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30 gennaio Talking about Dos and Don
Judges, left, Randy Jackson, Paula Abdul, and Simon Cowell will help
America choose the next "Idol."
Dos and Don'ts for 'Idol' Hopefuls A handy checklist for what to do (and what not to do) if you
want a shot at winning the show
By Larry Carroll Every new year brings with it hope. The hope of world peace, of good health for friends and family and, naturally, renewed hope for thousands that they'll make it through the nationwide auditions to become the next "American Idol." This year's process has already begun, and Season 7 launched Jan. 15. But, if
you're among the few and the chosen, are you really ready for prime time? Based
on the fact that the same judges, and the same die-hard millions who've powered
"Idol" in the past, will be returning once again, the time has come to start
looking for patterns. So sit back, rest those vocal cords with some herbal tea, and read on. Because if you're going to become Season 7's big winner, you'll definitely want to hit these notes. Don't Dance Dog Is Your Co-Pilot Check Yourself Before You Wreck Yourself The South Shall Rise Again Pick Popular Songs Don't Be a Freak Don't Be a Skank Don't Ring in the New Year Gain a Few Pounds If You Haven't Got the Talent, Stay Home 20 gennaio Engineering and the Guitar (Part 4)In this series, we’ll try to de-mystify some engineering terms by using something familiar to many of us: the acoustic guitar. Formulas: Who Needs ‘Em? You know, it’s amazing the reaction some people have when they have to solve, or in some cases “memorize” a formula—they’d rather scrape gum off the sidewalk than go through the math. Hey, don’t fall into that trap! Formulas are the magic key to the kingdom. Sometimes the simplest formula holds the secret to understanding how something works…why an airplane can fly or why your skateboard flexes without breaking. Of course developing the formula is just the start. Once you “get” what the formula is trying to tell you, you might even be able to improve the design—the design of a car, a radio, a windsurfer or a guitar. The word “guitar” in the title of this article should give you a clue as to which one of these systems we’re going to use as an example. It will be an ACOUSTIC guitar…one with nylon strings. By the way, if you really understand what a formula’s trying to tell you, ‘memorizing’ becomes trivial. Understanding and deduction are great memory aids. The CHALLENGE: DERIVE THE FORMULA FOR THE FREQUENCY (PITCH) OF A GUITAR STRING. There are a couple of ways we could do this. One is to delve into the mathematics of vibration, looking at the variables surrounding the string. This answer is readily available in physics textbooks. The more interesting way, one often used by practicing engineers, is to just try a few things. You might accidentally get the answer, and you might even learn something along the way. THEN you can go back and verify the answer with math. Yeah, you still need to be able to handle the math, but this way it will feel much easier. Let’s start by examining an acoustic guitar. What can you tell just by looking at it?
OK, that didn’t take a rocket scientist, and we can deduct a lot from our observation. [Hint: 90% of innovation in engineering is observing and being prepared to notice when something weird happens.] GUESS A formula has a DEPENDENT VARIABLE…the thing you’re trying to analyze (in our case, the string frequency). There are also some INDEPENDENT VARIABLES—things that affect the dependent variable. So our first guess is… f = F {string length}* F{Some Other stuff} That is, the frequency f is a Function of the length of the string and some other independent variables. The first part should be a pretty easy “win” for us…after all, that’s why the frets are on the guitar. Pluck the low E string without touching it with your other hand. The E string is the largest string, the one with the lowest pitch. When you don’t push down on any frets, it’s called an open string. Now push the same string down to any fret and pluck it. Does the pitch (frequency) go up or down? The answer’s pretty obvious: the pitch goes up as you use frets that are closer and closer to the bridge. That means the frequency is INVERSELY proportional to string length. In other words, the shorter the string, the higher the pitch. Oops…that means our first guess was upside down. Let’s change it to… f = F {1/string length}* F{Some Other stuff} OK, so we know somehow it’s proportional, but is it a linear relationship? Let’s find out by halving the length of the string, and measuring the frequency. If it’s linear, the frequency should double. Find the fret that’s located where the guitar body meets the neck. That’s usually the 12th fret. What we’re after is the place where the string is exactly _ of its “open” length. Push down the string against this fret and pluck the string. What do you hear? We can either test this with a frequency meter or an oscilloscope, or in this case, we can simply listen. It turns out that, at the halfway point, the frequency of vibration is exactly TWICE that of the open string. In musical terms, this is one OCTAVE higher. The term ‘octave’ comes from the fact that eight musical steps are required to get from one note to its equivalent higher note: ABCDEFGA. Logically, I count only seven steps in this sequence, but musicians also count the note they started on. [I know, it sounds crazy to me too, but I’m an engineer, not a musician.] We now have our first relationship with some certainty. The frequency is inversely proportional to the string length, and we can prove it’s linear by dividing the length into fourths, etc. Indeed, it is a linear relationship. So… f = {1/string length}* F{Some Other stuff} Pretty cool. And so far, we haven’t opened a math book, although we’ll do that later. POSITION Let’s
experiment by using a tuning fork. As the two tines of the fork move
back and forth in sympathetic vibration, the fork produces a fairly
pure sound of known frequency. To tune guitars, most musicians use a
fork tuned to an “A” note at 440 Hz.
