What is a decibel? A decibel (dB) is a logarithmic way of expressing the ratio between a measured quantity and a reference quantity. In airborne acoustics, the familiar sound pressure level compares measured root-mean-square sound pressure with a reference pressure of 20 µPa. The logarithmic scale compresses the enormous range of pressures the human ear can detect into practical numbers.
A decibel value is incomplete unless the acoustic quantity, reference, frequency weighting, and time descriptor are understood. 60 dB SPL, 60 dBA LAeq,8h, and a 60 dB sound power level do not describe the same thing. Learning those distinctions helps clients read noise surveys, product reports, and “dB reduction” claims correctly.
Key takeaways
- A decibel expresses a logarithmic ratio; it is not a linear unit like a metre or pascal.
- For sound pressure level in air,
Lp = 20 log10(p/p₀), wherep₀ = 20 µPa.0 dB SPLmeans the sound pressure equals the reference pressure. It does not mean that no sound exists.- A
3.01 dBincrease represents approximately twice the sound power or intensity; a6.02 dBincrease represents twice the sound-pressure amplitude.- Two equal, independent sound levels combine to approximately
+3 dB, not twice the dB number.- dB, dBA, and dBC are not interchangeable. A and C identify frequency weightings.
- A sound level must include a metric such as
LAeq,T,LAFmax, orLCpeakto be interpreted reliably.- NRC and αw describe sound absorption, not a guaranteed reduction in room level or sound transmission.
Table of Contents
- What is a decibel in acoustics?
- Why is the decibel scale logarithmic?
- How is sound pressure level calculated?
- Does 0 dB mean silence?
- What do changes of 3, 6, and 10 dB mean?
- How are decibel levels added and subtracted?
- What is the difference between dB, dBA, and dBC?
- Which sound-level metrics appear in acoustic reports?
- Sound pressure, sound power, and loudness
- How do distance and rooms change sound level?
- How to evaluate a “dB reduction” claim
- A practical sound-level measurement checklist
- Common decibel mistakes
- Frequently asked questions
What Is a Decibel in Acoustics?
The decibel, symbol dB, expresses the value of a specified logarithmic ratio. The BIPM SI Brochure states that 1 dB = 0.1 B, where B is the bel, and that bels and decibels use the base-10 logarithm. It also emphasizes that the underlying quantity and reference must be stated.
The decibel is accepted for use with the International System of Units, but it is not itself an SI unit. ISO 80000-8:2020, together with its 2025 amendment, provides names, symbols, definitions, and units for acoustic quantities.
The general form for a power-like quantity is:
LX = 10 log10(X/X₀) dB
where:
Xis the measured power-like quantity;X₀is its stated reference quantity;log10is the base-10 logarithm;LXis the resulting level.
This definition explains why a bare statement such as “the sound is 70 dB” lacks technical precision. Seventy decibels relative to what quantity, reference, weighting, averaging time, position, and operating condition? Everyday conversation may omit those details, but a specification or test report should not.
Is a decibel a measure of loudness?
Not directly. A sound level meter measures physical acoustic quantities, while loudness is a perception influenced by sound level, frequency spectrum, duration, temporal pattern, listening environment, and the listener. A higher sound pressure level often sounds louder when other conditions remain similar, but dB and loudness are not synonyms.
ISO 226:2023 specifies combinations of frequency and sound pressure level that are perceived as equally loud for pure tones under controlled conditions. Those equal-loudness contours show why identical dB SPL values at different frequencies need not sound equally loud.
Why Is the Decibel Scale Logarithmic?
Sound pressure encountered in acoustics spans a very large range. A commonly used airborne reference is only 20 µPa, or 0.00002 Pa, while a sound pressure of 20 Pa corresponds to 120 dB SPL. The pressure ratio between those two values is one million to one.

