FMVSS 108 headlamp photometry is a laboratory measurement of the light a lamp throws 100 feet onto a calibrated detector, checked point by point against candela limits published in Table XVIII for the upper beam and Table XIX for the lower beam. A lamp that passes has been measured under a defined procedure; a lamp that carries the letters DOT has only been certified by its manufacturer. Those are two different claims, and the difference explains most of the confusion around “DOT approved” headlights sold online.
The tables are not a brightness contest. They are a set of floors that keep enough light on the road and a set of ceilings that keep light out of other drivers’ eyes, and the ceilings are where most of the engineering lives. A lower beam can put 15,000 candela or more into the road ahead and still be failed for about 136 candela in a zone above the horizontal on the left, because that zone is where an oncoming driver’s face is. This article walks through the test as it is actually performed: the bench, the distance, the aiming step, the point list, the glare caps, and the parts of the regulation that the tables do not contain.
FMVSS 108 headlamp photometry is performed at a test distance of 100 feet (about 30.48 m) with the lamp on a goniometer, aimed to a defined reference, and measured with a photometer whose calibration traces to a national standard. The measured quantity is luminous intensity in candela at named angular positions such as H-V, 4.0U-8.0L or 2.0D-9.0R, where H and V are the horizontal and vertical reference lines and U, D, L and R mean up, down, left and right in degrees. The lower beam must stay under 125 candela anywhere in the zone from 10 degrees up to 90 degrees up, and under much tighter caps in the few degrees just above the cut-off on the left. The upper beam must reach at least 40,000 candela at H-V and must not exceed 75,000 candela there. A pass therefore means the beam’s shape and its spill were measured at those points on that day; it does not mean the lamp is legal on every road, and it does not mean the beam is pleasant to drive behind.
Federal Motor Vehicle Safety Standard No. 108 sits in the United States Code of Federal Regulations at 49 CFR 571.108. Its scope sentence is short: the standard “specifies requirements for original and replacement lamps, reflective devices, and associated equipment.” Its purpose sentence is the useful one, because it names both halves of the job: reducing crashes “by providing adequate illumination of the roadway, and by enhancing the conspicuity of motor vehicles on the public roads.”
Application is defined by vehicle type rather than by product category. The standard applies to passenger cars, multipurpose passenger vehicles, trucks, buses, trailers other than pole trailers and trailer converter dollies, and motorcycles, and separately to replacement equipment for those vehicles. That last clause is what makes the regulation reach into the aftermarket: a replacement headlamp sold for a vehicle the standard already covers is inside the scope, and it is expected to meet the same photometry as the part it replaces.
The standard is administered by the National Highway Traffic Safety Administration and enforced through self-certification, not through a government type-approval stamp. The regulation requires the lens of each original and replacement headlamp, and of each beam contributor, to be marked with the symbol “DOT” to indicate certification under 49 U.S.C. 30115. The mark is a manufacturer’s statement. Nothing in the rule has a government engineer measuring your particular lamp before it ships.
| Clause | Subject | Why a buyer or engineer cares |
|---|---|---|
| S1, S2, S3 | Scope, purpose, application | Defines which vehicles and replacement parts are covered |
| S4 | Definitions | Fixes the meaning of cut-off, H-V axis, axis of reference, aiming plane |
| S6.2.1 | Impairment | Forbids adding equipment that degrades required lighting |
| S6.5.1 | DOT marking | The mark is a certification, not an approval |
| S10.13.3, S10.14.6, S10.15.6 | Headlamp photometry | Points sealed beam, integral beam and replaceable bulb systems at Table XVIII and Table XIX via the S14.2.5 procedure |
| S10.18.7 to S10.18.9 | Aimability | Sets how the lamp is aimed, and how a visually/optically aimable lamp is judged |
| S14.2.5 | Photometric test procedure | The procedure that converts the tables into a measurement |
Luminous flux in lumens describes how much light leaves a source in all directions. Luminous intensity in candela describes how much of it leaves in a particular direction, per steradian. A headlamp is a device whose entire job is direction, so the regulation measures direction.
That choice has a consequence that surprises people who compare spec sheets. A lamp’s lumen figure can rise while its beam gets worse, because flux pushed into the wrong part of the pattern still counts as flux. FMVSS 108 headlamp photometry ignores the total and asks a narrower question at each point: how many candela are leaving in this direction, and is that number above the floor or below the ceiling for this direction.
