p i t ch shifch shift i n gt i n g - berklee college of...

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RECORDING OCTOBER 2000 D is the point of maximum negative amplitude and occurs 3 milliseconds after the beginning of the cycle. And E has our sine wave returning 4 milliseconds after point A to what looks exactly like the starting point: the amplitude is zero, and increasing. Okay so far? We are going to follow these points through some signal process- ing and move them around a bit. Fixed delay Run this sine wave through a fixed delay of, say, 1 mil- lisecond, and you get the situation described in Figure 1ii.Visually, you might say the sine wave slips along the horizontal time axis by 1 millisecond. Looking point by point,Table 1 shows us what hap- pens. Point A originally occurred at a time of zero. Introduce a fixed delay of one millisecond and Point A now occurs at time equals one millisecond. The other points follow. Point D, for example, occurred undelayed at a time of 3 milliseconds. After it has been run through a fixed, unchanging delay of one millisecond, Point D is forced to occur at a time of 4 milliseconds. Accelerating delay Here’s the mind bender. What happens if the delay isn’t fixed? What if the delay sweeps from a starting time of 1 millisecond and then increases, and increases, and increases...? Table 2 summarizes. Here the delay changes at a rate of one millisecond per millisecond. Say what? For every millisecond that ticks by during the course of this experi- ment, the delay gets longer by one millisecond. For P i tch Shift i n g P i tch Shift i n g BY ALEX CASE W e all know what happens when you play an audio tape at a faster speed than it was recorded: the pitch of the recording goes up. Play it slower than the recorded speed and the pitch goes down. Somewhere in this simple principle lies an opportunity for audio explo- ration and entertainment. Can it be done digitally? Of course. How is it done? Using a delay. Yes, I said delay. Loyal readers of Nuts & Bolts have just spent the last three issues reading about delays: echo, chorus, flange, and their many cousins.Yet we aren’t finished discussing delay, because even pitch shifters are built on this effect. To see how, you’ve got to put up with a bit of math (which I seem to sneak into every article) and follow along with Figure 1. Figure 1i shows a simple sine wave with a chosen frequency of 250 Hertz. This sine wave completes a cycle every 4 milliseconds, confirmed cour- tesy of the following familiar equation: Period = the time to complete one cycle Period = 1 / Frequency Period = 1 / 250 Hz Period = 0.004 seconds or 4 milliseconds Figure 1i labels some key landmarks during the course of a single cycle. We start the clock at point A. Here, at time equals zero, the sine wave is at an ampli- tude of exactly zero and is increasing. It reaches its posi- tive peak amplitude at B, taking exactly 1 millisecond to do so. It has an amplitude of zero again at the halfway point (time equals 2 milliseconds) labeled C. This makes it look a lot like point A, but while the amplitude is the same, notably zero, it is decreasing this time.

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Page 1: P i t ch Shifch Shift i n gt i n g - Berklee College of Musicmpe.berklee.edu/documents/articles/nuts_bolts/16_pitch... · 2008-01-25 · Of cours e . H o w is it done? Using a delay.Ye

RECORDING OCTOBER 2000

D is the point of maximum negative amplitude ando c c u rs 3 milliseconds after the beginning of the cy c l e .And E has our sine wave returning 4 milliseconds afterpoint A to what looks ex a c t ly like the starting point: theamplitude is ze ro, and incre a s i n g . O k ay so far? We aregoing to fo l l ow these points through some signal pro c e s s-ing and move them around a bit.

Fixed delayRun this sine wave through a fixed delay of, s ay, 1 mil-

l i s e c o n d , and you get the situation described in Fi g u re1 i i . Vi s u a l ly, you might say the sine wave slips along theh o r i zontal time axis by 1 millisecond.

Looking point by point, Table 1 shows us what hap-p e n s . Point A originally occurred at a time of ze ro.I n t roduce a fixed delay of one millisecond and Point An ow occurs at time equals one millisecond.

The other points fo l l ow. Point D, for ex a m p l e , o c c u r re du n d e l ayed at a time of 3 milliseconds. After it has beenrun through a fixed, u n changing delay of one millisecond,Point D is fo rced to occur at a time of 4 milliseconds.

Accelerating delayH e re ’s the mind bender. What happens if the delay

i s n ’t fixed? What if the delay sweeps from a starting timeof 1 millisecond and then incre a s e s , and incre a s e s , a n di n c re a s e s . . . ?

