hz (4:1), the velocities of 300Hz
component are as indicated in left column.
L/R interchanging every 12 seconds for 33 1/3 rpm
By rotating at 45rpm, test signal approx. 400/4000Hz and L/R interchanging every 9 seconds [EP/LP=rpm ratio 1.35, 1.35x300Hz=405Hz]
|Side B: Tracking Ability Test Record as per DIN 45549: A test record based on this standard was produced by DGG.|
|B1||Left Channel||5.6||8||Reference Tone Level = 0dB 1kHz 15seconds|
|B2||Right Channel||5.6||8||Reference Tone Level = 0dB 1kHz 15seconds|
Rectangular wave 1kHz cut as triangle shape in groove with amplitude 11μm. L&R each 15seconds
Test by 1.8kHz+2.2kHz (1:1)
L/R interchanging every 12 seconds
|B9||Lateral||7.0||9.9||315Hz peak amplitude 50microns (displacement 0 to peak)|
|B10||8.4||11.9||315Hz peak amplitude 60microns (displacement 0 to peak)|
|B11||9.8||13.9||315Hz peak amplitude 70microns (displacement 0 to peak)|
|B12||11.2||15.8||315Hz peak amplitude 80microns (displacement 0 to peak)|
|B13||12.6||17.8||315Hz peak amplitude 90microns (displacement 0 to peak)|
|B14||14.0||19.8||315Hz peak amplitude 100microns (displacement 0 to peak)|
|B15||15.4||21.8||315Hz peak amplitude 110microns (displacement 0 to peak)|
|B16||16.8||23.8||315Hz peak amplitude 120microns (displacement 0 to peak)|
DIN 45550 (1976):Schallplatten-Hüllen; Außen- und Innenhüllen, Maße und Beschriftung (Record sleeves; outer-and inner-sleeves, dimensions and inscription) & DIN 45551 (1976): Schallplatten-Kassetten für 30 cm-Schallplatten; Maße und Beschriftung (presentation-box for 30cm-record; dimensions and inscription)
The German people really likes norms - I never imagined such specifications were existing. Jacket size for LP is width315xheight311 with side opening (inner thickness 2mm). Basic inner sleeve for LP is almost square(w309xh304) with circular cut for label. DIN 45536(Mono 17cm)/45546(Stereo 17cm) &45537(Mono 25/30cm)/45547(Stereo 25/30cm) are quoted as specifications of records though sleeves for 25cm records is not specified (maybe by 1976 the production of MP=medium play records is much reduced).
My Summary Note:
These industry standards (IEC/DIN/NAB/JIS) cover almost all the products specifying minimum requirements for not only soft but mainly reproducing equipment available at the times. Hence their specifications don't tell anything new/essential on music recorded groove radii. One thing I feel curious in IEC60098(1987) is about inner groove radius 63.5mm which is recommended for the performance of automatic player (my Kenwood P-5E Linear Tracking Player will lift arm around 60mm radius before finishing groove located around 54mm radius). In 1987 when CD players became already popular, it might be thought that record players could be also automated as seen mostly in low and middle price range of record players.
It seems funny to me that some long time play-back records have not utilized inner radii to maximum. For example, one EMI/Seraphim record: Schubert String Quartet No. 14(Death and Maiden)=38min26sec on one side (pseudo-stereo made from monaural recording) and Piano Quintet (Trout)=32 minutes on other side (both inmost recorded radii are larger than 70mm). Usually it is said that LPs have 150-300 grooves per inch. Hence when music band width is max 83mm(146.5-63.5) then 490-980 grooves for 15-29minutes. The above EMI/Seraphim case: 38min26sec/75mm=about 433 grooves/inch - too fine pitch! I suppose that this record has not utilized extreme inner groove radius in order to avoid (expected) inner tracing distortion by the sacrifice of out-put level (dynamic range and S/N).
Tracking Error and its distortion: it might be critical (audible) only with
recent elliptical/line contact tip in stereo groove esp. if anti-skating
mechanism is not equipped on overhang-offset arm. With spherical tip in
monaural groove, its distortion is not so critical even without
anti-skating mechanism (or other distortions due to spherical tip are enough to
mask this relatively small distortion?). Considering the inner
groove is rarely less than 70mm for LP and if the inmost music groove radius is 63.5mm and
outmost music groove radius is 146.3mm, an optimum arm design
based on Baerwald method can be as follows: Linear Offset for Baerwald method i.e. peak distortion rating similar at
63.5/88.561/146.3mm is 96.04mm (instead of current Baerwald type linear offset
Null points: 69.2/122.8mm (instead of current Baerwald type null points: 66/120.9mm)
In comparison with current Baerwald type, this new design has wider offset angle and also increased overhang (hence higher anti-skating force required to mate with increased side thrust force).