A linear scale would force engineers to work with many zeros and would make relative changes difficult to compare. A logarithmic scale converts multiplicative ratios into manageable differences:
| Sound pressure | Pressure ratio to 20 µPa | Sound pressure level |
|---|---|---|
| 20 µPa | 1 | 0 dB SPL |
| 200 µPa | 10 | 20 dB SPL |
| 2 mPa | 100 | 40 dB SPL |
| 20 mPa | 1,000 | 60 dB SPL |
| 0.2 Pa | 10,000 | 80 dB SPL |
| 2 Pa | 100,000 | 100 dB SPL |
| 20 Pa | 1,000,000 | 120 dB SPL |
Every 20 dB rise in sound pressure level represents a tenfold increase in pressure amplitude. Every 10 dB rise represents a tenfold increase in a corresponding power-like quantity, such as sound intensity under compatible conditions.
The logarithmic scale also matches the way many engineering systems are compared. Ratios become differences, multiplication becomes addition, and a wide dynamic range can fit on one chart. That convenience does not mean human hearing follows one simple dB-to-loudness rule in every situation.
How Is Sound Pressure Level Calculated?
Sound pressure level, commonly abbreviated SPL and written Lp, is the level most people mean when discussing the sound measured at a position in air. The equation is:
Lp = 20 log10(p/p₀) dB
where:
p= root-mean-square sound pressure in pascals;p₀= reference sound pressure,20 µPafor airborne sound;Lp= sound pressure level in decibels.
It may also be written as:
Lp = 10 log10(p²/p₀²) dB
The factor is 20 in the first form because acoustic power and intensity are related to the square of sound pressure under the relevant assumptions. The NIST Guide for the Use of the SI gives 20 µPa as the reference for sound pressure in air, while the OSHA Technical Manual provides worked examples of sound pressure, sound power, and level addition.
Worked example: 0.02 Pa
If the root-mean-square sound pressure is 0.02 Pa:
Lp = 20 log10(0.02/0.00002)
Lp = 20 log10(1,000)
Lp = 20 × 3 = 60 dB SPL
Worked example: 2 Pa
If the sound pressure is 2 Pa:
Lp = 20 log10(2/0.00002)
Lp = 20 log10(100,000) = 100 dB SPL
These are mathematical conversions, not universal examples of particular sound sources. The level produced by a voice, machine, vehicle, or loudspeaker depends on distance, direction, environment, operating state, measurement bandwidth, and time descriptor.
Airborne and underwater dB values cannot be compared casually
The standard reference pressure for airborne sound is not the same as the reference commonly used for underwater sound. The propagation medium and measurement conventions also differ. A numerical dB value reported underwater should therefore not be compared directly with the same numerical airborne value as though they represented identical pressure or risk.
Does 0 dB Mean Silence?
No. Zero decibels sound pressure level means that the measured root-mean-square pressure equals the reference pressure of 20 µPa in air. It does not mean zero pressure, zero acoustic energy, or a complete absence of sound.
A result below 0 dB SPL is mathematically possible when the measured sound pressure is lower than the reference. Sensitive laboratory systems and hearing tests can produce negative sound pressure levels in limited frequency bands. Negative dB does not mean “less than no sound”; it means “below the stated reference level.”
The reference is often associated with an approximate threshold of hearing under specific conditions, but real hearing thresholds vary by frequency and person. A listener may detect some frequencies below 0 dB SPL and require much higher levels at other frequencies. Background noise, ear condition, age, test method, and signal duration all matter.
The safest interpretation is simple: 0 dB is a reference point, not an acoustic vacuum.
What Do Changes of 3, 6, and 10 dB Mean?
Because the decibel scale is logarithmic, a numerical change represents a ratio. The meaning depends on whether the underlying quantity is power-like or amplitude-like.
| Level change | Power or intensity ratio | Sound-pressure amplitude ratio | Correct interpretation |
|---|---|---|---|
| +1 dB | 1.26× | 1.12× | A small physical change; audibility depends on conditions |
| +3.01 dB | 2× | 1.414× | Approximately double the power or intensity |
| +6.02 dB | 4× | 2× | Double the pressure amplitude |
| +10 dB | 10× | 3.162× | Ten times the power or intensity |
| +20 dB | 100× | 10× | Ten times the pressure amplitude |
The corresponding negative change uses the reciprocal ratio. A −3.01 dB change means approximately half the power, while −6.02 dB means half the pressure amplitude.
