The Phenomenon of Beats
Imagine you are standing in a room where two musicians are playing slightly different notes on their instruments. Instead of hearing a smooth, continuous sound, you hear a distinct "wobble" or a rhythmic pulsing in the volume. This fascinating acoustic phenomenon is known as beats.
Beats occur due to the principle of superposition. When two sound waves of slightly different frequencies interfere with each other, they periodically fall in and out of phase. When they are in phase, they construct a louder sound (constructive interference). When they are out of phase, they cancel each other out, creating a softer sound (destructive interference).
The number of these loud-soft cycles you hear per second is called the beat frequency. Mathematically, it is beautifully simple. The beat frequency is exactly equal to the absolute difference between the two source frequencies:
Analyzing the Initial State
In our problem, we are given a known tuning fork with a frequency of f1=288 Hz (or cps, which stands for cycles per second). When sounded together with an unknown tuning fork of frequency f2, they produce 4 beats per second.
Using our beat frequency formula, we can set up the following equation:
Because of the absolute value, this equation branches into two distinct possibilities. The unknown frequency could be 4 Hz higher than the known frequency, or it could be 4 Hz lower.
Possibility 1: f2=288+4=292 Hz
Possibility 2: f2=288−4=284 Hz
At this stage, we are at a crossroads. Both 292 Hz and 284 Hz are perfectly valid candidates. We need more physical information to break this tie.
The Physics of Waxing a Tuning Fork
This is where the problem introduces a physical manipulation: placing a little wax on the prongs of the unknown tuning fork. To understand what this does, we must look at the mechanics of a tuning fork.
A tuning fork behaves much like a simple harmonic oscillator, similar to a mass on a spring. Its natural frequency of vibration depends on two main factors: the stiffness of the metal (analogous to the spring constant, k) and the mass of the prongs (m). The relationship is given by:
When we stick wax onto the prongs, we are effectively increasing the mass (m) of the oscillating system without changing its stiffness. According to the proportionality above, an increase in mass in the denominator will cause the overall frequency (f) to decrease.
Therefore, whatever the original frequency f2 was, the new frequency f2′ after waxing must be strictly less than f2:
The Logical Deduction
Eliminating the Impossible
We are told that after the wax is applied, the new beat frequency drops to 2 beats per second. Let's test our two initial possibilities against this new constraint.
Testing Possibility 2 (284 Hz):
Suppose the original frequency was 284 Hz. Adding wax will decrease this frequency further. It might drop to 283 Hz, 282 Hz, or even lower.
Let's calculate the new beat frequency with the known 288 Hz fork. If the new frequency is, say, 283 Hz, the beats would be ∣288−283∣=5 Hz. The gap between the two frequencies is widening! The beat frequency would increase to 5, 6, or more.
However, the problem explicitly states the new beat frequency is 2 Hz. Since 284 Hz leads to an increase in beats, this possibility is physically impossible and must be rejected.
Testing Possibility 1 (292 Hz):
Now suppose the original frequency was 292 Hz. Adding wax will decrease this frequency. It will start moving down from 292 Hz towards the known 288 Hz.
If the frequency drops by exactly 2 Hz due to the wax, the new frequency becomes f2′=290 Hz. Let's check the new beat frequency:
This perfectly matches the condition given in the problem! By starting at a higher frequency, the decrease caused by the wax brings the unknown fork closer to the known fork, thereby reducing the beat frequency from 4 to 2.
The Final Conclusion
By systematically applying the physics of beats and the mechanics of harmonic oscillators, we have eliminated the incorrect path. The only logical conclusion is that the original frequency of the unknown tuning fork, before any wax was added, was indeed 292 Hz.