Anti-skating mechanism is problematic. It is rare that the anti-skating
force will match side thrust force due to eventual friction forces. Some Thorens arms have 4 different scales
for anti-skating: wet/dry x spherical/elliptical tip. The following
graph shows imbalance of pressures on flank L/R for three representative designs
of geometry (Stevenson/Baerwald/Loefgren) when anti-skating device is omitted
(parameters: effective coefficient of stylus drag 0.3 and
effective length of arm 231.2mm).
Note: theoretically the true coefficient of friction = 1/(SQRT(2) ) of the measured or empirical value since vertical stylus pressure is to be divided statically into VTF/(SQRT(2) ) each on groove flank. Then stylus drag force is [VTF/SQRT(2)]*2*coefficient of friction=VTF*SQRT(2)*coefficient of friction. This tricky calculation is based on armchair theories because the VTF cannot be actually divided evenly during stylus drag. Hence usually effective coefficient of stylus drag as empirical results is assumed to be theoretically equivalent to SQRT(2)*coefficient of friction. This coefficient of stylus drag 0.3 (coefficient of friction 0.212) for example is rather too small in comparison to the past investigations (coefficient of stylus drag 0.27-0.5 by Rangabe or 0.25-0.55 by JVC-1979 as shown in the following table). The dynamic load of stylus pressure on the groove is never constant. There are many factors involved: stylus contact profile and record elasticity (depth of stylus dipping into groove wall by VTF - see my stylus.xls) / groove modulation amplitude and frequency (mechanical impedance of stylus movement corresponding to such groove characteristics) in addition to the dusts and sticky matters on contaminated records and stylus tip.
The following rates seem to be indicating stylus
drag coefficient instead of coefficient
of kinetic friction
|Spherical tip (17μ）||Elliptical tip (7ｘ17μ）||Shibata tip (7ｘ65μ）|
|Mute plain groove||0.25||0.3||0.28|
Note that the deflection of cantilever due to the side thrust force (skating force) is too small that one cannot adjust anti-skating force seeing the deflection of cantilever. When we recognise apparently cantilever deflection during playing a record, then it has a defective cantilever or anti-skating force is too high. Hence both Dual Skate-0-meter and Orsonic Lateral Pressure Detector were invented as the deflection magnifying device. Lehmann and Harnisch invented Dual "Skate-0-meter" and commented in their US Patent 3328037-1967: "To permit accurate adjustment, hitherto a record was used which had no grooves but only a smooth surface. The pick-up with its scanning needle was placed on the rotating disc and the antiskating so adjusted that the pickup remained stationary. Investigations have proved that this method is only apparently accurate. The actual friction of the scanning needle in a sound groove is different. Direct measurement of this friction, which as such gives a direct measure for the necessary anti-skating force, is however relatively complex." And they recommended to apply Skate-0-meter on a plain groove with normal recording pitch while Nakatuka in his USP4183537-1980 recommended to apply Orsonic Lateral Pressure Detector on sound grooves for anti-skating adjustment. Also note that usually the bottom profile of stylus is unspecified or unpolished since such part of stylus is designed simply to have enough clearance from the bottom of groove. The higher stylus drag for higher frequency and higher amplitude can be attributed to the mechanical impedance of respective pick-up. In order to move stylus in higher frequency, there arises instantaneous higher stylus pressure to groove walls as reaction from undulating walls. Thus effective low mass or low inertia of moving parts is required for tracing such high frequency recorded groove with relatively light stylus down-force. Mechanically a pickup has three different (stiffness or compliance/resistance/mass or inertia) controlled domains in mechanical impedance curve. Typically: stiffness controlled domain (20Hz-1kHz), resistance-domain (1kHz-10kHz or around) and mass- or inertia-domain (around 10kHz and upward) though its domain and curve of mechanical impedance (dyne sec/cm) is shifting up or down as per the make and design.
