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LNGR SPKRHIFI. TWO WAYS. HANDCRAFTED.
Knowledge / Power, control & measurement
LNGR · Learning workshop

Measure rather than guess

A measurement only answers questions its setup can support. Room, windowing and reference quantities belong with the curve.

Δf ≈ 1/TTime ↔ frequency

Functional illustration · equations and topology in the text

Start without prior knowledgeUnderstand the model limitsDE / EN
01

The mental picture

A photo can be sharp yet show the wrong crop. A frequency response can similarly look clean while its conditions hide an important property. A short time window excludes later reflections but sacrifices low-frequency resolution.

02

The principle

Electrical impedance and acoustic response are different loudspeaker measurements. Acoustic work needs documented position, distance, excitation and suitable microphone calibration. Combining drivers requires a consistent timing reference.

03

Try it yourself

Interactive experiment

Measure rather than guess

Compare 5 ms and 20 ms windows. Characteristic frequency resolution improves, but the longer window may include more room reflections.

Model limits: Only the relation between window length, approximate frequency resolution and path difference. No simulation of a specific room or measurement system.

04

A worked example

A 5 ms window corresponds roughly to 200 Hz frequency resolution. Smoothing does not make a response below that range suddenly reliable. At 343 m/s, an extra reflection path of 1.715 m corresponds to about 5 ms.

A closer look · equations and assumptions
Formula notes
\Delta f\approx\frac{1}{T}
\Delta s=cT
c\approx343\,\frac{\mathrm{m}}{\mathrm{s}}

Δf ≈ 1/T is a guide, not a sharp validity boundary. Window shape and analysis change spectral behaviour. Near-field data can extend low-frequency information, but merging with far-field data requires correct scaling and consideration of different radiation conditions.

A common pitfall. Do not blindly add or compare curves taken at different levels, microphone positions or independent time offsets.

05

Workshop takeaway

Change one thing at a time and label it clearly. One simple reproducible measurement is worth more than ten ambiguous curves.

Sources & transparency

Original illustrations and educational calculations. No measurements of a specific product. Edited 11 October 2026.

Work it out · answers unfold

Write down your prediction first, then your calculation. Open the answer only when you are ready to compare.

01 · An unpowered resistor measures 998 Ω. Nominal value 1 kΩ. Find relative error.

Show worked answer
  1. Deviation: -2 Ω.
  2. Divide by nominal 1000 Ω.
  3. Result: -0.2%.
Calculation
\delta=\frac{998-1000}{1000}\cdot100\%=-0.2\%

02 · Why may an in-circuit resistance measurement be too low?

Show worked answer
  1. Other components may form parallel paths.
  2. The meter sees their equivalent resistance.
  3. Measure unpowered; isolate one lead if necessary.

03 · A 10 kΩ/10 kΩ divider at 10 V is measured across its lower resistor using a 10 MΩ voltmeter. Estimate the reading.

Show worked answer
  1. Lower equivalent resistance: 9990.01 Ω.
  2. U = 10 · 9990.01/(10000 + 9990.01).
  3. Reading: 4.9975 V.
Calculation
U_m\approx4.9975\,V

04 · The same 10 MΩ meter measures a 10 MΩ/10 MΩ divider at 10 V. Find the reading.

Show worked answer
  1. Lower resistor parallel meter: 5 MΩ.
  2. Divider: 10 MΩ upper, 5 MΩ lower.
  3. Reading: 3.333 V rather than unloaded 5 V.
Calculation
U_m=10\frac{5}{10+5}=3.333\,V

All new learning modules →

Project connection · LNGR 2-PR-THT-PR

See how driver spacing, passive radiators, crossover design and measurements meet in this planning project. CNC geometry v1.2; not yet built or acoustically measured.

Open the project build log →