The definitions in S4 carry the precision. “Axis of reference” is the characteristic axis of the lamp, used as the direction of reference at H = 0 degrees and V = 0 degrees for angles of field in photometric measurement. “H-V axis” is the line from the centre of the principal filament to the intersection of the horizontal and vertical lines of the test screen. “Cutoff” is defined as “a generally horizontal, visual/optical aiming cue in the lower beam that marks a separation between areas of higher and lower luminance” — a cue, not a geometric line, which is why the aiming test later needs a gradient criterion rather than a ruler.
The measurement itself excludes a small neighbourhood. “Effective light-emitting surface” is defined as the portion of the lamp that directs light to the photometric test pattern, excluding transparent lenses, mounting bosses, reflector area, beads and rims “that may glow or produce small areas of increased intensity as a result of uncontrolled light from an area of 1/2 degree radius around a test point.” In plain terms, a bright speck a quarter of a degree wide does not count as beam.
A compliance test is a dark room, a rigid stand and a lot of geometry. The lamp is mounted in a fixture that reproduces how it sits on the vehicle, the fixture is carried on a goniometer that rotates the lamp in known increments, and a photometer looks back at the lamp from a fixed distance. Rotating the lamp is equivalent to moving the detector around a sphere, which is what makes a two-axis point list like “2.0D-9.0R” meaningful.
The published NHTSA compliance reports show what the equipment list looks like in practice. In the 2018 test of a 2012 Nissan Leaf left-hand combination headlamp, report 108-CAN-18-013, the laboratory recorded a test distance of 100 feet, a reference detector control number of NIST P181-2, a custom goniometer with stepper motors at 0.001 degree resolution and plus or minus 0.01 degree accuracy, and a luminous intensity photometer covering 0.1 candela to 600 kilocandela with plus or minus 2.0 percent accuracy. The 2019 test of a 2018 Subaru Impreza left-hand replaceable-bulb headlamp, report 108-CAN-19-002, records the same 100-foot distance and the same NIST reference detector number.
Two details in that list matter more than they look. The 0.001 degree goniometer resolution is what allows a cut-off gradient to be measured at all, because the gradient criterion lives inside a couple of degrees. The NIST-traceable detector and the stated accuracy are what make the numbers comparable between laboratories; a lamp measured with an uncalibrated sensor is not doing photometry, it is doing photography.

One hundred feet is 30.48 metres, and that number sets the angular scale of everything else. At 30.48 m, one degree of rotation moves the projected spot by 30.48 times the tangent of one degree, which is about 0.53 m. Two degrees is about 1.06 m, four degrees about 2.13 m, and ten degrees about 5.37 m. Those are the distances between the rows of the point grid on a real screen.
| Angle | Offset at 100 ft (30.48 m) | What sits there in a lower beam |
|---|---|---|
| 0.5 degree | about 0.27 m | First cap above the cut-off, 1,000 cd in the left zone |
| 1.0 degree | about 0.53 m | Tightest cap above the cut-off, 700 cd in the left zone |
| 1.5 degree | about 0.80 m | 1,400 cd cap in the right-hand band |
| 2.0 degree | about 1.06 m | Nominal aim point for a visually aimed lamp, H/2.0R |
| 4.0 degree | about 2.13 m | Downward floor of 300 cd and a 12,500 cd ceiling |
| 10.0 degree | about 5.37 m | Start of the glare zone, 125 cd maximum to 90 degrees up |
The distance also explains why the regulation measures intensity rather than illuminance. Candela is defined at the source, so a lamp’s candela at a point does not change with the distance of the test. Illuminance does: at 30 m a beam producing 20,000 candela delivers about 22 lux on a surface facing it, and at 100 m the same beam delivers about 2 lux, by the inverse-square relation E = I / d squared. Testing at 100 feet keeps the detector signal large enough to be measured accurately while remaining far enough away for the far-field pattern to be representative. Both of those are engineering reasons for the distance, not quotations from the rule.
The cost of the distance is that the test is a far-field measurement of a small solid angle. It does not tell you what the beam looks like on a road that curves and undulates, and it cannot, because the road is not in the room.