BTW: There is no effective measuring method for distortion due to lateral tracking
angle error because this kind of distortion is usually masked by much bigger
distortions (i.e. tracing distortions) when tracing actual record with a stylus
tip of considerable contact radii. Also read the end of this page about the
comparison of various distortions. Generally tracking (angle) error distortion
is in small order (less than 2%) in comparison with tracing error distortion
(often exceeding 10%) due to effective contact radius of stylus tip. Hence in
order to check angle error and alignment it is of no use to see playback wave
forms on oscilloscope since distortion rate ascertainable on oscilloscope
should be more than 10% otherwise not easy to find as a distortion or deformed
wave. Actual impulsive mis-track (stylus skipping from groove walls mainly due
to defective groove or dirty sticky stylus) can be seen on a oscilloscope or heard very
cruelly with our ears.
How stand the relative rates among these distortions? If you are interested in the equations for the following simulations, please download my EXCEL file and check by yourself.
Due to different styli shapes between cutter and reproducer etc
A. Vertical Tracing Distortion (mainly 2nd harmonic at 1kHz, 3rd harmonic increases at 10kHz). The following graph indicates the trajectory of spherical 18micron tip centre on sinusoidal vertical modulation at velocity 6.3cm/s, groove radius 6cm, frequency 5kHz.
B. Horizontal Tracing Distortion (mainly 3rd harmonic distortion) due to different styli shapes between cutter and reproducer
These (A&B) can be improved by making tip radius smaller. IEC98(1987) specified groove
dimensions: top width 30micron min. bottom radius 8micron max. The clearance between the stylus tip
and bottom of the groove shall be 0.002mm min and the stylus tip shall not touch the groove edges.
In order to get such clearance from groove bottom and edges, the appropriate
radius of spherical tip shall be limited to 0.5-0.8mil (13-21micron).
The effective (contact with groove flank) radius of curvature of elliptical tip is 0.2-0.4mil while its radius toward bottom is more than 0.7mil (18micron). But too small spherical tip may dig the dusts in the bottom of groove so that it tends to be noisy.
|The appropriate spherical tip radius depends on the dimensions of groove modulation|
|1||groove bottom radius||<7.5micron||<4micron||<8micron|
|4||included angle of spherical tip||40-50degrees||40-55degrees||<55degrees|
|top width* is applicable for monophonic only. In DIN 45547 Stereophonic disk records St33(1981) top width average =/>35micron, momentary value =/>25micron|
Example of cutting stylus for fine groove: this example is obsolete. Current cutting stylus has the burnishing facet width less than 5micron for lacquer cutting (no burnishing facet for copper cutting）. Bottom radius of cutter should be also less than 5micron.
Spherical Tip on Fine Groove: strictly speaking not spherical because it has included angle less than 55degrees in order to reduce pinch effect to some extent (about 40% less as compared to true spherical ball tip).
Applied maximum spherical tip radius is half of minimum top width of groove
|Minimum top width about 152micron for monophonic coarse groove (SP) / tip radius 76micron (3mil)|
|Minimum top width about 50micron for monophonic fine groove (LP) / tip radius 25micron (1mil)|
|Minimum top width about 35micron for stereophonic fine groove (LP) / tip radius 18micron (0.7mil)|
|Minimum top width about 30micron for stereophonic fine groove (LP) / tip radius 15micron (0.6mil)|
|Minimum top width about 25micron for stereophonic fine groove (LP) / tip radius 13micron (0.5mil)|
Sample of stereophonic groove: please note that top width of stereophonic groove is changing momentarily and that the minimum top width is depending on the displacement (amplitude) and the nominal top width of plain groove. Specific to stereophonic groove of 45degree modulations, the amount of lateral displacement is always same as that of vertical displacement irrespective of amplitude and frequency differences between channels. Hence cartridge to trace such groove should have same compliance laterally as well as vertically - however lateral compliance is usually higher than vertical compliance in most stereophonic cartridges. In practice the stereo grooves are cut with various kinds of limiters. In US Patent 3013125 (Stereophonic Recording) Goldmark referred to such limiter: "Normally, these two signals [sum and difference] are of similar amplitude and it is difficult to design a pickup which will follow them without generating distortion. We have discovered that the difference signal can be limited in amplitude so that it will be as little as one-half that of sum signal, or less, without impairing substantially the stereophonic character of the recorded information." In case of playing compatible discrete 4 channel records, same compliance for both lateral and vertical directions was demanded for pick-up cartridge. In case of playing usual stereophonic grooves cut with such vertical amplitude limiter, the imbalance of cartridge compliance for lateral/vertical directions did not become any serious problem since stereophonic groove in practice was a gimmick or the product of compromises from the outset!