Does 10 dB sound twice as loud?
“A 10 dB increase sounds twice as loud” is a useful introductory approximation, not a universal physical law. Perceived loudness depends on starting level, frequency spectrum, bandwidth, duration, listening conditions, and the individual. ISO 226’s equal-loudness data apply to controlled pure-tone conditions and illustrate why frequency cannot be ignored.
For product or project communication, separate the measurable claim from the perceptual description:
- measurable: “
LAeqdecreased by 8 dB at the stated receiver position”; - perceptual: “occupants reported that the room sounded more comfortable”;
- unsupported shortcut: “the solution made the room exactly half as loud.”
Is a 1 dB change audible?
There is no one threshold that applies to every sound and listener. Under controlled comparison conditions, a small change may be detectable; in a changing occupied room, the same numerical difference may be masked. Measurement uncertainty can also be comparable to a small reported difference. Do not turn “1 dB” or “3 dB” into a universal noticeability rule without context.
How Are Decibel Levels Added and Subtracted?
Decibel values cannot normally be added arithmetically. Two independent machines that each produce 60 dB at the same receiver do not produce 120 dB. Their corresponding energy quantities are added first, and the total is converted back into decibels.
For compatible sound levels:
Ltotal = 10 log10(10^(L1/10) + 10^(L2/10) + ... + 10^(Ln/10))
Examples of level addition
| Source levels at the same receiver | Combined level | Practical lesson |
|---|---|---|
| 60 dB + 60 dB | 63.01 dB | Two equal independent sources add about 3 dB |
| 60 dB + 50 dB | 60.41 dB | A source 10 dB lower adds less than 0.5 dB |
| 60 dB + 40 dB | 60.04 dB | A source 20 dB lower has little effect on the total |
| Three sources at 60 dB | 64.77 dB | Three equal sources add about 4.8 dB |
| Ten sources at 60 dB | 70 dB | Ten equal sources add 10 dB |
These examples assume compatible levels from independent or incoherent sources and the same measurement conditions. Coherent sources can interact through phase, creating reinforcement or cancellation. A sound-system array therefore requires more analysis than simple energy addition.
Subtracting background sound
Acousticians may use logarithmic subtraction to estimate a specific source from an ambient measurement and a residual measurement. For compatible quantities:
Ls = 10 log10(10^(La/10) − 10^(Lr/10))
where:
La= ambient level with the source operating;Lr= residual level without the source;Ls= estimated specific source level.
If the ambient level is 65 dB and the residual is 60 dB, the calculated specific level is approximately 63.35 dB. When ambient and residual levels are too close, the result becomes highly sensitive to measurement variation and may be unreliable. The metrics, time periods, operating conditions, and measurement positions must match before subtraction is attempted.
What Is the Difference Between dB, dBA, and dBC?
dB identifies the logarithmic unit. dBA and dBC indicate that frequency weighting has been applied to the measured spectrum before the bands are combined into a single value.

Human hearing is not equally sensitive at all frequencies. Frequency weighting applies a standardized response to represent a stated measurement purpose. Sound level meter performance, including frequency-weighted and time-weighted levels, is covered by IEC 61672-1:2013.
| Expression | Meaning | Common use |
|---|---|---|
| dB or dB SPL | Unweighted or otherwise stated sound pressure level | Technical spectra, band levels, general acoustic calculations |
| dBA or dB(A) | A-frequency-weighted sound level | Environmental noise, occupational exposure, many building-noise criteria |
| dBC or dB(C) | C-frequency-weighted sound level | High-level or low-frequency-sensitive assessments, peak-related reporting when specified |
| dBZ or Z-weighted | Approximately flat response within specified limits | Broadband technical measurement and spectral analysis |
A-weighting attenuates low frequencies substantially and also reduces very high frequencies. C-weighting has less low-frequency attenuation. The difference between a simultaneous A- and C-weighted result can therefore indicate that low-frequency energy may be significant, but it is not a complete diagnosis. Octave- or one-third-octave-band data is more informative.