Photometry only means something once the lamp is aimed. The regulation separates lamps that are aimed mechanically, using three pads on the lens that form an aiming plane, from lamps that are aimed visually or optically, and it names the second group in the definitions: a “visually/optically aimable headlamp” is one designed to be aimed in accordance with S10.18.9. The lens carries a mark for this. In both NHTSA reports reviewed here, the laboratory verified under S10.18.9.6 that the lens was marked “VOR” in letters not less than 3 mm high, and under S10.18.5 that the lens carried an optical axis mark.
The aiming procedure used in both reports is stated in one sentence each: the aim hardware was adjusted until the lower beam maximum, Gmax, sat at H/2.0R and the beam was level from H/1.0R to H/3.0R. Everything measured afterwards is measured from that aim. Move the lamp half a degree and every number in the table changes.
That is why the aiming section of a compliance report is not boilerplate. It is the reference frame. It is also why the practical advice in our auxiliary light aiming and glare guide starts with the lamp and the vehicle rather than with a wall: an unaimed lamp has no photometry, only brightness.
The upper beam table is a set of floors with two ceilings. The floors rise toward the centre of the pattern and fall away at the edges, which is the shape of a beam designed to put light far down the road without wasting it in the sky. The ceilings do two jobs: they cap the centre of the beam, and they cap the bottom of the pattern so the beam does not over-light the ground immediately in front of the vehicle.
The numbers below are the limits recorded by the laboratory in the two NHTSA reports for a two-lamp upper beam system, UB2, measured against Table XVIII. They are reproduced as the reports give them, in candela.
| Test point | Limit type | Limit (cd) | What it constrains |
|---|---|---|---|
| 2.0U V | minimum | 1,500 | Light thrown high, used for overhead signs and crests |
| 1.0U 3.0L | minimum | 5,000 | Upper-left quadrant of the beam |
| 1.0U 3.0R | minimum | 5,000 | Upper-right quadrant of the beam |
| H 12.0L | minimum | 1,500 | Far left edge at the horizon |
| H 9.0L | minimum | 3,000 | Left shoulder |
| H 6.0L | minimum | 5,000 | Left of centre |
| H 3.0L | minimum | 15,000 | Near-centre left |
| H V | minimum | 40,000 | Beam centre |
| H V | maximum | 75,000 | Beam centre |
| H 3.0R | minimum | 15,000 | Near-centre right |
| H 6.0R | minimum | 5,000 | Right of centre |
| H 9.0R | minimum | 3,000 | Right shoulder |
| H 12.0R | minimum | 1,500 | Far right edge at the horizon |
| 1.5D 9.0L | minimum | 2,000 | Lower left |
| 1.5D V | minimum | 5,000 | Below centre |
| 1.5D 9.0R | minimum | 2,000 | Lower right |
| 2.5D 12.0L | minimum | 1,000 | Low left edge |
| 2.5D V | minimum | 2,500 | Low centre |
| 2.5D 12.0R | minimum | 1,000 | Low right edge |
| 4.0D V | maximum | 12,000 | Ground close to the vehicle |
Two readings of this table are worth keeping. First, the 40,000 to 75,000 candela window at H-V is a window, not a target: a lamp at 76,000 candela fails the standard even though it is brighter. Second, the minimum at H-12.0L and H-12.0R is 1,500 candela, which is more than ten times the 125 candela glare cap in the lower beam. The upper beam is allowed to be bright in other drivers’ eyes; it is simply not allowed to be on when they are there.
The lower beam table looks like the upper beam table until you read the location column closely. Several rows are not points at all. They are bands, and the regulation’s demand is that the limit hold anywhere inside the band. The laboratory therefore has to scan each band and record the worst location it finds, which is why two samples of the same part number can report the same limit at different locations.
The limits below are the ones recorded in the two NHTSA reports for a two-lamp visually aimed lower beam, LB2V, against Table XIX-a.
