**Derivation of the Net Exposure Factor**

In close-up and macro photography where a subject is magnified, relative to infinity focus there is a net loss of exposure density (defined as light intensity per unit area per unit time) at the film plane. This loss of exposure density can be expressed as a fraction of the exposure density at the film plane when the subject is focused at infinity and is defined by the following relationship:

**Net loss of exposure density = exposure density lost (magnification) x exposure density gained (close focusing) **

* (Eq 1)*

Once the net loss of exposure density is calculated, this value may in turn be easily converted into an * Exposure Factor* that can be used to compensate for the exposure density loss. Essentially, this Exposure Factor tells us how many stops of exposure compensation (typically converted into a corrected shutter speed) are needed to achieve a proper exposure of a magnified subject.

To derive the net loss of exposure density, and thus the Exposure Factor, we will apply the classic thin lens model and the time-honored Inverse Square Law.

**Thin Lens Equation**

The **Inverse Square Law**: the intensity of light (energy per unit area) emanating from a point light source is inversely proportional to the square of the distance from the light source at that point in space and time.

First, let’s derive the exposure density loss (light intensity per unit area per unit time) due to magnification (i.e., extending the lens from the film plane). Based on the Inverse Square Law, in terms of the light traveling from the lens plane a distance ** D_{i}** to reach the film plane, the intensity of light striking the film plane before (

*(Eq 2)*

where *D _{i}*

Thus, magnification is the ratio of the image height, ** H_{i}**, on the film plane to the subject height,

In this case, we are varying only the image distance (*i.e., *lens extension) to achieve magnification; the subject distances (before and after the lens is extended) will remain constant. Rearranging the equation for magnification (in terms of the image and subject distances) followed by substitution into Equation 2 gives:

* (Eq 3)*

Equation 3 represents the exposure density lost (light intensity per unit area) at the film plane due to magnification. Next, let’s derive the exposure density gained (light intensity per unit area) at the film plane due to close focusing (*i.e.*, moving the camera/lens toward the subject). Based on the Inverse Square Law, in terms of the light traveling from the subject a distance** D_{O}** to reach the lens plane, the intensity of light striking the film plane before (

*(Eq 4)*

Starting with the classic thin lens equation and applying algebraic manipulations, we eventually have:

Since we know from above that magnification is the ratio of the image distance to subject distance, we have:

Next, substituting this new relationship for** D_{O}** into Equation 4 gives:

* (Eq 5)*

Equation 5 represents the exposure density gained (light intensity per unit area) at the film plane due to close focusing (*i.e.*, decreasing the subject distance). Next, substituting both Equation 3 and Equation 5 into Equation 1, we have:

Since ** M_{2 }**>

In order to neutralize this inevitable exposure density loss at the film plane as the subject is magnified and achieve a proper exposure of the subject, this same factor (converted to a reciprocal factor) must be applied to the exposure indicated by the light meter in order to yield a corrected shutter speed. Hence, the ** Exposure Factor** correction becomes:

To derive relationships for the Exposure Factor and Magnification expressed in terms of the extension (or bellows), we start with the thin lens equation:

The expression for magnification then becomes:

By definition, in the thin lens model the image distance, ** D_{i}**, equals the focal length,

The salient feature of this expression is that magnification is directly proportional to the lens extension in use:

Intuitively, what this expression tells us is that by enabling the light to * travel farther* between the lens and the image plane, the projected image circle will enlarge, which is also a consequence of the Inverse Square Law.

In the case of a camera using solely a bellows attachment directly between the film plane and the lens, we know that when the lens is focused at *infinity*, by definition the bellows length equals the focal length. Subsequently, when the lens is extended from infinity to magnify, the bellows length is the sum of the focal length and the extension of the lens past infinity focus: ** B = EXT + f**. With additional algebra, the magnification becomes:

Expressed in terms of the bellows length, with more algebraic manipulations the Exposure Factor correction becomes:

Intuitively, what this expression tells us is that by enabling the light to * travel farther* between the lens and the image plane to form an enlarged image circle (

Thus, even a small increase in the lens extension results in a significant loss of exposure density (light intensity per unit area per unit time) at the image plane.