Is A-weighting the same as human loudness?
No. A-weighting is a standardized frequency response used for particular sound-level measurements. It does not model every level-dependent feature of hearing, temporal response, tonality, impulsiveness, binaural listening, or individual perception. It is useful because regulations and assessment methods define how to use it—not because it converts a meter into a complete loudness model.
Why the notation after dB matters
Compare these statements:
45 dB— incomplete unless the quantity and method are known;45 dBA— frequency weighting is clearer, but the time descriptor is still missing;LAeq,15min = 45 dB— A-weighted equivalent continuous sound level over 15 minutes;LAFmax = 45 dB— maximum A-weighted Fast time-weighted sound level.
The last two values can differ even when measured during the same event. ISO 1996-1:2016 specifically warns that several different physical measures can be expressed in decibels and that the underlying quantity must be specified.
Which Sound-Level Metrics Appear in Acoustic Reports?
A professional report does more than place “dB” after a number. Its subscripts define what the instrument measured and how the result was processed.
| Metric | Plain-language meaning | Typical question it answers |
|---|---|---|
LAeq,T | Energy-equivalent A-weighted continuous sound level over period T | What was the average sound energy during the stated period? |
LAFmax | Highest A-weighted level measured with Fast time weighting | What was the maximum indicated level during the event? |
LASmax | Highest A-weighted level measured with Slow time weighting | What was the maximum level with a slower instrument response? |
LCpeak | C-weighted peak sound pressure level | What was the highest instantaneous peak under the specified method? |
L90,T | Level exceeded for 90% of the stated period | What lower, persistent level characterized much of the period? |
Octave-band Lp | Sound pressure level in each frequency band | Which frequencies dominate the problem? |
LAFmax and LCpeak are not the same measurement. “Maximum” is the greatest value from an exponential time-weighted detector; “peak” tracks the greatest instantaneous pressure under its defined detector and weighting. A short impact can produce a peak result far above the maximum time-weighted result.
Metrics also depend on the application. Environmental noise, occupational exposure, building services, room acoustics, sound insulation, and product testing use different descriptors and standards. A consultant should select the metric before measurement, not search afterward for the most convenient number.
A safety note about 85 dBA
The U.S. National Institute for Occupational Safety and Health recommends an occupational exposure limit of 85 dBA as an eight-hour time-weighted average, using a 3 dB exchange rate. Under that recommendation, 88 dBA corresponds to four hours and 91 dBA to two hours for the same daily dose. See the NIOSH noise-exposure guidance.
This is an occupational exposure recommendation, not a universal comfort target, environmental limit, or statement that every brief exposure below 85 dBA is harmless. Applicable national regulations, exposure duration, impulsive sound, vulnerable users, and project requirements must be considered.
Sound Pressure, Sound Power, and Loudness
Several different concepts may all be described using “decibels.” Keeping them separate prevents major specification errors.
Sound pressure level: what exists at a position
Sound pressure level depends on the source, distance, direction, reflections, barriers, room absorption, and receiver position. A machine can produce different SPL values at 1 m and 5 m, or in a reverberant factory and an outdoor free field.
Sound power level: what the source emits
Sound power describes the total acoustic power emitted by a source. Its level is commonly calculated with:
Lw = 10 log10(W/W₀) dB
where W₀ = 1 pW, or 10⁻¹² W. Sound power level is a source property determined under a stated test method; it is not the level a person will measure at an arbitrary distance.
A product data sheet that lists Lw = 80 dB should not be rewritten as “the machine produces 80 dB at the listener.” Predicting receiver sound pressure requires source directivity, distance, room or outdoor propagation, barriers, and other paths.