| Band or point | Limit type | Limit (cd) | Note from the reports |
|---|---|---|---|
| 4.0U 8.0L | minimum | 64 | Above the cut-off, far left |
| 4.0U 8.0R | minimum | 64 | Above the cut-off, far right |
| 2.0U 4.0L | minimum | 135 | Above the cut-off, left |
| 1.5U, 1.0R to R | minimum | 200 | Band; the report records where it was measured |
| 1.5U, 1.0R to R | maximum | 1,400 | Same band, ceiling |
| 1.0U, 1.5L to L | maximum | 700 | Tightest ceiling in the beam |
| 0.5U, 1.5L to L | maximum | 1,000 | One step looser |
| 0.5U, 1.0R to 3.0R | minimum | 500 | Floor just above the cut-off |
| 0.5U, 1.0R to 3.0R | maximum | 2,700 | Ceiling on the same band |
| H 8.0L | minimum | 64 | Horizon, far left |
| H 4.0L | minimum | 135 | Horizon, left |
| H V | no limit listed | none | Centre of the lower beam is uncapped in this table |
| 0.6D 1.3R | minimum | 10,000 | The aiming region |
| 0.9D 3.5L | minimum | 1,800 | Left, below the horizon |
| 0.9D 3.5L | maximum | 12,000 | Same point, ceiling |
| 0.9D V | minimum | 4,500 | Centre, below the horizon |
| 1.5D 2.0R | minimum | 15,000 | Where Gmax is expected |
| 2.0D 15.0L | minimum | 1,000 | Wide left |
| 2.0D 9.0L | minimum | 1,250 | Left |
| 2.0D 9.0R | minimum | 1,250 | Right |
| 2.0D 15.0R | minimum | 1,000 | Wide right |
| 4.0D 20.0L | minimum | 300 | Far left near the vehicle |
| 4.0D 4.0R | maximum | 12,500 | Foreground ceiling |
| 4.0D 20.0R | minimum | 300 | Far right near the vehicle |
| 10.0U to 90.0U, 90L to 90R | maximum | 125 | The glare zone |
The structure is the argument. Going up from the horizontal on the left, the ceiling drops from 2,700 candela in a band that starts just above the cut-off, to 1,000 candela, to 700 candela, and then the zone above 10 degrees up is capped at 125 candela across the entire remaining sky. Going down below the horizontal, floors rise to 15,000 candela where the beam is supposed to be strongest and then fall away to 300 candela at 4 degrees down and 20 degrees out.
That 700 candela ceiling deserves a sentence of arithmetic. At 100 metres, 700 candela produces 700 divided by 100 squared, or 0.07 lux, on a surface facing the lamp. The tightest glare limit in the American lower beam standard is a fraction of a lux at highway distance. It is not there to make the beam dim; it is there to stop a small excess from becoming an annoyance at 100 metres and a complaint at 30.
The last row of the lower beam table is the one that catches modified lamps. It is not a point and it is not a band in one direction. It covers the whole field from 10 degrees up to 90 degrees up and from 90 degrees left to 90 degrees right, and the maximum permitted luminous intensity anywhere in that field is 125 candela.
In both reports the laboratory records this as a single scanned result with the location of the worst value: “MX(10U-90U/90L-90R)”, followed by the point where the maximum was found. For one Leaf sample the worst value was 25.04 candela at 10.0U-3.7R, comfortably inside the cap. For one Impreza sample the worst value was 135.83 candela at 10.0U-7.3R, and the report marks it as a failure.
Two lessons follow, and they are the practical core of this article. A lamp can be failed for 136 candela, which is roughly one three-hundredth of the light at its own beam centre. And the failure location, 10 degrees up and 7.3 degrees right, is exactly where a lifted or poorly aimed lamp puts its spill.

Nothing in Table XIX describes the shape of the cut-off. The table constrains levels above and below it, but a lamp could satisfy every point and still have a soft, ragged edge that produces glare between the rows. The regulation handles that separately, in the aimability requirements of S10.18, and the NHTSA reports show how the check is recorded.
For a visually/optically aimable lamp the laboratory measures a maximum vertical gradient and compares it with a required value greater than 0.13, confirms that the horizontal width of the cut-off is greater than 2 degrees centred at 2.0R, and confirms that the maximum inclination of the cut-off is within plus or minus 0.2 degrees. At the H/1.0R position the four Leaf samples recorded 0.304, 0.305, 0.310 and 0.241, and the four Impreza samples recorded 0.202, 0.227, 0.205 and 0.192. All eight clear the 0.13 floor, and the lowest of them clears it by less than half.
| Aimability check | Criterion recorded in the reports | What it protects against |
|---|---|---|
| Maximum vertical gradient | greater than 0.13 | A cut-off so soft that spill above the line is uncontrolled |
| Horizontal width of cut-off | greater than 2 degrees, centred at 2.0R | A cut-off so short that it does not cover the lane |
| Maximum inclination of cut-off | within plus or minus 0.2 degrees | A tilted cut-off that dips into the road or rises into traffic |
A gradient of 0.13 is a weak floor by the standards of a good projector beam, and the samples here clear it easily. The criterion’s purpose is not to reward a sharp edge; it is to refuse a beam that has no edge at all.