Strike the tuning fork (not on the guitar!), and put its base against the neck of the guitar. What happens? Now strike it again and try it against the side of the guitar. And the back. And the top. It’s pretty obvious that the volume of the sound increased dramatically when you put the tuning fork near the bridge on the top of the guitar. It's almost like having an amplifier built into the guitar. Looks like there’s a reason they chose that spot for the bridge. By touching the tuning fork to the top of the guitar, we get the whole top vibrating at the frequency of the fork. OK, so we didn’t expect the pitch to change with location, but one thing happened that would not have happened if we just played with the math—we learned something extra. Guitar makers have long known that the top, or soundboard, is the most important component of the guitar. In fact, some very good acoustic guitars are constructed with the back and sides made of plastic, but with the top made of the best wood available. One famous guitar maker even created a guitar with a back made of papier-mâché, just to prove the point. It made a pretty decent sound. TENSION Sure. With more tension, the frequency goes up. So… f = {1/string length}* F{Tension + Some Other stuff} That is, the frequency (pitch) is proportional to tension and inversely proportional to length. Is it linear? Just
get a broom handle, and either drill a hole through the broom, or wrap
the guitar string so that you can rotate the broom handle and keep the
length exact. The string length is about 65 cm, or about 24-26 inches
for a standard guitar. Suspend a bucket from the other end of the
string, and just start adding small weights until you get the right
frequency when you pluck the string.
There’s a rule in experimentation: Only change ONE variable at a time. That’s why you have to keep the type of string and its length the same. The top of the bucket handle will be a pretty good “node”, which means you can do a pretty good job of defining the string length. Now start adding weights, beginning with a 2-kg weight. Don't forget to count the weight of the bucket. By the way, if you’re having trouble hearing the tone produced as you pluck the string, you could VERY CAREFULLY hold the guitar upside down against the broom handle, with the bridge just touching the handle. You’ll be amazed how much louder the note is. What did you find? On my guitar, the tension was about 7 kg. per string. Think about that--multiply 7 kg by 6 strings, and that’s the weight of a sack of concrete! Now imagine suspending a bag of concrete from the face of that beautiful guitar. It must have taken a lot of experimentation (and more than a few tears) for the early guitar makers to come up with the right bracing to have the wooden top withstand such a force and still vibrate freely. The bracing is every bit as sophisticated as that of a highway bridge.
Fig 1. 7 kg X 6 strings = 42 kg. That’s roughly the same weight as a standard sack of concrete. Want to have some fun? Attach a set of guitar strings to a closet rod. Then attach the other end to each of six separate wooden handles. Have one person hold the rod while six other people hold one string each. Pull on the strings until you have a tone that's roughly the same frequency as that of the appropriate guitar string. The poor person on the closet rod, who has to pull against all the other six strings, is in for a real workout. It gives you a good idea of how much force there is on the guitar's bridge. If you have the luxury of using an oscilloscope to measure the frequency, you can create a plot of frequency vs. weight. What you’ll find is that the relationship is NOT linear. So… f = {1/string length}* F{Tension + Some Other stuff} …which is what we had before, but now we at least know that the formula is NOT simply {tension/length}. MASS Try this: Pluck the low E (6th) string. Now pluck the high E (1st) string. They should be two octaves apart in frequency. Now loosen the tuning peg of the high E string such that it matches the frequency of the low E string. What do you notice? Incredibly,
what was once the high E string is now almost impossible to play. It’s
too loose. It’s also extremely difficult to keep it in tune at the
lower frequency. This must have something to do with the fact that the
six strings are different. Let’s take another guess. The guess is that
the mass of the string is important. We could create an engineering
model for this system--let’s assume it looks like:
Fig 2. The model has two springs and a weight in the center. In our model, the string is made of two springs, with a mass in the center. Let’s try it on the guitar. Re-tune the high E string to its former pitch. (It should be the same pitch as the next string, when the next string is played on its fifth fret.) Now put a small piece of putty on the high E string. Something like tacky putty works, but it’s more dramatic if you use lead putty from a local fly-fishing shop. (You can buy it in the non-lead, or environmentally friendly version.) Put the putty exactly at the center of the string, typically on the fret where the neck joins the body of the guitar. Strike
the string very gently at the center, and see what happens to the
frequency. Now strike the string just above the hole in the guitar top
and notice what happens.
Fig 3: Adding some lead putty (center) to the high “E” string radically changes the acoustic properties of the string. The result? The tiniest piece of lead putty not only lowers the fundamental frequency of the string, but it also has a devastating effect on the quality of the tone. That
explains it. Now we know why the strings are wound with metal wire.
It’s to create a DISTRIBUTED weight system that evens the extra weight
out over the entire string. The model should be more like this:
Fig 4: A better model distributes the weight all along the string. Distributed models are typically used to emulate complex devices like transmission lines. That adds the last independent variable to our equation: f = {1/string length}* F{Tension, Mass and maybe some other stuff} In fact, if we open a physics book and do the math we’ll find the string frequency is:
This of course is a simplified equation. If you want to get picky about it, you can add effects due to temperature, barometric pressure, gravity and all kinds of other second-order effects, but the major items are here. What does this equation tell you? It says:
Well, we learned a lot by experimenting to find the answer. The hands-on approach taught us a few things that we would not have learned if we had simply focused only on the mathematics of string vibration. And, knowing what you now know about guitars, you might consider designing your own musical instrument. Let your imagination run wild. For example, how about making a string instrument that uses an entire building? You could suspend a huge diaphragm that looks like a drumhead on the ceiling of an auditorium, and connect a large cable to it. You'd have to figure out how to "pluck" the 30-meter long "string", but once you did the "instrument" would produce a sound too low in pitch to hear, but you could "feel" the sound once you were seated. It's your world. Explore it. ©2002 |
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