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5.4 Working with light⧉

A face beside a window can have plenty of light and still photograph badly if the eyes fall into shadow. Move the subject or the source before changing exposure. Exposure scales the measurement; lighting changes the relationships within the scene.

Describe a source by its direction, apparent size, intensity, spectrum and timing. Direction places the shadows. Apparent size controls their penumbra. Intensity sets the photon budget and the balance with other sources. Spectrum affects color, and timing determines whether a flash freezes motion or a lamp produces bands. These properties are related in practice, but none substitutes for the others.

A large source can soften a shadow without filling it. Shadow contrast also depends on light arriving from other directions and on the surroundings. A small source can be useful for revealing texture or making a crisp graphic shadow. Soft light is a useful choice for many portraits, not a requirement for a good photograph.

Move a light sideways and the shadows move; enlarge it without changing its central direction and their edges soften. These are different changes. A small frontal source can make texture difficult to see because its shadows lie behind the relief from the camera's viewpoint. Raking side light reveals the same relief with visible shadows. A large source spans a range of directions, so a point near a shadow boundary can see part of the source while another part is occluded. That partial visibility produces the penumbra. A reflector, diffuser, or softbox should therefore be judged from the subject's position: what luminous area does the subject actually see?

Highlights provide another way to inspect the source. On a glossy object, their shape depends on both the source and the material's reflection function. A small bright source can produce a concentrated highlight; a broad source can produce an extended reflection. On glassware or a polished object, moving or enlarging the source can change the visible form more than changing exposure. Lighting controls the reflected image of the environment as well as the shadows cast onto the subject.

5.4.1 Natural illumination⧉

Outdoors, separate direct sunlight from sky illumination. Direct sun is a small, directional source. The sky supplies light over a broad range of directions and fills areas hidden from the sun. A shaded face and a sunlit background therefore receive different mixtures of illumination.

Low sun changes shadow direction and often warms direct illumination because its path through the atmosphere is longer. Photographers name the windows: the golden hour after sunrise and before sunset, when low, warm sun rakes across texture, and the blue hour just after sunset, when only the sky lights the scene, evenly, cool and dim enough to want a long exposure. Clouds turn the sky into a large diffuser that lowers contrast, and haze lifts the shadows and softens distant detail. It does not substantially enlarge the solar disk. A softer overall impression can come from the balance of direct sun and sky, or from clouds and haze. Under overcast light, inspect where the brightest part of the sky lies; the illumination can still have useful direction. A doorway or overhang can remove overhead light and create stronger modeling.

Direct sun and blue sky can produce different casts within one frame. White balance chosen for one region will not necessarily neutralize the other. A reflector, a change of position or added light can simplify the mixture at capture; Chapter 24.2, Mixed-lighting white balance treats spatial correction. Correlated color temperature summarizes some illuminants, but equal color temperature does not imply equal spectra or identical rendering of skin and fabrics.

The sky simulator makes the effects of sun direction and atmospheric conditions visible. Analytic daylight models, including Preetham et al. Preetham et al. 1999 (daylight model) and Hošek and Wilkie Hošek & Wilkie 2012 (sky-dome model), provide controlled examples; a particular cloudy sky can depart from those models.