A lamp measured cold is not the lamp a driver gets. The regulation anticipates this in its definitions: “seasoning” is the process of energizing the filament of a headlamp at design voltage for a period equal to 1 percent of design life, or another equivalent method. The reports apply the idea to LEDs as well, and they state the stabilisation criterion explicitly.
In the Leaf report the lower beam LEDs reached 1 percent stability within 30 minutes of activation, with the measurement taken after a 60-minute warm-up at 12.80 V and 1.677 A. The same report notes that the tabulated values can be multiplied by 1.12 to obtain the one-minute values, which is a compact way of saying that a cold LED beam is brighter than a warm one by about 12 percent. The Impreza report records seasoned H11 bulbs at 12.80 V and 4.561 A, and a separate HB3 at 12.80 V and 5.118 A for the upper beam.
| Measurement condition | Leaf lower beam | Impreza lower beam | Why it is recorded |
|---|---|---|---|
| Voltage at the lamp | 12.80 V | 12.80 V | Candela scales with voltage; the number is meaningless without it |
| Current | 1.677 A | 4.561 A | Confirms the lamp is drawing what the design expects |
| Stabilisation | 1 percent, within 30 minutes | Seasoned source | Removes the cold-bright effect |
| Warm-up before reading | 60 minutes | Seasoned bulb | Makes samples comparable |
| Cold-to-warm factor | multiply by 1.12 for one-minute values | not stated | Shows how much a cold reading overstates output |
This is the part of the test that aftermarket claims most often skip. A seller who quotes a candela figure without a voltage, a warm-up time and a stabilisation criterion has quoted a number that cannot be compared with anything, including the regulation.
Photometry says how much light leaves in a direction. It says nothing about what colour that light is. The colour requirement is tested separately under S14.4.1, and the reports record the chromaticity coordinates at a named target: 1.5D/2.0R for the lower beam, H-V for the upper beam and the signal functions.
For white light the box recorded in both reports is 0.31 to 0.50 in x, 0.38 to 0.44 in y, with y greater than or equal to 0.75x plus 0.05 and y less than or equal to 0.64x plus 0.15. The Leaf lower beam measured x = 0.3307 and y = 0.3488 at one minute; the Impreza lower beam measured x = 0.4283 and y = 0.4021. Both passed, and both sit in visibly different parts of the white region, which is a reminder that “white” in a regulation is an area rather than a point.
The 3,000 K versus 6,000 K argument is an aesthetic argument inside that area. Colour temperature preferences are covered in our LED light bar colour temperature guide, and none of it changes the photometry.
The most useful thing about a public compliance report is that it shows the test failing. The 2019 Impreza report records that two of four lower beam samples failed photometry, that all four failed side reflex reflector photometry, and that every other listed test passed. The failures are specific and small in absolute terms.
| Sample | Failure | Measured (cd) | Limit (cd) |
|---|---|---|---|
| LH1 | 1.0U, 1.5L to L band | 879.48 | 700 maximum |
| LH1 | 0.5U, 1.5L to L band | 1,368.98 | 1,000 maximum |
| LH1 | Glare zone above 10U | 135.83 | 125 maximum |
| LH4 | 1.0U, 1.5L to L band | 957.57 | 700 maximum |
| LH4 | 0.5U, 1.5L to L band | 1,539.52 | 1,000 maximum |
| LH4 | 4.0D 20.0R | 288.85 | 300 minimum |
Read the direction of those numbers. The failures are not a lamp that is too dim. They are a lamp that puts between 879 and 1,540 candela where the standard allows 700 and 1,000, in a band one to one and a half degrees above the horizontal on the left. Everything else in that beam, including 15,000 candela floors and 40,000 candela centres, was met.
That is the shape of a real photometry failure: a beam that is broadly correct and locally generous in exactly the direction that reaches other drivers. It is also the reason a “DOT” lens mark and a passing report are not the same claim. The mark says the manufacturer certified the design; the report says a laboratory measured these four samples on these two days.
Passing is a floor, not a compliment. Three gaps between the tables and the road are worth naming.