**Derivation of the Subject-Lens Distance Threshold for Exposure Compensation**

** Rule of thumb**: the threshold lens-subject distance at and within which exposure compensation must be applied for exposure density loss (light intensity per unit area) due to magnification corresponds to a minimum distance of nine focal lengths. If the lens-subject distance is exactly nine focal lengths, an exposure compensation of +⅓ stops of light must be applied.

A subject distance of 9 focal lengths corresponds to a magnification of:

Of course, at a subject distance of twice the focal length, the magnification will be 1:1 (100%), and the exposure compensation will be +2 stops of light.

**Derivation of the “Effective F-stop"**

By definition, the physical size of the aperture equals the ratio of the focal length to the F-stop. Let *f*1 be the focal length at infinity focus and *f*2 the "effective focal length" -- the sum of the focal length at infinity and the extension of the lens from infinity focus. Similarly, let F-stop1 be the F-stop at infinity (*i.e., *the "working F-stop") and F-stop2 be the "effective F-stop" at the point of lens extension:

In the special case of a 1:1 magnification where by definition two stops of exposure density (light intensity per unit area) are lost at the film plane, the “effective F-stop” is equal to twice the working F-stop:

Thus, a working F-stop of *f/*16 used to make an exposure at 1:1 behaves “as if” the real F-stop were *f*/32 to make the exposure, since two stops of exposure density are lost at the film plane; yet the *actual physical size of the aperture is unchanged *and the* total quantity of light exposing the film per unit time is also unchanged. *

This is a salient conceptual point: all things being equal, compared to infinity focus there is *no change in the exposure* when a subject is magnified. But, there is a loss of exposure ** density **(light intensity

In the special case of a 1:1 magnification, the same exposure at infinity focus is now spread out over an image circle that is twice in diameter and four times larger in surface area. Hence, the ¼ loss of exposure * density *at 1:1. For pedagogical purposes, this may be conceptualized as conservation of energy. For a given quantity of energy (

*The identical exposure* *at infinity focus and at 100% magnification *(i.e.,* **equivalent scene luminance, aperture, shutter speed*), *yet markedly disparate exposure densities.*

If the photographer chooses to use an “effective F-stop” to calculate Exposure Factor, then this “effective F-stop” can be used on the light meter to determine the corrected shutter speed to make the exposure.

For example, if the spot light meter gives an EV of 9.0 at *f*/16 with ISO 100 film, then the shutter speed would be ½ second. Multiplying this shutter speed by the Exposure Factor, 4x (or two stops), gives a corrected shutter speed of 2 seconds at a 1:1 magnification. Alternatively, if the photographer sets an “effective aperture” of *f*/32 on the light meter, then the corrected shutter speed is read off directly from the meter as 2 seconds.

Further, in terms of the “effective focal length”, the focal length at very close range behaves “as if” it were increased by an amount equivalent to the lens extension. That is,

For example, at 1:1 magnification a lens with a focal length of 150 mm behaves “as if” it has an actual focal length of 300 mm, since the lens must be extended by 150 mm to create a 100% magnification. Thus, since light must travel twice the distance to reach the film plane compared to infinity focus at 150 mm, the Inverse Square Law dictates that the light intensity per unit area exposing the film is reduced by ¼, or two stops of light.

Derivation of the Image Circle Diameter at 1:1

By the Inverse Square Law,

By similar triangles,

The Inverse Square Law becomes:

By definition, at 1:1 magnification the exposure density (light intensity per unit area) at the film plane is reduced by ¼. The relationship then becomes:

Thus, at 1:1 the diameter of the image circle doubles.

If the photographer prefers to work at a set “working distance” (closely approximated by the subject-lens distance) and does not wish to compromise this distance for technical or aesthetic reasons, then more magnification can be attained by simply using a lens of a *longer* focal length, provided of course, the photographer has the means to increase the lens extension. Mathematically, this is shown by the following relation:

At a fixed subject distance (working distance), the magnification can be increased with a longer focal length. But to obey the thin lens equation, the image distance, ** D_{i}** (

Alternatively, if the photographer has a limited amount of lens extension with which to work but does not care about the working distance, then increasing magnification can be achieved by using a lens of a *shorter* focal length, but this of course would involve moving the lens even closer to the subject. Mathematically, this is shown by the following relation:

At a fixed lens extension, the magnification can be increased with a shorter focal length. But to obey the thin lens equation, the subject distance, ** D_{o}** (working distance), must also be decreased.

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