fig-color-temp-time
Figure 5.4.1. Daylight is the warm sun plus the cool sky (interactive). Daylight is really two illuminants at once. Choose the season and drag the time of day: a simple solar-geometry model sets the sun's elevation, and from it the direct sun (warm, reddening to ~2000 K and dimming near the horizon, and gone once it sets) and the sky, the cool blue skylight (~10000–13000 K) that stays all day and is the only light left in the twilight "blue hour". A bar shows the relative light each contributes: the sun dominates when high, the sky takes over near sunset, and only the sky remains after it. What a camera records is their mixture, whose correlated color temperature is the white balance it must track, swinging from very warm at the golden hour to blue at dusk. Raise the turbidity (haze) and the sky whitens, the direct sun dims and reddens, and the sky's fill grows. Common white-balance presets (tungsten, daylight, cloudy, shade) are marked on the temperature scale. The values come from a simple clear-sky model and are examples, not a universal schedule. This is why the same subject reads warm at 6 pm and blue at dusk, and why white balance exists. Interactive: set season, time of day, and turbidity, and read off the sun's and sky's color temperatures, their relative contribution, and the mixture the camera white-balances to.
fig-sky-illumination-sim
Figure 5.4.2. Natural illumination from a physical sky (interactive). A 3-D head bust and figure stand under a modeled sky dome; you set the sun's azimuth and elevation (or drive it from a clock, time of day, day of year, and latitude, with a spinning-globe inset marking the chosen parallel) and the sky's turbidity (haze), and watch the light change, hard and warm at a low sun, soft and neutral under a high or hazy sky. Under the hood the scene is lit not by the continuous dome but by its point-light approximation: the sky is sampled by many point light sources over the hemisphere, each carrying the modeled sky radiance in its own direction, so the soft, wrap-around fill you see is the sum of dozens of little lights standing in for the sky, plus one bright distant light for the sun. Turn the sun to the horizon for golden-hour raking light and long shadows; raise the turbidity and the shadows fill and soften as the sky brightens. In the printed edition this stands in as a screenshot.

5.4.2 Flash⧉

A flash delivers light over a short interval. Electronic strobes store energy in a capacitor and discharge it through a lamp; the stored energy in joules is not the emitted optical energy. Beam shape, modifiers and efficiency affect the illumination of the subject.

A guide number summarizes direct-flash reach under specified conditions:

$$\mathrm{GN}=Nd.$$

With a guide number of 40 m at ISO 100 and the stated head setting, a subject at 5 m calls for approximately f/8. Doubling distance needs two more stops of flash exposure. The estimate assumes direct illumination and the specified beam; it does not survive a bounce or softbox unchanged. Raising ISO by a factor of four doubles the nominal guide number but does not increase emitted light.

When ambient illumination contributes little, flash duration determines motion blur even if the shutter stays open longer. On many electronically quenched flashes, lowering output shortens the pulse; other flash designs have different duration curves. Compare durations under the same definition, because a short bright peak can be followed by a tail that records motion. Edgerton's photographs in Chapter 2.6, Motion blur show how controlling illumination time can reveal events that an ordinary shutter cannot resolve.

Electronic flash changed the workflow from consuming a light source to recharging one. Flash powder burned in the open; flashbulbs enclosed combustible material in a bulb used for one exposure. A capacitor-driven discharge lamp supplies a repeatable pulse whose timing and duration can be controlled. Edgerton's work made such control a photographic instrument for studying rapid events. The energy stored electrically, quoted in watt-seconds or joules, is different from the light delivered in a chosen direction.

The square-root scaling of guide number follows from the inverse-square law. Doubling flash-to-subject distance spreads the same light over four times the area. To retain the same exposure, we need four times the emitted energy in that direction or two stops more aperture area. At fixed beam shape and sensitivity, four times the flash energy doubles the guide number. Increasing ISO changes the nominal exposure setting for the same light; it does not supply that extra energy.

We can trace the measurement in photometric units. Let $Q$ be the luminous intensity integrated over the flash pulse, in candela-seconds. For a small source illuminating a normally oriented patch at distance $d$, its luminous exposure is $H_s=Q/d^2$ in lux-seconds. A Lambertian patch of reflectance $\rho$ then supplies a luminance-time integral $\rho H_s/\pi$. The lens and sensor determine how much of that light is recorded. Converting this photometric description to photons additionally requires the spectrum and spectral response; guide number alone does not uniquely determine the photon count.

5.4.3 Flash metering⧉

Through-the-lens (TTL) flash automation commonly measures a preflash and estimates the main pulse. A reflective background or a change in framing can alter that estimate. Use flash exposure compensation to adjust the result, or manual flash output for repeatable lighting when subject distance stays fixed. A handheld flash meter measures the actual illumination at a selected location.

With a short pulse wholly inside the open shutter interval, the sensor receives ambient and flash contributions:

$$H=E_a t+H_f.$$

Here $E_a$ is ambient image-plane illuminance and $H_f$ the image-plane exposure delivered by the flash at the chosen aperture. Lengthening shutter time increases the ambient contribution while leaving that captured pulse approximately unchanged. Aperture and ISO affect the rendered flash as well as the ambient. This separation lets us keep a lit subject readable while deciding how much of the room appears behind it.