Loudness: what a listener perceives
Loudness is perceptual. Two sounds with the same A-weighted equivalent level can still differ in perceived character because of spectrum, tonality, modulation, impulses, duration, and meaning. A tonal fan and broadband ventilation noise may therefore attract different reactions at similar headline levels.
Sound absorption and sound insulation: what the construction changes
Sound absorption reduces reflected sound energy within a room. Sound insulation reduces transmission from one space to another. Both can influence measured dB values, but they solve different problems and use different laboratory metrics.
- Read What Is Hertz (Hz)? Understanding Sound Frequency in Acoustics to understand why level must be examined by frequency.
- Read Understanding Noise Reduction Coefficient (NRC) Rating and What Does αw (Alpha-w) Mean? before comparing absorption products.
- Read What Is Reverberation Time? RT60 Explained to connect absorption with sound decay in rooms.
How Do Distance and Rooms Change Sound Level?
In an ideal free field, away from reflecting surfaces, sound from a small omnidirectional point source spreads over an increasing area. Doubling the distance reduces sound pressure level by approximately 6 dB:
Lp,2 = Lp,1 − 20 log10(r₂/r₁)
If a source produces 80 dB SPL at 1 m under those assumptions, the predicted level is approximately 74 dB at 2 m and 68 dB at 4 m. This is the inverse-square relationship expressed as sound pressure level.
Real buildings often depart from this model. The 6 dB per doubling rule can fail when:
- walls, ceilings, floors, or façades create strong reflections;
- the source is large or behaves more like a line than a point;
- the receiver is in the near field;
- several sources operate together;
- doors, openings, ducts, or structures create alternative paths;
- the room’s reverberant field becomes important;
- outdoor ground and weather conditions affect propagation.
Why acoustic panels do not provide one universal room-level reduction
Absorptive panels reduce reflected energy and can shorten reverberation time. The change in a meter reading depends on how much of the original level came from the direct sound and how much came from the reverberant field, along with coverage, placement, frequency response, room volume, source-receiver geometry, and occupancy.
Close to a loud source, direct sound may dominate, so adding wall absorption may improve decay and speech comfort without producing a large reduction at that microphone position. Farther away in a reflective room, reducing the reverberant contribution may have a greater effect. A tested NRC or αw value alone cannot predict one fixed dB reduction for every room.
How to Evaluate a “dB Reduction” Claim
“Reduces noise by 20 dB” sounds precise, but it is not verifiable without a test context. Before using such a statement in procurement, specification, or marketing, ask the following questions.
1. Which acoustic quantity changed?
Was it sound pressure level at a receiver, sound power level of a source, insertion loss, airborne sound reduction index, impact sound level, or another metric? All may use decibels, but they describe different systems.
2. Was it an absolute result or a difference?
“The completed room measured 40 dBA LAeq” is an absolute result. “The level decreased by 8 dB” is a before-and-after difference. The second statement needs both original and final conditions.
3. Which frequencies were included?
A product might reduce 1,000 Hz strongly but perform differently at 125 Hz. Ask for octave- or one-third-octave-band data instead of relying only on a broadband headline.
4. Which weighting and time descriptor were used?
An A-weighted equivalent level cannot be compared directly with an unweighted peak or a C-weighted maximum. Confirm whether the result is LAeq,T, LAFmax, LCpeak, band-limited insertion loss, or something else.
5. Where were the source and receiver?
Record distance, height, orientation, room, boundary, and microphone position. Moving the meter can change the result even when the product has not changed.
6. What were the operating and background conditions?
Machine load, number of sources, occupancy, doors, windows, HVAC state, weather, and residual noise must be comparable. A before-and-after test made under different conditions cannot isolate the treatment reliably.
7. What exact assembly was tested?
Thickness, density, air gap, backing, frame, joints, perimeter sealing, fasteners, substrate, and specimen size can affect performance. A result for a complete tested wall or ceiling build-up should not be assigned to a visually similar finish.