Table 2 summarize s . H e re the delay changes at a ra t eof one millisecond per millisecond. S ay what? For eve rymillisecond that ticks by during the course of this ex p e r i-m e n t , the delay gets longer by one millisecond. Fo r

P i tch Shift i n gP i tch Shift i n gBY ALEX CASE

We all know what happens when you play an audiotape at a faster speed than it was re c o rded: the

p i t ch of the re c o rding goes up. P l ay it slower than there c o rded speed and the pitch goes dow n . S o m ew h e re inthis simple principle lies an opportunity for audio ex p l o-ration and entertainment.

Can it be done digitally? Of cours e . H ow is it done?Using a delay. Ye s , I said delay. L oyal re a d e rs of Nuts &Bolts h ave just spent the last three issues reading ab o u td e l ays: ech o, ch o r u s , f l a n g e , and their many cousins. Ye twe are n ’t finished discussing delay, because even pitchs h i f t e rs are built on this effect.

To see how, yo u ’ ve got to put up with a bit of math( w h i ch I seem to sneak into eve ry article) and fo l l owalong with Fi g u re 1. Fi g u re 1i shows a simple sine wavewith a chosen fre q u e n cy of 250 Hertz. This sine wavecompletes a cycle eve ry 4 milliseconds, confirmed cour-tesy of the fo l l owing familiar equation:

Period = the time to complete one cy c l ePeriod = 1 / Fre q u e n cyPeriod = 1 / 250 HzPeriod = 0.004 seconds or 4 millisecondsFi g u re 1i labels some key landmarks during the cours e

of a single cy c l e . We start the clock at point A .H e re , at time equals ze ro, the sine wave is at an ampli-

tude of ex a c t ly ze ro and is incre a s i n g . It re a ches its posi-t ive peak amplitude at B, taking ex a c t ly 1 millisecond todo so. It has an amplitude of ze ro again at the halfwaypoint (time equals 2 milliseconds) labeled C. This make sit look a lot like point A , but while the amplitude is thes a m e , n o t ab ly ze ro, it is decreasing this time.

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ex a m p l e , if at one point the delay is 10 milliseconds,then five milliseconds later the delay unit is operating at15 milliseconds.

If you have n ’t had the chance to study phy s i c s , yo umight be puzzled by the idea of changing the delay timeat a rate of 1 millisecond per millisecond. I find it help-ful here to get in my car.

S ay you are driving at a speed of 8 5 (edited for your safe-ty) 55 miles per hour and accelerating at a rate of 1 mphper hour (our Canadian neighbors should use kilometersper hour for similar re s u l t s ) . That means that for each hourthat passes by your speed increases by one mile per hour.D r iving 55 mph now becomes 56 mph an hour from now.Wh o a !

If you subscribe to the idea that cops wo n ’t pull yo uover for speeding until you are at least 10 miles per hourover the speed limit, then—starting at the speed limit—you can drive most of the way across Texas (it’s about 600miles from Dallas to El Paso) without getting a ticke t .

B a ck to the mu s i c . H e re we are increasing the delay by1 millisecond each millisecond. And the surprising re s u l tis a change in the pitch of the tra ck .

Table 2 shows the location of our sine wave landmark sboth befo re and after thei n t roduction of thiss t e a d i ly increasing delay.Point A initially occurs ata time of ze ro. At thistime the delay is alsoze ro. Point A thenremains unchanged ando c c u rs at time ze ro.

Skip to point C. It orig-i n a l ly occurs at a time oft wo milliseconds. By thistime the delay hasi n c reased from ze ro tot wo milliseconds. Th i sd e l ay of two millisecondsleads point C to finallyoccur at a time of fo u rmilliseconds after thebeginning of this ex p e r i-m e n t .

Do the math point bypoint and you get a sinewave that looks likeFi g u re 1iii.The key land-m a rks are identified.The result is clearly still a sine wave .But since it takes longer to complete the cy c l e , we know thep i t ch has ch a n g e d .

B a ck to our trusty equations. Looking at the new sinewave at the bottom of Fi g u re 1, l e t ’s calculate its fre-q u e n cy. The sine wave in Fi g u re 1iii takes a full 8 mil-liseconds to complete its cy c l e .

Period = the time to complete one cy c l ePeriod = 8 milliseconds or 0.008 secondsFre q u e n cy = 1 / Pe r i o dFre q u e n cy = 1 / 0.008Fre q u e n cy = 125 HertzThat’s right.The constantly increasing delay caused

the pitch of the signal to change. We sum it up as fol-lows.A 250 Hertz sine wave run through a delay thatincreases constantly at the rate of 1 millisecond per mil-lisecond will be lowered in pitch to 125 Hertz. Strange,but true.