The first is between the rows. The lower beam caps are applied in named bands, and a lamp can sit just under every cap while filling the gaps between them. The gradient criterion narrows that gap but does not close it, because a gradient of 0.14 passes.
The second is between the samples and the fleet. A compliance test measures a handful of lamps, often purchased retail, and the reports here use four. Production spread in reflector alignment, LED binning and lens moulding is real, and a design that passes at the nominal centre of its tolerance can drift at the edges. Our article on white LED colour binning describes the same mechanism in colour rather than intensity.
The third is between the bench and the vehicle. The lamp is measured on a fixture at a defined aim, at 12.80 V, in a dark room. On the vehicle it is aimed by a technician or by a self-levelling system, it runs at whatever the alternator or DC-DC converter supplies, and it is loaded by passengers, fuel and trailer tongue weight. None of those variables is in Table XVIII or Table XIX.
The European system asks a different question in a different geometry, and the difference is easiest to see in how aim is expressed. American photometry is written in degrees from the H-V axis, measured at 100 feet. The European-type dipped beam is described in a percentage dip, and the British MOT inspection manual states the acceptance bands that a tester applies.
| Feature | FMVSS 108 lower beam | European-type dipped beam as inspected in the UK |
|---|---|---|
| Aim reference | Degrees from H-V, e.g. Gmax at H/2.0R | Percentage dip of the horizontal cut-off |
| Aim tolerance, lamp centre 850 mm or less | Fixed nominal aim plus aimability criteria | Cut-off between the 0.5 percent and 2.75 percent lines |
| Aim tolerance, lamp centre above 850 mm | Not expressed this way | Cut-off between the 1.25 percent and 2.75 percent lines |
| Beam shape | Generally horizontal cut-off, gradient criterion | Horizontal cut-off on the right with a wedge of light, the kick-up, to the left |
| Above the cut-off | Floors of 64 to 200 cd and a 125 cd sky cap | White light must not show in the zone formed by the 0 percent vertical and 0.5 percent horizontal lines |
| Assessment | Type test of photometry plus self-certification | Periodic inspection of aim plus approval markings |
The percentage figures convert to angles by the tangent: 0.5 percent is about 0.29 degrees, 1.25 percent about 0.72 degrees, and 2.75 percent about 1.57 degrees. So the British inspection band for a lamp below 850 mm is roughly a quarter of a degree to one and a half degrees of dip. That is a narrow window, and it explains why the MOT treats incorrect aim as a major defect rather than an advisory.

The kick-up is the other structural difference. A European-type beam deliberately raises light to the near side to illuminate signs and the verge, and the geometry of that raise is what the percent bands are checking. The American table reaches the same objective through point floors at 4.0U and 2.0U above the horizontal on the left and right, which allows light up there but caps it hard. Two philosophies, both aimed at the same trade: see the verge, do not blind the oncoming lane.
The regulatory numbers in this comparison come from different documents, and the European side here is the inspection practice described in the MOT manual rather than the type-approval text of a United Nations regulation. The underlying UN regulation numbers are widely cited, but the photometric tables of those regulations were not retrieved for this article, so no clause numbers or limits from them appear here.
A passing report proves four things. The lamp was measured at a stated distance with a traceable photometer. It was aimed to a stated reference before measurement. Its intensity at a defined list of points and zones fell inside the floors and ceilings. Its cut-off met the gradient, width and inclination criteria.
It does not prove that the lamp is legal to use on a road, because road-use rules are a separate body of law and in the United States they are largely state law. It does not prove that the lamp is legal to sell as a replacement part for a specific vehicle, because that depends on the part being a replacement of like equipment. It does not prove that the beam is comfortable, because comfort is not measured. And it does not prove that a particular unit in a particular box was measured, because self-certification is a design-level statement.
The distinction matters most for replacement light sources. A replaceable light source is defined in S4 as an assembly of capsule, base and terminals designed to conform to appendix A or appendix B of 49 CFR part 564, and the headlamp lens must be marked with the bulb designation in front of each replaceable light source under S6.5.3.4.1. An LED bulb dropped into a halogen housing has no such relationship with the housing unless the combination was designed and tested together. Our article on DOT versus E-Mark markings covers how to read the marks themselves; the point here is narrower: the mark on the lens belongs to the lamp assembly, not to the bulb inside it.