8. Which standard and laboratory were used?
A result is more useful when the report identifies the applicable test standard, laboratory, specimen, uncertainty, and date. Review Leeyin’s available acoustic test reports and match the evidence to the proposed assembly.
What NRC and αw do—and do not—prove
NRC and αw summarize sound-absorption performance under their respective methods. They can help estimate equivalent absorption and reverberation control. They do not directly state:
- the dB reduction at a listener position;
- the sound insulation between two rooms;
- the reduction of footsteps through a floor;
- the sound power reduction of a machine;
- the final acoustic comfort of every room.
If the complaint is excessive reverberation, absorption products may be appropriate. If sound passes through a wall, door, floor, ceiling, or façade, the solution may require mass, airtightness, decoupling, resilient layers, vibration isolation, and control of flanking paths. Start with the acoustic mechanism before selecting a product.
A Practical Sound-Level Measurement Checklist
A phone app can help identify patterns, but contractual, compliance, or hearing-risk decisions normally require suitable calibrated equipment and a defined method. IEC 61672-1 specifies performance requirements for Class 1 and Class 2 sound level meters.

Before measuring:
- Define the question: comfort, compliance, source diagnosis, sound insulation, or occupational exposure.
- Select the required metric, frequency weighting, time weighting, bandwidth, and duration.
- Choose equipment suitable for the applicable standard and expected level range.
- Check acoustic calibrator and meter calibration status.
- Document source state, room condition, occupancy, doors, windows, HVAC, and weather where relevant.
During measurement:
- Calibrate before the survey according to the method and record the result.
- Keep the microphone away from the operator’s body and unintended reflective surfaces unless the method specifies otherwise.
- Use a windscreen where required and avoid wind, handling, and cable noise.
- Record representative operating cycles rather than only a convenient quiet or loud moment.
- Note unusual events that may contaminate the result.
After measurement:
- Perform the required post-survey calibration check.
- Retain time histories and frequency spectra where useful.
- Report positions, periods, metrics, settings, equipment, calibration, and uncertainty.
- Compare only like-for-like quantities and conditions.
- Diagnose the path before recommending absorption, insulation, enclosure, silencing, or vibration control.
For a room-treatment project, combine sound-level data with reverberation measurements, plans, dimensions, finishes, and source locations. The acoustic panel quantity guide explains why panel count should follow a defined room-acoustic target rather than a universal coverage percentage.
Common Decibel Mistakes
| Mistake | Correct interpretation |
|---|---|
| Treating dB as linear | 80 dB is not twice 40 dB; compare the underlying ratios. |
| Adding dB arithmetically | Two independent 70 dB sources combine to about 73 dB, not 140 dB. |
| Calling 0 dB silence | 0 dB SPL equals the reference pressure; lower levels are possible. |
| Mixing dB, dBA, and dBC | Preserve the frequency weighting and the full metric whenever a value is copied. |
| Confusing pressure and power | SPL is measured at a receiver; sound power characterizes source emission under a test method. |
| Calling +10 dB exactly twice as loud | This is only a limited perceptual approximation, not a universal law. |
| Turning NRC or αw into room dB reduction | Absorption ratings do not guarantee one receiver-level change. |
| Ignoring measurement time | A maximum and an eight-hour equivalent level answer different questions. |
| Treating common-sound charts as guarantees | Source model, operation, distance, environment, bandwidth, and meter settings change the result. |
Frequently Asked Questions
How loud is 1 dB?
One decibel describes a ratio, not a fixed sound by itself. A 1 dB increase corresponds to about 1.26× the sound power or intensity and 1.12× the sound-pressure amplitude under compatible conditions. Whether the change sounds noticeable depends on the signal, comparison method, environment, and listener.
Is 40 dB twice as loud as 20 dB?