Skipping the details—though you are encouraged top rove these on your ow n — we find a number of finerpoints on pitch shifting. Our example demonstrated that

an increasing delay lowe rs the pitch . It is also true that ad e c reasing delay raises the pitch .

In add i t i o n , our example found that changing the delayat a rate of 1 millisecond per millisecond moved the pitchby an octave . It is also possible to change the pitch by twoo c t ave s , or a minor third , or a perfect fifth—whatever yo ud e s i re; one need only change the delay at the correct ra t e .

So the underlying methodology of pitch shifters isreve a l e d . A pitch shifter is a device that changes a delayin specific controlled ways so as to allow the user toaffect the pitch of the audio.

N a t u ra l ly, it ain’t easy. We ’ ve got a key pro b l e m . R e t u r nto our example in which we lowe red the 250 Hz sine waveby an octave through a steadily increasing delay. If weimagine applying this effect to an entire three and a halfm i nute tune, not just a single cycle of a sine wave , wefind we are increasing the delay from a starting point ofone millisecond to a final delay time of 210,000 millisec-onds (31/2 m i nutes equals 210,000 milliseconds).

That is, at the start of the tune we add an incre a s i n gd e l ay: 1 ms, then 2 ms, and so on. By the end of the tune,we are adding a delay of 210,000 milliseconds. This high-lights two pro b l e m s .

Fi rs t , we need a ve ry long delay. Most delays are capa-ble of a one second delay (1,000 milliseconds) at them o s t . Super cool mega turbo delays might go up tom aybe 10 seconds of delay. But a delay of hundreds ofthousands of milliseconds (hundreds of seconds) is a lotof signal processing hors e p ower that is ra re ly ava i l ab l e —RAM isn’t that ch e a p.

S e c o n d , our song, w h i ch used to be 31/2 m i nutes long, d o u-bles in length to seven minutes as we lower the pitch by oneo c t ave . Consider the last sound at the ve ry end of the song.

B e fo re pitch shifting it occurred 31/2 m i nutes (210,000milliseconds) after the beginning of the song. By this timeour pitch shifting delay has increased from 1 millisecondto 210,000 milliseconds. Th e re fo re the final sound of thep i t ch shifted song occurs at 210,000 milliseconds (originaltime) plus 210,000 milliseconds (the length of the delay ) .That is, the song now ends 420,000 milliseconds (that’ss even minutes!) after it began. The 31/2 m i nute song isl owe red an octave but doubled in length.

S i m p ly increasing the delay fo rever as ab ove is ex a c t-ly like playing a tape back at half the speed it wa s

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re c o rd e d . The pitch goes down andthe song gets longer.

Wh e re pitch shifting signal pro c e s-s o rs differentiate themselves fro mtape speed tricks is in their cleve r n e s sh e re . Digital delays can be manipulat-ed to always incre a s e , but also to re s e tt h e m s e l ve s .

In our sine wave ex a m p l e , what hap-pens if our digital delay increases at arate of ex a c t ly one millisecond per mil-lisecond but never goes over 50 mil-liseconds in total delay? That is, eve rytime the delay re a ches 50 millisecondsit resets itself to a delay of ze ro andc o n t i nues increasing from this newd e l ay time at the same rate of one mil-lisecond per millisecond.

The result is pitch shifting that neve ruses too mu ch delay and never make sthe song more than 50 milliseconds longer that the un-p i t ch shifted ve rs i o n . After all, our analysis showed itwas the rate of change of the delay that led to pitch shift-i n g , not the absolute delay time itself. A ny delay time

that increases at rate of 1 millisecondper millisecond will lower the audioby one octave .A ny delay time. So whynot keep it a small delay time?

The devil is in the details. G e t t i n gthe pitch shifter to reset itself in thisway without being noticeable to the lis-tener isn’t easy. It is a problem solve dby clever softwa re engineers who findways to make this inaudible.

Older pitch shifters ‘ g l i t ched’ as they tried to return tothe original delay time.These day s — we are lucky to bea l ive in audio in the year 2000—those glitches are mostlyg o n e .To d ay we simply re a ch for a device labeled “ p i t chs h i f t e r,” dial in the desired settings (gimme a shift up of amajor third mixed in with a shift down of a perfect fo u r t h ) ,and get to wo rk . Life is good.

