Module VIII
Play the real horn in front of a class while the screen measures it. Ready-made demonstrations for maths and science, ages 11–18.
1.Set up (two minutes)
Laptop on the projector, within a couple of metres of you. Open this page, press Start the microphone and allow it. Set B♭/F or straight B♭ in the header to match your instrument.
2.Play, then ask
Each card says what to play, what the class should look at, and the questions to ask before you explain. Keep the Reveal folded until they have guessed.
3.Let them measure
Use Capture to log one note per slide position. The class’s own numbers make the graph — predictions, error and all.
live lab · play the real trombone
note (sounding)
—
play a long note
frequency
—
vibrations per second (Hz)
period
—
milliseconds per vibration
wavelength
—
metres · λ = v ÷ f, v = 343 m/s
harmonic no. (position 1)
—
pick the tube below
the tube you’re playing
Position 1: lowest possible note (the pedal) ≈ 58.3 Hz. Every note you can play here is a whole-number multiple of it.
Try: one harmonic — the F on the fourth line of the bass staff in 1st, then down through positions 1→7 without changing your lips — capturing each. The prediction is ÷ 1.0595 per position.
the run-sheet
The lips are a valve, opening and closing about 117 times a second. On their own they buzz at whatever speed they like — a messy spectrum. In the horn, the air column has a few frequencies it 'likes' (resonances) and it pushes back on the lips until they lock to one of them. The spectrum turns into clean, evenly spaced spikes.
frequency = vibrations per second. B♭ ≈ 116.5 Hz → one vibration every 1 ÷ 116.5 = 8.6 milliseconds.
Sound as vibration; frequency and pitch (NCERT/CBSE Class 8–9 ‘Sound’; NGSS MS-PS4-1).
A tube of fixed length can only resonate at whole-number multiples of its lowest frequency (the pedal B♭, 58.3 Hz). The notes you can lip-slur to are the 2nd, 3rd, 4th, 5th and 6th of those multiples — the harmonic series. The gaps between them are big at the bottom and close up at the top, so there are notes in between that this length of tube simply cannot make. That is what the slide is for.
58.3 × 2, 3, 4, 5, 6 = 116.5, 174.8, 233.1, 291.4, 349.6 Hz. Ratios 2 : 3 : 4 : 5 : 6. Octave = 2 : 1, fifth = 3 : 2, fourth = 4 : 3.
Multiples and ratio (CCSS 6.RP.A.1); sequences; harmonics (HS physics: standing waves in pipes).
Sound travels at a fixed speed in the room. The tube length sets the wavelength, so frequency = speed ÷ wavelength falls as the tube grows. Double the length, halve the frequency: frequency × length is a constant. The graph is not a straight line — it is the reciprocal curve.
f × L = constant ⇒ f = k ÷ L. On harmonic 3 at 20 °C, f × L for the whole air column ≈ 1.5 × 343 ≈ 515 Hz·m.
Inverse proportion and non-linear functions (CCSS 8.F.A.3); v = fλ (NGSS HS-PS4-1).
One semitone lower always means the whole tube × 1.0595 (the twelfth root of 2). The tube is longer each time, so 5.95% of it is a slightly longer piece each time: the gaps grow from about 8.1 cm to 10.9 cm. Equal ratios, not equal steps — that is exponential growth.
L(n) = L₀ × 2^((n−1)/12). Gap from 1st to 2nd = 2.74 m × 0.0595 ÷ 2 ≈ 8.1 cm (÷2 because the slide is a U: moving it 1 cm adds 2 cm of tube).
Linear vs exponential (CCSS HSF-LE.A.1); rational exponents, 2^(1/12) (CCSS HSN-RN.A.1).
The trigger switches in about 0.92 m of extra tubing, making the horn 1.335 times longer — a perfect fourth lower. Because every trigger semitone needs 1.335 times as much slide, the positions spread out: only six fit, and the seventh (low B) would be 75.7 cm out, past the end of the slide.
2^(5/12) = 1.3348 ≈ 4/3 = 1.3333. B♭ 7th = 56.7 cm × 1.335 = 75.7 cm. Tenor slide ends near 64 cm.
Ratio, scale factor and percentage increase; approximation.
Sound travels faster in warm air. The tube fixes the wavelength, so if the speed goes up the frequency must go up too: the horn goes sharp as it warms. Cold horn, flat band.
v ≈ 331.3 + 0.606 T m/s. 20 °C → 343.4 m/s; 30 °C → 349.5 m/s, 1.7% faster. 10 °C of warming ≈ 29 cents sharp — over a quarter of a semitone.
Speed of sound in different conditions; v = fλ (NCERT/CBSE Class 9 ‘Sound’; NGSS HS-PS4-1).
Pitch is the spacing of the spikes — set by the lowest frequency. Timbre is the pattern of their heights. Playing loud pushes energy into the high harmonics, which is the bright brassy edge; a mute filters some harmonics out. Same spacing, different shape.
The spikes stay at f, 2f, 3f … The vertical axis is in decibels — every 10 dB is ten times the power.
Pitch, loudness and quality of sound (NCERT/CBSE Class 8–9 ‘Sound’); reading graphs.
Two notes a few hertz apart fall in and out of step. The sound swells each time they line up: the swell happens |f₁ − f₂| times a second. When the beats stop, the two are in tune — which is exactly how brass players tune to each other.
233 Hz against 236 Hz → 3 beats per second.
Subtraction, rates; superposition of waves (HS physics).
Syllabus lines say which school topic each demonstration serves (CBSE/NCERT, Common Core and NGSS codes where they fit). They are pointers for the teacher, not endorsements — no exam board has reviewed Atlas.