There is a distortion toward inner groove namely "pinch effect" which can be reduced by using elliptical tip. This effect may cause vertical modulation of double cycle. In case of fundamental 5kHz lateral recording, the cycle of vertical modulation due to pinch effect is 10kHz. If cartridge has same compliance for vertical and horizontal movement, then the distortion due to pinch effect shall be approximated as shown in following graphs. Here the distortion ratio % is calculated as Vertical velocity (arising from pinch effect) divided by Lateral velocity of the recorded signal.
Schematic of 1.3kHz Lateral Modulation at groove radius 6cm, displacement peak to peak 30µm：velocity about 12.25cm/s (velocity=2πfa where f=frequency, a=displacement of 0 to peak)
At tracing the above groove with spherical tip radius 18micron, the inclination of modulation corresponds with that of points of contact of spherical tip on flanks. Pinch effect eminent toward inmost groove radius is additional vertical modulation arising from original lateral modulation of high velocity/frequency. In this case, vertical output calculated (1micron x 2f)/(15micron x 1f) is 13.5%(-17dB) of lateral output.
There is an additional distortion （similar to Wow=fluctuating groove speed±%) due to eccentric groove or hole which happens to be displaced more than 1mm sometimes. Right graph shows Fluctuation of Frequency at groove radius 10cm with eccentricity 1mm where pitch (groove speed) fluctuates +/- 1% per rotation=1.8sec in case of 100/3rpm (200degree/sec) from recorded frequency. Thus the rate 0.5555cycle(=once per 1.8sec) indicates modulating frequency (FM). Additional amplitude modulation (AM) if any due to this displacement is rather small (max 0.35cm/s at 1mm displacement of hole) and harmless since this amplitude of 0.5555Hz can be usually suppressed with filter and compliance of cartridge as far as arm pivot has high sensitivity to follow this displacement smoothly. Meanwhile frequency fluctuation (FM) shall remain uncompensated with any filter.
There is still another kind of distortion: Reproducing loss of fundamental at higher frequency depending on tip radius & groove radius & amplitude of recorded level. The frequency response of high frequency is usually measured at outer groove radius and the recorded level (amplitude) for frequency response test is lower than reference tone level (see DIN 45543 test record etc). Lateral modulation at outer groove radius 11.5cm shall mean groove velocity around 40cm/s where this loss is almost negligible. Graphs show loss at lateral modulation: constant velocity 5cm/s peak (flat recording without RIAA recording emphasis). Vertical reproducing loss is almost twice lateral reproducing loss.
Due to different angles between VMA (effective vertical modulation angle) at recording and VTA (vertical tracking angle) at reproduction
C. Vertical Tracking Distortion: The height adjustment of arm cannot affect this distortion on a large scale since the rate of height change at arm post is very limited: max±1.3degree by ±5mm at the effective lateral length of arm 220mm while nominal VTA of current cartridge is ranging from 15 to 25 degrees and there is no way to ascertain actual VMA of each record -some special test records are required to measure VMA. It is truly complicated about distortion arising from the difference between VMA and VTA. Note that 2nd harmonic distortion % as shown in graph is based on one sinusoidal wave only while there must be another distortion from mixed tones as used in measuring VTA of cartridge by DIN 45542 test record (f1=1850 or 370Hz f2=3150 or 630Hz) etc. IMO: quality control of cartridge about VTA&SRA is most important since sound quality cannot be improved afterward by changing VTA of existing cartridges forcibly to comply with VMA: to change VTA drastically is to change SRA at the same time - deviating further from allowable range of SRA between +4 and -8degrees for non-spherical tip.
Due to the error of Lateral Angle/Alignment
D. Lateral Tracking Distortion: The distortion rate at larger error angle is similar to that at VTA difference (see above graph). This 2nd harmonic distortion can be reduced to less than 1% with correct alignment for pivoted arms. When the deviation from exact alignment is within +/-3mm for overhang (shift on shell) or shift of arm on bedplate, then error angle is within +/-4degree and distortion less than 2% with 9inches arms at signal velocity 5cm/sec. Theoretically 0% for linear tracking arms (nominal error max 0.15degree for most linear trackers using LED+photo sensor+motor to control angle error). The following graph shows comparison of Micro MA-505 (Effective Length 237mm near to "Stevenson type" alignment) and "Baerwald and Loefgren type" alignments applied for the arms of same length when aligned each as designed. Note on this graph: in order to make prompt and easy comparison with other graphs of distortion & ratings, signal velocity is set at 5cm/sec instead of usual 10cm/sec.