A focal-plane shutter has a sync limit: above it, a traveling slit may expose only part of the sensor during one short pulse. High-speed sync extends emission over the traverse and reduces effective reach. Leaf and global shutters have different timing constraints; check the actual camera and flash combination. For daylight fill at a wide aperture, an ND filter can permit a longer time within normal sync, while also attenuating flash light.

For a backlit portrait, expose for the background detail we want to retain, then add enough flash to bring the face into the intended range. Judge the face and catchlights. A fixed “minus two stops” recipe does not describe every TTL baseline, subject distance or desired balance.

fig-shutter-sync
Figure 2.7.10 (reproduced). Focal-plane shutter and flash sync, interactive (slowed way down). Watch the first curtain open and the second curtain chase it down the sensor. Above the sync speed (set here to 1/250 s) the two curtains form a moving slit, so only part of the frame is ever uncovered at once. Press Shutter + flash: at or below sync the whole frame is open together and the single flash lights it evenly, but above sync the flash lights only the slit's band and the rest is left to the dim ambient, the partial-flash banding. Then press Shutter + HSS (high-speed sync): the flash strobes continuously across the traverse, lighting every row as it is uncovered, so the whole frame exposes evenly even above sync, at the cost of several stops of flash power. Slide the shutter speed to see where the band comes from and how HSS fills it in. The curtains sweep top to bottom over a real photo of the scene, not an abstract diagram. The diagram is for a focal-plane shutter; leaf and global shutters behave differently.

The moving slit explains the daylight-fill problem. Above a focal-plane shutter's ordinary synchronization speed, one part of the sensor is already covered while another is still being uncovered. A short flash pulse therefore illuminates only the exposed strip. High-speed sync extends illumination across the curtains' travel, usually with a pulse train, so successive strips receive light. Much of that emitted light arrives while any particular strip is covered, reducing effective output.

For example, a wide aperture chosen for shallow depth of field in bright daylight can require a shutter speed above normal sync. High-speed sync preserves that aperture choice but costs flash range. A neutral-density filter can permit a slower shutter, but it attenuates the flash as well as ambient light. Leaf-shutter systems have different synchronization behavior; their supported speeds and the flash duration still need to be checked.

Flash metering has used two different measurement times. Some film cameras measured light reflected from the film during the exposure, terminating the flash once the integrated reading reached a target. The Olympus OM-2 history describes its direct off-the-film metering. The measurement used the actual taking path, but still depended on how the photographed subject reflected the light.

A preflash instead supplies a measurement before the main exposure. The camera estimates the main pulse from that return, possibly using scene regions and focus information. The subject can move or blink between the measurement and the capture, and a changed framing can alter the metered return. Manual output is useful when the setup is fixed because it removes that per-shot estimate. It does not remove the need to recheck exposure when subject distance or a modifier changes.

5.4.4 Indirect illumination and bounce flash⧉

Direct on-camera flash can produce a small-source shadow and a strong frontal reflection, which may be exactly the desired appearance. For softer directional light, bounce off a suitable wall or ceiling. The illuminated area becomes the source seen by the subject. Its location, apparent size, color and distance matter; a distant dark ceiling can consume most of the available flash energy.

A small diffusion cap on a flash does little to enlarge the apparent source outdoors. Indoors it may spread light onto walls that then become larger sources. A softbox or scrim works through the illuminated area visible from the subject, so bringing it closer generally increases its angular size.

A white reflector redirects available light into shadows. A silver surface is more directional, and a colored surface tints the reflected illumination. A black panel removes fill. Move the panel while watching the face before adding another lamp.