FMVSS 108 does not contain a photometry table for a roof light bar. It contains a prohibition. S6.2.1 states that no additional lamp, reflective device or other motor vehicle equipment is permitted to be installed that impairs the effectiveness of lighting equipment required by the standard. S6.2.3.1 adds that headlamps, when activated in the steady burning state, must not have any styling ornament or other feature, such as a translucent cover or grille, in front of the lens.
So the compliance question for an auxiliary lamp is not “which table does it meet”. It is “does it degrade a required function”. A bar mounted across the grille in front of the headlamps does. A pod on a bumper that leaves the headlamp beam unobstructed and is switched separately does not, on the face of the rule. Whether it may be used on a public road while moving is a different question again, answered by state law and summarised in our article on whether LED light bars are street legal.
| Auxiliary product type | Photometry table in FMVSS 108 | Governing question instead |
|---|---|---|
| Roof or bumper light bar | None | Does it obstruct or impair a required lamp (S6.2.1)? |
| Grille-mounted bar covering part of the headlamp | None | S6.2.3.1 forbids features in front of the headlamp lens |
| Work lamp on a vehicle or machine | None | Not a required function; road-use rules decide |
| Replacement headlamp assembly | Table XVIII and Table XIX | Must meet the same photometry as the part it replaces |
| Replaceable light source | Part 564 appendices, plus the housing’s own approval | The housing and source must be a tested combination |
Nothing about an auxiliary lamp makes the headlamp test irrelevant. A bar strong enough to matter is also strong enough to ruin the aim of everything around it if it is mounted badly, which is why the interesting engineering in a product like the Jungle Series 40 inch bar is the bracket and the beam shape rather than the lumen number on the box. For a catalogue view of the shapes available, the LED light bars category and the LED work lights category show the two ends of that range.
The regulation’s newest headlamp concept is the adaptive driving beam, defined in S4 as a long-range beam “which automatically modifies portions of the projected light to reduce glare to traffic participants on an ongoing, dynamic basis.” Its requirements are written as a modification of the same two tables, which is why it belongs in a photometry article.
Inside an area of unreduced intensity, the beam must meet Table XVIII. Inside an area of reduced intensity, it must meet Table XIX. Between the two, a transition zone is permitted, and S9.4.1.6.4.5 caps it: the transition zone may not exceed 1.0 degree in either the horizontal or the vertical direction, and although the table requirements do not apply inside it, the maximum at H-V from Table XVIII may not be exceeded at any point in it. Below 32 km/h (20 mph) the system must provide only lower beams unless the driver overrides it.
That 1.0 degree cap is the photometric expression of a control problem. A system that dims a patch around an oncoming car has to do it within one degree, or the transition itself becomes a moving glare source.
Most lighting listings publish a lumen figure, a colour temperature and a photograph of a wall. A photometry claim worth trusting answers different questions. Ask these in order, and treat a missing answer as a missing test.
| Question | A good answer looks like | Why it matters |
|---|---|---|
| At what distance and with what instrument was this measured? | A stated distance, a calibrated photometer, a traceable reference | Candela without a bench description cannot be checked |
| Was the lamp aimed, and to what reference? | e.g. Gmax at H/2.0R, level from H/1.0R to H/3.0R | Unaimed numbers describe a different lamp |
| At what voltage and after what warm-up? | e.g. 12.80 V after 60 minutes, 1 percent stability | Cold readings overstate output |
| Is the figure a point value or a zone maximum? | The named point or band | A zone maximum is a different, harder claim |
| Which table was it tested against, and which system type? | e.g. Table XIX-a, LB2V | Limits differ by system and aim method |
| What was the highest reading above 10 degrees up? | A number under 125 cd for a lower beam | This is the glare number that matters |
| Which sample failed, and what did it measure? | Any honest discussion of spread | Four samples passing is not a distribution |
A supplier who can answer the first three has done photometry. A supplier who can answer all seven has done the test and read the report.