Not in a simple physical or perceptual sense. The 20 dB difference means the 40 dB sound has 100 times the corresponding power and 10 times the pressure amplitude under compatible conditions. Perceived loudness does not follow one universal ratio, so “twice as loud” is not a reliable conclusion.
Can a human hear a 1 dB difference?
Sometimes, under controlled comparison conditions, but not always. Detectability depends on frequency, starting level, signal type, duration, listening method, background sound, and the individual. In field measurements, instrument uncertainty and changing room conditions may also make a reported 1 dB difference unsuitable as proof of an audible improvement.
What is one decibel equal to?
One decibel equals one-tenth of a bel. For a power-like quantity, 1 dB represents a ratio of approximately 1.2589:1. For an amplitude-like quantity such as sound pressure, it represents a ratio of approximately 1.1220:1 when the corresponding power is proportional to amplitude squared.
What is a decibel in simple terms?
A decibel is a logarithmic way to express a ratio. In airborne sound pressure level, it compares measured sound pressure with the 20 µPa reference. Because it is logarithmic, equal numerical steps represent equal ratios rather than equal additions of pressure or energy.
What is the difference between dB and dBA?
dB identifies the logarithmic unit, while dBA indicates that A-frequency weighting has been applied. A-weighting attenuates low and very high frequencies before producing a broadband value. For full interpretation, the result also needs a metric and time period, such as LAeq,15min.
Can acoustic panels reduce decibels?
Acoustic panels can reduce reflected sound energy, shorten reverberation, and sometimes lower the reverberant contribution to a measured room level. The result is not one universal dB value. It depends on coverage, absorption by frequency, room volume, mounting, source-receiver geometry, and existing conditions.
What information should accompany a dB value?
State the acoustic quantity, reference where required, frequency weighting, time weighting, averaging or assessment period, frequency range, measurement position, source condition, equipment, and applicable method. For a reduction claim, also provide the original level, final level, exact assembly, and comparable test conditions.
Use Decibels to Define the Problem Before Choosing the Solution
Understanding what a decibel is turns a vague noise complaint into a measurable brief. The logarithmic scale explains why levels do not add normally; sound pressure level connects pascals with dB; weighting and time descriptors explain what a meter actually reports; and frequency data reveals whether the problem is speech, low-frequency plant, reverberation, transmission, or impact.
The practical rule is to never buy a “dB solution” without defining the acoustic mechanism. Use absorptive wall or ceiling treatments for reflected-sound and reverberation control. Use tested isolation constructions, airtight detailing, resilient systems, enclosures, silencers, or vibration control when the problem follows another path.
Explore Leeyin’s acoustic products and review the matching test evidence before specification. For a project-specific assessment, contact Leeyin Acoustic with room plans, dimensions, photos, source information, existing measurements, target criteria, and the proposed construction.
Authoritative Sources
- Bureau International des Poids et Mesures — The International System of Units, 9th edition, version 4.01. Definition and writing of bel and decibel; accessed August 24, 2026.
- International Organization for Standardization — ISO 80000-8:2020, Quantities and units, Part 8: Acoustics, with Amendment 1:2025. Current status checked August 24, 2026.
- International Electrotechnical Commission — IEC 61672-1:2013, Sound level meters, Part 1: Specifications. Current publication page accessed August 24, 2026.
- International Organization for Standardization — ISO 1996-1:2016, Environmental noise, Part 1. Current edition status checked August 24, 2026.
- International Organization for Standardization — ISO 226:2023, Normal equal-loudness-level contours. Accessed August 24, 2026.
- National Institute of Standards and Technology — Guide for the Use of the International System of Units. Sound pressure reference example; accessed August 24, 2026.
- U.S. Occupational Safety and Health Administration — OSHA Technical Manual, Section III, Chapter 5. Sound-pressure, sound-power, and level-addition examples; accessed August 24, 2026.
- U.S. National Institute for Occupational Safety and Health — Understand Noise Exposure. Occupational exposure metric and measurement guidance; accessed August 24, 2026.