Red-eye is more likely when the source lies close to the viewing axis and the pupil is large. Moving the flash away from the lens axis or changing the lighting geometry can reduce the return from the eye. Software can alter its appearance afterward, but it does not change the lighting recorded on the rest of the face. The geometry is a retroreflection: an on-camera flash a centimeter or two from the lens sends light through the pupil, the retina and the blood-rich choroid behind it return it red, and it comes back along nearly the same line into the lens. Moving the source off axis throws that return cone clear of the lens, and a pre-flash that contracts the pupil shrinks it. Many animals show green or white eyeshine instead, from the reflective tapetum behind their retinas (Chapter 3.6, Animal eyes).

fig-bounce-flash-sim
Figure 5.4.3. Try it yourself (web edition). A live bounce-flash simulator. A face sits in a small room, with a flash just above the camera. Aim the flash with the presets or the two angle sliders: point it straight at the face for the harsh, flat, hard-shadowed look of a bare flash, or bounce it off the white ceiling or a colored wall so that whole surface becomes a big soft light that wraps the face (a colored wall also tints the light). The left panel is the photograph; the right panel renders the same scene from a wider angle so you can see how the flash fills the room, softening as the bounce surface grows. Color controls let you gel the flash, switch the white balance, and add a warm ceiling light. The bounce is computed live so the soft light and its shadows are physically consistent. In the printed edition this stands in as a screenshot.
fig-reflector-sim
Figure 5.4.4. The reflector: bouncing the sun (interactive). A face is lit by the sun, a single hard, parallel source that keys one cheek and drops the other into shadow. A photographer's assistant holds a large white reflector to the side: it catches the sun and throws it back as a big, soft second source that fills the shadow without adding a lamp of its own. This is global illumination put to work, the fill light is the sun arriving by way of one bounce. Drag the assistant around the subject (azimuth) and in or out (distance) and watch the fill soften and shift; the right view shows the whole setup, sun, reflector, assistant, and camera, from any angle. A gold reflector warms the fill and a silver one is brighter, and the same physics runs a flash bounced off a wall or a studio umbrella. The 3D assistant is generated with Meshy AI.

5.4.5 Multiple-point lighting⧉

Start with one source and decide where its shadow should fall. Add fill if that shadow is too dark for the intended picture. Add a rim or background light only if separation needs it. A good setup can contain one light; the names describe functions, not a minimum equipment list.

In a key-plus-fill setup, specify what a quoted lighting ratio compares. The ratio of lamp outputs is not the ratio of illumination on the two sides of a face: the bright side can receive both key and fill, and reflected light arrives from the room. Measure or inspect the subject under the combined illumination.

The portrait simulator lets us move the key and vary its extent while retaining the same face. Compare the shadow edge, eye sockets and specular highlights separately. “Butterfly,” “Rembrandt” and “split” are useful names for recurring shadow patterns, but a light placement should serve this person's face and the photograph's purpose.

fig-portrait-lighting-sim
Figure 5.4.5. Try it yourself (web edition). A live portrait-lighting simulator: three soft area lights, a key, a fill, and a kicker, each with its own direction (azimuth, elevation), size, intensity, and color, sculpt a 3D face, with area-light-supersampled soft shadows and a physiologically grounded melanin/hemoglobin skin model. A second "from behind" view shows the lights as studio umbrellas plus the camera so you can read the whole setup, and one-click presets (butterfly, loop, Rembrandt, split, clamshell, rim) let you feel how a light's placement and size, not brightness, shape a face. In the printed edition this stands in as a screenshot. The 3D studio umbrella is generated with Meshy AI.

The lighting names identify jobs:

LightJob
KeyEstablishes the main direction and shadows
FillSupplies light to shadows left by the key
Rim, kicker, or hair lightProduces an edge or highlight that can separate subject and background
BackgroundSets the backdrop independently of incidental spill

Three-point lighting combines key, fill, and rim. It is a common arrangement, not a minimum requirement. A reflector can do the fill's job without a second powered source. Separating the jobs makes adjustment easier: a brighter background need not require a brighter face.

Portrait-pattern names describe shadows on the face. Butterfly lighting places a small nose shadow below the nose; loop lighting moves that shadow sideways; Rembrandt lighting produces a lit triangle on the shadowed cheek; split lighting divides the face more strongly into lit and shadowed halves. Clamshell lighting combines a source above with fill below. The exact placement depends on the face, pose, and source size. Use the name to describe the observed pattern rather than treating a fixed angle as a recipe.