Several beliefs about FMVSS 108 headlamp photometry are widespread and wrong in ways that change buying decisions.
| Misreading | What the documents actually say |
|---|---|
| “DOT approved” | The lens is marked DOT as the manufacturer’s certification under 49 U.S.C. 30115; there is no approval step |
| Brighter is more compliant | The upper beam has a 75,000 cd ceiling at H-V and the lower beam has a 700 cd ceiling in its tightest band |
| Passing means legal on the road | Road use is governed separately, largely by state law in the United States |
| Any DOT-marked bulb makes a DOT headlamp | The lens and the light source are separate items, and the housing is approved with a specified source |
| The test measures lux on a wall | It measures candela at named angles, with the lamp on a goniometer |
| A 125 cd glare cap is trivial | It is roughly one three-hundredth of beam centre and it fails real samples |
| Auxiliary lamps need their own table | The regulation constrains them through the impairment rule instead |
| A passing report covers production | It covers the samples measured, on those days, at that voltage |
The last row is the one to keep. Four samples passing is evidence, not a guarantee, and the Impreza report shows what happens when two of four do not.
There are three situations where a photometry measurement is the only honest answer. The first is designing a lamp: you cannot iterate a reflector or a projector without a goniometer. The second is defending a product claim: a candela figure at a named point, with a distance, a voltage and a warm-up stated, is defensible in a way that a lumen figure is not. The third is diagnosing a pattern problem that no amount of aiming fixes, such as a hot spot above the cut-off that appears only on one side of a production run.
What to ask for is narrow. Ask for the point list, the limits, the measured values and the pass or fail per point. Ask for the aiming statement. Ask for the voltage and the stabilisation criterion. Ask which table and which system type. A report that gives all four can be checked against the regulation by anyone with the text; a report that gives a single “max candela” number cannot.
What not to expect is a road verdict. A laboratory can tell you that a beam puts 690 candela one degree above the horizontal on the left. It cannot tell you whether the driver in front of you finds it annoying, because that depends on mirror geometry, following distance and the fact that the other driver’s mirrors are not at 100 feet on a goniometer.
The two NHTSA compliance reports examined for this article both record a test distance of 100 feet, which is about 30.48 metres, and both cite the same NIST reference detector number, P181-2. The distance is recorded on the photometry summary sheet of each report.
For the two-lamp visually aimed lower beam, LB2V, the point list recorded in the reports runs to about two dozen rows, and several of those rows are bands rather than points, so the number of individual measurements is larger than the row count. Each band must satisfy its limit anywhere inside it.
For the lower beam the field from 10 degrees up to 90 degrees up, across 90 degrees left to 90 degrees right, is capped at 125 candela. Closer to the cut-off the caps are tighter in places: 700 candela in the 1.0U left band and 1,000 candela in the 0.5U left band.
Yes, in two places. The upper beam has a maximum of 75,000 candela at H-V, and the lower beam has zone maxima including 12,500 candela at 4.0D-4.0R and 12,000 candela at 0.9D-3.5L. A lamp above those numbers fails even though nothing about it is dim.
No. The mark is a certification by the manufacturer under 49 U.S.C. 30115. Testing is how a manufacturer establishes the basis for that certification, and public compliance reports exist because NHTSA also tests samples independently, but the mark itself is a statement rather than a test certificate.
Because the tables constrain intensity at named angles and the cut-off’s gradient, not the whole continuous field, and because the lamp on the vehicle is aimed, loaded and powered differently from the fixture in the laboratory. A lamp at the edge of every limit can pass and still be unpleasant.
Not automatically. A replaceable light source is defined by reference to 49 CFR part 564, and the lens is marked with the bulb designation it was designed for under S6.5.3.4.1. An LED source that is not the designated type for that housing has no tested relationship with it.
It checks that the cut-off has a measurable edge. The laboratory records a maximum vertical gradient and compares it with a required value greater than 0.13, along with a cut-off width greater than 2 degrees centred at 2.0R and an inclination within plus or minus 0.2 degrees.
No. American photometry is written as candela at points in degrees from H-V at a 100-foot distance. The European-type dipped beam is inspected as a percentage dip of the horizontal cut-off, with bands such as 0.5 percent to 2.75 percent for lamps mounted at 850 mm or less, plus a kick-up to the near side.
For a lower beam, the highest reading above 10 degrees up. It is the number that decides whether the lamp is a glare problem, it has a hard cap of 125 candela, and it is the number most often missing from marketing material.
SAEC Lighting Engineering Team, Foshan
Last updated: 2026-10-18
This article describes the photometric requirements of Federal Motor Vehicle Safety Standard No. 108 as they appear in the retrieved text of 49 CFR 571.108 and in two published NHTSA compliance test reports. It is an engineering explanation, not legal advice, and it is not a statement that any particular product meets or does not meet the standard.