Side effectsB e fo re we get into the special effects we create with

p i t ch shifting dev i c e s , it is worth noticing that pitchshifting is a natural part of some effects we ’ ve alre a dyi nvestigated here in the Nuts & Bolts s e r i e s . Recall thechorus effect that comes from adding a slow ly modulatedd e l ay of about 30 milliseconds.

As you listen to the richness that the chorus effecta dds to a vocal or guitar, listen for a subtle amount ofp i t ch shifting. Th a t ’s right, p i t ch shifting is a componentof that effect we call ch o r u s .

Since a chorus pedal relies on a modulating delay, i ti n t roduces a small amount of pitch shifting. As the delaytime sweeps up, the pitch is slightly lowe re d . As thed e l ay time is then swept dow n , the pitch is then ra i s e d ,ever so slightly. Repeat until thicke n e d .

Special effectsThe Nuts & Bolts rev i ew of the a basic pop mix, ‘ M i x i n g

by Numbers’ in the 4/00 issue, i n t roduced a commoneffect built in part on pitch shifting: the spre a d e r.

A quick rev i ew of this effect: the spreader is a “ p a t ch ”that enables you to take a mono signal and make it a littlem o re stere o - l i ke .You ‘ s p read’ a single tra ck out by sendingit through two delays and two pitch shifters .

The delays are kept short, e a ch set to different va l u e ss o m ew h e re between about 15 to 50 milliseconds. To oshort and the effect becomes a flange/comb filter (as wediscussed last month). Too long and the delays stick out asdistinct ech o e s . So our window for acceptable delay timesin this effect is between about 15 and 50 milliseconds.

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In using a spreader, the return ofone delay output is panned leftwhile the other is panned right. Theidea is that these quick delays add adose of support to the originalmonophonic track. In effect, thesetwo short delays simulate some earlysound reflections that we wouldhear if we played the sound in a realroom. The spreader takes a singlemono sound and sends it to twoslightly different short delays to sim-ulate reflections coming from theleft and right.

Th a t ’s only half the story. Th eeffect is taken to the next leve lcourtesy of some pitch shifting.Shift each of the delayed signalsever so slightly, and the fo r m e rlyboring mono signal becomes a mu chm o re immers ive , i n t e resting loud-s p e a ker cre a t i o n .

Detune each delay by a nearlyi m p e rceptible amount, m aybe 5 to 15c e n t s . The goal of the spreader is toc reate a stereo sort of effect. As are s u l t , we try to keep the signal pro-cessing on the left and right sidesever so slightly different from eacho t h e r. Just as we dialed in uniqued e l ay times for each side of thise f f e c t , we dial in different pitch shiftamounts as we l l — m aybe the left sidegoes up 8 cents while the right sidegoes down 8 cents.

L i ke so mu ch of what we do inre c o rding and mixing pop mu s i c , t h eeffect has no basis in re a l i t y. B ya dding delay and pitch shifting, wea re n ’t just simulating early re f l e c-tions from room surfaces any m o re .The spreader makes use of our signalp rocessing equipment (delay andp i t ch shifting) to create a big stere osound that only exists in loudspeake rmu s i c . This sort of thing doesn’t hap-pen in symphony halls, o p e ra houses,stadiums or pubs. I t ’s a studio cre-a t i o n , plain and simple.

Ta ke this effect further and yo uend up with what I think of as a‘ t h i cke n e r.’ Why limit the patch tot wo delays and two pitch ch a n g e s .What if you have the signal pro-cessing hors e p ower in your DAW orin your ra cks of gear to ch a i nt ogether eight or more delays andp i t ch shifts?

Try it. While it’ll sound unnaturalwhen used on vocals, many keyboardparts respond well to the thickeningtreatment. Modulate those delayslike a chorus and, guess what? Morepitch shifting is introduced.Addedin small, careful doses, this denselypacked signal of supportive, slightlyout-of-tune delays will strengthenand widen the loudspeaker illusionof the track.

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Big timeEnough with these subtle pitch

ch a n g e s . L e t ’s add a serious amountof pitch shifting.

Hammond B3 organs and manyblues guitars are often sent thro u g ha rather wa cky device: the LeslieC ab i n e t . The Leslie is a hybrid effectthat is built on pitch shifting, vo l u m ef l u c t u a t i o n , and often a good dose oftube ove rd r ive distortion.

It is essentially a tricked out gui-tar or keyboard amp in which thespeakers rotate. Honest. The highfrequency driver of a Leslie is hornloaded, and the horn spins aroundwithin the amp.