Theoretical rate of distortions:
For example: tracing 5kHz velocity of 5cm/sec peak with spherical tip radius 18micron=0.7mil. Velocity 5cm in the following analysis should be understood as vertical modulation velocity for A & C and horizontal/lateral modulation velocity for B & D. But all distortions from A to D will be involved in actual stereophonic groove which has lateral and vertical components. In stereophonic pickup the velocity toward 45 degrees should be counted - hence vertical or lateral modulation velocity 5cm/s can be converted to 3.54cm/s [=5/SQRT(2)] per channel for direction towards 45degrees. Inversely modulation velocity toward 45degrees can be divided into x1/SQRT(2) each for lateral and vertical components. Hence upon measuring distortion actually on test record, we must be careful about the kind of groove (vertical/horizontal/45) and its velocity specified in cm/s peak or rms.
At inner groove radius 6cm
A. Vertical tracing distortion/VTD:2nd harmonic distortion rating 32%, 3rd harmonic distortion 16%
B. Horizontal=Lateral tracing distortion/LTD: Mainly 3rd harmonic distortion 8%
C. Vertical tracking distortion/VtD: 2nd HD 2.1% with Cartridge VTA 5degree different from VMA, 4.2% in case of 10degree difference
D. Lateral tracking distortion/LtD: Baerwald type alignment usually under 0.3% for groove radii 60-146mm. If you use Stevenson type alignment null point around 60.325mm, then distortion is ignorable toward inmost groove.
At outer groove radius 14cm
A. VTD: 2nd harmonic distortion rating 6%, 3rd harmonic distortion 0.5%
B. LTD: Mainly 3rd harmonic distortion 0.3%
C. VtD: 2nd HD 0.9% with Cartridge VTA 5degree difference, 1.8% with VTA 10degree difference
D. LtD: Baerwald type alignment 0.3% for groove radii 60-146mm. If you use Stevenson alignment, then distortion reaches around 0.4% at this radius and around radius 8cm.
In short, vertical tracing distortion is bigger than lateral/horizontal tracing distortion because vertical movement is restricted with contact height only while the needle for horizontal direction is restricted by both sides of walls. And this might be the good reason why monophonic sound with lateral modulation is better than stereophonic sound with 45/45 modulation. I find the following text in US Patent 3229048 for RCA Dynagroove： "An analysis of tracing distortion shows that lateral cut records are superior to vertical cut records (hill-and-dale). In lateral cut records, the two groove walls, moving in the opposite directions relative to the reproducing stylus center, form a push-pull system which tends to eliminate the even order harmonic and intermodulation components of tracing distortion. In vertical cut records, vertical-lateral stereophonic records, or in 45-45 type stereophonic records the cancellation of even order harmonic and intermodulation distortion does not take place and the tracing distortion problem becomes significant."
Note on graphs: above input frequencies (f) are fundamental. Hence actual distortion for velocity sensitive cartridge output after phono stage (RIAA equalization) : 2nd harmonic distortion shall be reduced to almost 1/2, 3rd to 1/3 over 5000Hz. These adjustments can be applied for all harmonic distortions though it is complicated further due to pre-emphasis=recording characteristics of RIAA with emphasis about +6dB/Oct at high frequencies. I read that the peak of high frequencies in classical music has generally level around -6dB/Oct. But "new music" or "noises" might have another kind of spectra.
From above: highest distortion for high frequencies arises from VTD at inner groove in particular. Meantime it is said that the vinyl deformation due to its elasticity reduces such extreme distortions and the real rates of distortions are less than calculated: Distortion from the elastic deformation of groove wall is rather small in comparison with tracing distortion and it has reverse phase of tracing distortion so that the distortion in effect becomes smaller than the theoretical value of tracing distortion.
Main problems when simulating the distortions for vinyl reproduction: Above analysis on respective distortions is based on a ball model tracing on sinusoidal groove modulation. And this simulation or calculation is carried out usually on 2 dimensional planes separately. That is: vertical modulation (vertical tracing error from original trajectory of groove modulation)/lateral modulation (lateral tracing error from original trajectory)/pinch effect (additional vertical modulation arising from original lateral modulation)/VTA difference (difference between the vertical movement of cantilever and effective modulated angle of record)/Lateral tracking error because of arc movement of the pivoted arms. Then how is all in all of these distortions? If anyone is skilled in 3D CAD and applied mathematics, please try to make a model of modulated groove/stylus tip/generating system for more realistic simulation. As for me I am not capable of it - I must confess. Every distortion or deviation has different character having vertical or lateral or 45degrees or non-directional component so that the sum of these distortions in the result is in complex stage (impossible to sum up on one single plane actually).
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