Experiencing beats
The best way to understand beats is to hear them. We start with a reference tone of \(440\,\text{Hz}\), the note A. Choose a chip in Fig 2.1 and press Listen. The drawn curve follows the chip, and so does the sound.
Reference tone (440 Hz). The first chip plays \(440\,\text{Hz}\) alone. Its loudness is steady, and its envelope in Fig 2.1 is flat.
Slow beats (2 Hz). Now add a second tone at \(442\,\text{Hz}\), so \(\Delta f = 2\,\text{Hz}\). Listen for the two slow pulses per second. In the drawing, the envelope pinches to zero twice in the second.
Faster beats (4 Hz). If we raise the second frequency to \(444\,\text{Hz}\), then \(\Delta f = 4\,\text{Hz}\). The pulsing becomes noticeably faster, four times a second. The pitch you hear rises a little too, to the average, \(442\,\text{Hz}\).
Perfect unison (0 Hz beats). When an instrument is perfectly in tune, the two frequencies match, and \(\Delta f = 0\). The beat frequency becomes zero, and the pulsing disappears. What remains is a steady, combined tone. The last chip plays two tones of \(440\,\text{Hz}\), each at amplitude \(0.7\). Their envelope is flat at \(0.7 + 0.7 = 1.4\).
In the unison chip, two \(440\,\text{Hz}\) tones of amplitude \(0.7\) each sound together, in phase. What does the resultant look like?
Tuning musical instruments
This effect is fundamental to tuning instruments. A musician plays a reference note and the same note on the instrument, both at once. If beats are heard, the instrument is out of unison with the reference. The musician adjusts the tuning until the beats become slower. When the beats finally disappear, \(f_{\text{beat}} = 0\), and the two frequencies are perfectly matched.
Before a concert, a sitar player sounds a string together with the steady drone of the tanpura. If the two notes differ by \(3\,\text{Hz}\), the sound throbs three times a second. The player turns the peg slowly. If the throbbing slows, the string is moving towards the drone; if it quickens, the peg is turned the wrong way. The player stops when the throbbing can no longer be heard.
Two tuning forks produce \(4\) beats per second when sounded together. You increase the frequency of one fork slightly, and the beat frequency decreases to \(2\) beats per second. Which fork's frequency did you increase?
A tuning fork of frequency \(384\,\text{Hz}\) gives \(3\) beats per second when sounded with another tuning fork. What are the possible frequencies of the second fork?
One beat rate, two possible frequencies
The last check shows a limit of beats. A beat rate gives the size of the mismatch, \(|f_1 - f_2|\), but not its sign. An unknown fork can lie above the known one or below it by the same amount. To decide, we change the unknown fork a little in a known direction and listen again.
A tuning fork vibrates like a mass on a spring. Its prongs are the mass, and the bending of the metal is the spring. So the frequency of a fork depends on the mass of its prongs:
- Waxing a prong adds mass. More mass lowers the frequency.
- Filing the ends of the prongs removes mass. Less mass raises the frequency.
Where the metal is filed matters. Filing near the ends of the prongs removes mass where it moves most, so the frequency rises. Filing near the base, where the prongs join, weakens the bend that acts as the spring, and the frequency falls instead. Problems mean the ends unless they say otherwise.
Fig 2.2 shows the rule at work. Waxing B moves both possible values down by \(2\,\text{Hz}\). The value \(260\,\text{Hz}\) moves to \(258\,\text{Hz}\), towards A, so its beats fall to \(2\) per second. The value \(252\,\text{Hz}\) moves to \(250\,\text{Hz}\), away from A, so its beats rise to \(6\) per second. So the change in the beat rate tells us which candidate was true.
A tuning fork A of frequency \(256\,\text{Hz}\) gives \(4\) beats per second with a fork B of unknown frequency. When a little wax is put on the prongs of B, the beats fall to \(2\) per second. Find the frequency of B before it was waxed.
Known: \(f_A = 256\,\text{Hz}\), \(f_{\text{beat}} = 4\,\text{Hz}\) before waxing, and \(2\,\text{Hz}\) after. Waxing adds mass to B, so \(f_B\) decreases.
From \(|f_A - f_B| = 4\), the two candidates are \(f_B = 256 + 4 = 260\,\text{Hz}\) and \(f_B = 256 - 4 = 252\,\text{Hz}\).
If \(f_B = 260\,\text{Hz}\), a slight lowering brings B closer to \(256\,\text{Hz}\), and the beats fall. If \(f_B = 252\,\text{Hz}\), a slight lowering takes B further from \(256\,\text{Hz}\), and the beats rise. The beats fell.
So \(f_B = 260\,\text{Hz}\) before waxing. After waxing it is about \(258\,\text{Hz}\), which gives the observed \(2\) beats per second.
The rule assumes a small change. Suppose so much wax is added that \(260\,\text{Hz}\) falls to \(252\,\text{Hz}\). Then the beats are still \(4\) per second, because B has crossed over to the other side of A. A beat rate that does not change after waxing means exactly this. B was above A and dropped by twice the beat frequency.
A fork of unknown frequency gives \(5\) beats per second with a \(512\,\text{Hz}\) fork. The ends of the prongs of the unknown fork are filed a little, and the beats become \(7\) per second. What was the unknown frequency before filing?
Fork P has a frequency of \(300\,\text{Hz}\), and fork Q gives \(4\) beats per second with it. This time a little wax is put on P, the known fork, and the beats become \(6\) per second. What is the frequency of Q, in Hz?
A tuner hears \(3\) beats per second between a guitar string and a reference fork. Why can the beat rate alone not tell the tuner whether to tighten or loosen the string, and what should the tuner do?
The beat rate is \(|f_1 - f_2|\), the size of the difference without its sign. A string \(3\,\text{Hz}\) sharp and one \(3\,\text{Hz}\) flat give the same beats. The tuner tightens the string slightly, which raises its frequency. If the beats slow down, the string was flat and should be tightened further. If they speed up, it was sharp and should be loosened.
The two propellers of a twin-engine aircraft each hum at a frequency set by the speed of its engine. If the two speeds differ a little, passengers hear a slow, tiring throb, which is beats. Pilots, and in newer aircraft an automatic synchroniser, adjust one engine until the throb disappears. The engines then turn at the same rate, and the cabin is quieter.
- Giving only one value for an unknown frequency from a beat rate.\(|f_1 - f_2| = f_{\text{beat}}\) has two solutions, \(f_2 = f_1 \pm f_{\text{beat}}\). Keep both until more information decides.
- Thinking that wax raises the frequency of a fork.Wax adds mass, and more mass vibrates more slowly. Filing the ends of the prongs removes mass and raises the frequency.
- Forgetting which fork was changed.If the known fork is waxed or filed, move the known value, then compare it with both candidates for the unknown one.