C razy as it sounds, the engineerswho came up with this we re re a l lyt h i n k i n g . It would be ve ry difficult tospin the large woofer to continue theeffect at low fre q u e n c i e s . I n s t e a dt h ey enclosed the woofer inside ad r u m . The drum has holes in it andro t a t e s . The result is a low fre q u e n cys i mulation of what the Leslie isdoing with the horns at higher fre-q u e n c i e s , e r, we l l , sort of.

The Leslie is too funky a device toc over in detail now, but we mentionit because it is part of our pitchshifting toolkit.

So what’s it sound like? With thedrum and horn ro t a t i n g , the loudnessof the music increases and decre a s e sat any given listener position—amplitude modulation. And with thehigh fre q u e n cy horn spinning by, aDoppler effect is created: the pitchi n c reases as the horn comes towa rdthe listener/microphone and thend e c reases as the horn travels away.

The typical example used in thes t u dy of the Doppler effect is a tra i ngoing by, horns ab l a ze . That classicsound of the pitch dropping as thet rain passes is based on this princi-p l e . Sound sources appro a ching witha ny appre c i able velocity willi n c rease the perc e ived pitch of thes o u n d . As the sound source departs,the pitch similarly decre a s e s . The netresult of the Leslie system then is aunique fluttery and wo bb ly sound.

The Leslie effect is used whereve rB3s and their ilk are used. Ty p i c a l lyoffering two speeds of ro t a t i o n , yo ucan hear a fast Leslie and a slowLeslie effect, as well as the accelera-tion or deceleration in betwe e n .

Listen to the single note org a nline at the introduction to ‘ Ti m eand Time Again’ on the CountingC rows’ first re c o rd , August AndEverything After. The high notee n t e rs with a fast rotating Leslie.As the line descends, the speed isre d u c e d . Listen care f u l ly thro u g h-out this song, this album, and other

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B3-centric tunes and you’ll hear theLeslie pitch shifting vo c ab u l a rythat key b o a rdists love .

Of cours e , you can apply it to anyt ra ck you like — g u i t a r, vo c a l , o b o e —if you have the device or one of itm a ny imitators or simu l a t o rs .

The hazard with an obvious pitchshift is that it can be hard to getaway with mu s i c a l ly. Yo u ’ ve heardspecial effects in the movies and onsome re c o rd s , w h e re a vocal is shift-ed up or down by an octave or more .Too low and it conjures up imagesof death robots invading the mix toeat Shreve p o r t . Too high and yo u rsinger becomes a gre m l i n - o n - h e l i u msort of disaster.

In the hands of talented mu s i c i a n s ,a g gre s s ive pitch shifting re a l lywo rk s . TA N K A PA (The Artist NowK n own As Prince Again) lowe rs thep i t ch of the lead vocal tra ck andt a kes on an entire ly new persona inthe song, Bob George from The BlackA l bu m. The effect is obv i o u s . Th eresult is fa n t a s t i c .

No effort was made to hide theeffect in the bass line ofSledgehammer on Peter Gab r i e l ’sclassic ‘ S o.’ The entire bass tra ckseems to include the bass plus thebass dropped an entire octave .A n dthe octave down bass line is mixedright up there with the original bass.Nothing subtle about it.

You can even use a pitch shifter toa dd two - ,t h re e - , or fo u r-part harmonyif you are so inclined. But get outyour arranging book, because the

p i t ch shifter makes it easy to add ac o n s t a n t ,n ever ending, n ever ch a n g-i n g , just plain annoying harmony line.

Dial in a pitch change that is amajor third up and add it to the leadvo c a l . If the song is entire ly diatonicwithin a major key and is a ve ryh a p py song, I mean ve ry happy, t h i smight wo rk . Otherwise it is going tosound cloy i n g ly swe e t , l i ke add i n gmaple syrup to the ice cream you puton top of your shoo fly pie.

The trick to creating harmoniesusing pitch shifting is to composemusical harmonies. And a staticp i t ch shift will ra re ly cut it.

Fo r t u n a t e ly, d evices and softwa replug-ins to facilitate this abound (pro b-

ab ly the most famous is the DigiTe chVocalist series).The pitch shifting cane s s e n t i a l ly be tied to MIDI note com-mands enabling you to dictate the har-monies from your MIDI contro l l e r.Th ep i t ch shifter is processing the vo c a lline on tape or disk according to thenotes you play on the key b o a rd .

