grackle314
Well-known member
Light coming out of a binocular exit pupil is related to the light going into the objective. Minus the transmission losses, the light power collected through the objective is concentrated into the smaller exit pupil. The exit pupil area is approximately equal to the objective area divided by the square of the magnification. For a fixed objective area, the light from a higher magnification will be more intense at the exit pupil, in watts per square millimeter since a higher magnification has a smaller exit pupil area.
As an example, a 42 mm diameter objective will have an exit pupil diameter of 4.2 mm for a 10x magnification and 5.25 mm exit pupil diameter for an 8x . The light power output is spread over the area of the exit pupil, which is reduced compared to the objective area by the square of the magnification. Hence, for a fixed objective the light intensity power per square mm at the exit pupil is higher for the 10x compared to the 8x by the ratio of the reduction of the areas: 100 / 64. Simply put, the light goes into a smaller area for the 10x than the 8x . Keep in mind that the human eye pupil also restricts the light entering the eye, frequently this eye restriction is much smaller than the exit pupil. In typical bright daylight, most human eyes have pupils of 2 mm diameter or less. The light arriving from the binocular exit pupil which is outside the eye pupil will not enter the eye, this light is wasted for observation except that a larger exit pupil makes it easier to find the image. For the fixed objective where exit pupils are greater than the eye pupil, the greater magnification will have greater intensity entering the eye approximately by the square of the magnification ratio. One would expect for a fixed objective area with exit pupil greater than the human eye that a 10x binocular compared to an 8x in daylight will deliver approximately 100/64 = 1.56 more light per square mm to the eye pupil.
Below are the results of an experiment done with binoculars I have at hand. There are two binoculars with 10x and two with 8x, representing four manufacturers and four sizes of objectives.
For a constant input flat sheet white light source at one meter from the objective with the objective looking down a 7.5 cm diameter 1 m long tube and using a Newport optical power meter model 840, the exit pupil power was measured and the exit pupil power per square millimeter calculated.
One may see in the chart below both 10x binoculars have exit pupil output power of 0.57 to 0.58 microwatts per square millimeter and the 8x binoculars are at 0.40 microwatts per square millimeter. The 10x deliver more light per square millimeter at the exit pupil than the 8x . To compare with the 100/64 expected ratio, 0.40 microwatts per square mm x 100/64 = 0.625 microwatts per square mm which is 8% above the observed 10x power per square millimeter. This is a simple experiment and gives average power density over the exit pupil. Refinements such as radial power profile would be expected to alter the results a bit. And the human eye perception of this power is not discussed here other than to note the human eye also has a radial power detection profile.
As an example, a 42 mm diameter objective will have an exit pupil diameter of 4.2 mm for a 10x magnification and 5.25 mm exit pupil diameter for an 8x . The light power output is spread over the area of the exit pupil, which is reduced compared to the objective area by the square of the magnification. Hence, for a fixed objective the light intensity power per square mm at the exit pupil is higher for the 10x compared to the 8x by the ratio of the reduction of the areas: 100 / 64. Simply put, the light goes into a smaller area for the 10x than the 8x . Keep in mind that the human eye pupil also restricts the light entering the eye, frequently this eye restriction is much smaller than the exit pupil. In typical bright daylight, most human eyes have pupils of 2 mm diameter or less. The light arriving from the binocular exit pupil which is outside the eye pupil will not enter the eye, this light is wasted for observation except that a larger exit pupil makes it easier to find the image. For the fixed objective where exit pupils are greater than the eye pupil, the greater magnification will have greater intensity entering the eye approximately by the square of the magnification ratio. One would expect for a fixed objective area with exit pupil greater than the human eye that a 10x binocular compared to an 8x in daylight will deliver approximately 100/64 = 1.56 more light per square mm to the eye pupil.
Below are the results of an experiment done with binoculars I have at hand. There are two binoculars with 10x and two with 8x, representing four manufacturers and four sizes of objectives.
For a constant input flat sheet white light source at one meter from the objective with the objective looking down a 7.5 cm diameter 1 m long tube and using a Newport optical power meter model 840, the exit pupil power was measured and the exit pupil power per square millimeter calculated.
One may see in the chart below both 10x binoculars have exit pupil output power of 0.57 to 0.58 microwatts per square millimeter and the 8x binoculars are at 0.40 microwatts per square millimeter. The 10x deliver more light per square millimeter at the exit pupil than the 8x . To compare with the 100/64 expected ratio, 0.40 microwatts per square mm x 100/64 = 0.625 microwatts per square mm which is 8% above the observed 10x power per square millimeter. This is a simple experiment and gives average power density over the exit pupil. Refinements such as radial power profile would be expected to alter the results a bit. And the human eye perception of this power is not discussed here other than to note the human eye also has a radial power detection profile.
Binocular | M x Objective | Exit Pupil Diam. | Power out Exit Pupil (microwatts) | Microwatts per square mm |
Swaro NL Pure | 10x42 | 4.2 | 8.10 | 0.58 |
Zeiss VP | 8x25 | 3.125 | 3.10 | 0.40 |
Kowa Genesis | 10x22 | 2.2 | 2.17 | 0.57 |
Leica UVD | 8x20 | 2.5 | 1.97 | 0.40 |