What is metering?
Digital sensors, like film, require a certain amount of light to hit them before an image is recorded (or exposed). Too much light and the image is overexposed. This is sometimes referred to as ‘burnt out’ because the resultant image is too bright. Conversely, if too little light reaches the sensor or film the image is underexposed, with the result that it is too dark. As light levels are constantly changing the photographer has to use a combination of aperture, shutter speed and ISO to ensure that the correct amount of light exposes the image. The meter assists the photographer and the camera in determining the correct amount of light that should strike the sensor by calculating what the actual light level is and working out what adjustments (aperture etc.) are required to record the light without under or over exposing the image.
The complication with metering is that the meter, being part of a basic computer, cannot think. It only calculates. The photographer has to make the decision as to what to meter from and how to adjust the camera so as to correctly expose the image.
Film manufacturers (and later digital camera manufacturers) decided that on average light that exposes a piece of film should create an 18% tone of grey (In reality modern cameras actually meter for a 12-13% tone of grey – somewhat lighter than the traditional 18% grey). This is the same tone of grey that would be recorded on black and white film as green grass on a cloudless sunny day. It is also the same tone of grey that Ansel Adams chose as his zone 5. Some commentators have even argued that Adams persuaded Kodak to choose 18% grey on the basis that it was his zone 5 (I personally can’t verify this so put it down hearsay and trivia rather than fact). So the premise is basically that if the camera is adjusted to match the meter reading (i.e. aperture and shutter speed are set to what the meter regards as ‘correct’), the overall average tone of the scene being photographed should be 18% (in reality 12-13%) grey.
The problem lies in the fact that the natural world does not always present to us scenes of 18% grey. The camera, not responding to this real-world problem tries to make every scene that it photographs 18%grey in tonal value. Thus, if the scene is a brightly lit snow-scape, and therefore far lighter than 18% grey, the image becomes underexposed as the camera’s meter attempts to compensate for the brightness by making the image have a tonal value of 18% grey. Images with an overall light tone will therefore be underexposed by the cameras meter, while images with an overall dark tone will be overexposed by the cameras meter.
The complications with metering don’t only extend to situations where the overall tone is lighter or darker than 18% grey. There is also the issue of uneven tones in an image. For example, a portrait of someone with strong backlighting (the sun), or my favourite theoretical example: a white wading bird such as a Little Egret against a dark expanse of water and shadowy banks. Left to its own devices the cameras meter will meter for the dark background, attempt to reproduce it as 18% grey (lighter than it is in reality) and thereby overexpose the bird causing it to ‘burn out’. So how do we solve the problem?
Incident, Ambient and Through the Lens (TTL) Metering
First, we need to discuss the types of metering available to the modern day photographer in order to tackle the problem of the Little Egret. When we talk about metering a scene we are usually talking about calculating the reflectance value of the subject, i.e what is the intensity of light reflected off the subject towards the camera. This is known as incident metering. Prior to meters that were built into the camera, photographers used incident light meters (handheld lightmeter below right...this one known as the ‘Gossen Color Finder’) which were simple handheld devices with a selenium cell that measured light values. These light values were then applied to a simple calculator that would give the various aperture/shutter speed/ISO combinations. The problem was that the basic selenium cell was very sensitive to extremely bright situations and was also inadequate for situations where there were extreme shifts in tonal value. |