This results is a harmony or coun-t e r m e l o dy line with all the harmonyand dissonance you desire . I t ’s builton a single vocal tra ck , and re l i e salmost entire ly on good soundingp i t ch shifting.

Go beyond harmonies. Use pitchshifting to turn a single note into ane n t i re ch o rd . String patches cansometimes be made to sound moreo rch e s t ral with the judicious add i t i o nof some perfect octave and perfectfifth pitch shifting (ab ove and/orb e l ow) to the patch .

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And don’t stop with simple inter-va l s .C h o rds loaded with tensions areo k ay too, used we l l . Yes put it fro n tand center in ‘Owner of a LonelyHeart’ on the album 90125. S i n g l e -note guitar lines are tra n s formed intosomething more magic and less gui-t a r- l i ke using pitch shifters to cre a t ethe other notes.

A final obvious pitch shiftingeffect worth mentioning is the stoptape effect. As analog tape risksex t i n c t i o n , this effect may soon belost on the next generation of re c o rd-ing mu s i c i a n s .

When an analog tape is stopped, i td o e s n ’t stop instantly; it takes aninstant to decelera t e . L a rge reels oft a p e , l i ke two inch 24 tra ck , a re pre t-ty darn heav y. It takes time to stopthese large reels from spinning. I fyou monitor the tape while it tries tostop (and many fa n cy mach i n e sresist this, a u t o m a t i c a l ly muting to

avoid the distraction this causes dur-ing a session), you hear the tape slowto a stop. S ch l u m p. The pitch dive sd own as the tape stops.

This is sometimes a musical effect.And it’s not just for analog tape, a sGarbage demonstrates via a ProTools effect between the bridge andthe third Chorus of ‘I Think I’mPa ranoid’ on their second album.

Surgical effectsP i t ch shifting is also used to zo o m

in and fix a problematic note. We ’ veall been there .

In the old days of mu l t i t ra ck pro-duction (about a year ago), we usedto sample the bad note. Then wetuned it up using a pitch shifter. I twas raised or lowe red to taste.Fi n a l ly, the sampled and pitch shift-ed note was re - re c o rded back ontothe mu l t i t ra ck . With the pro b l e m a t i cnote shifted to pitch perfection, n oone was the wiser.

That was then. N ow, c l ever softwa retaking advantage of powerful hard-

wa re permits pitch shifting to be donea u t o m a t i c a l ly (Antares Au t o Tu n e[ h a rdwa re and softwa re ve rs i o n s ] ,Wave Mechanics Pitch Doctor, T CE l e c t ronic Intonator, e t c . ) . That is, t h eeffects device can monitor the pitch ofa vo c a l ,v i o l i n , or didgeridoo. When itdetects a sharp of flat note, it shiftsthe pitch automatically by the amountn e c e s s a ry to re s t o re tuning. Wow. A n dit re a l ly wo rk s .

But please be careful with thesed ev i c e s . Fi rs t ,d o n ’t over polish yo u rp ro d u c t .P i t ch shifting eve rything intoperfect tune is ra re ly desirab l e .Vi b ra t ois an obvious example of the de-tuningof an instrument on purp o s e .

And if Bob Dylan had been pitchshifted into perfect pitch , w h e rewould folk music be now? Th e re is alot to be said for a musical amountof ‘ o u t - o f - t u n e n e s s .’ Remove all thewa r t s , and you risk re m oving a lot ofemotion from the perfo r m a n c e .

S e c o n d , d o n ’t expect to create ano p e ra singer out of a lounge cro o n e r.Th e re is no replacement for actualmusical ab i l i t y. If the bass playe rc a n ’t play a fre t l e s s , g ive her one withthose pitch-certain things called fre t s .If the violin player can’t control hisi n t o n a t i o n ,h i re one who can.

D o n ’t expect to rescue poor mu s i-cianship with automatic pitch corre c-t i o n . People want to hear your mu s i c ,not your effects ra ck .

Out of timeThis month re p resents our fo u r t h

month of discussion on delay. A re wedone yet? Natura l ly, n o. We continu eour tour of the delay in a future Nuts& Bolts installment when we take adetailed look at reve r b .

Alex Case strapped his pitch shifter tohis gear shifter and drives by ch a n t i n g .

Request Nuts & Bolts topics viac a s e @ re c o r d i n g m a g . c o m .

If Bob Dylan had been

p i t c h - s h i fted into perfect pitch,

where would folk music be now?

Excerpted from the October edition of RECORDING magazine.©2000 Music Maker Publications, Inc. Reprinted with permission.

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