Photo System Engineering II, B&W negative films

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Photo Engineer

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In this part of our discussion we will look at the design of a B&W negative film. Again, it will be done with language as plain as possible with little technical jargon, but I have made some assumptions regarding the reader’s knowledge of science. I have also simplified much of this for ease of understanding.

The various processes described here can be modeled by computer programs either forward or backward. That is, you can start with the film characteristics and get the required emulsion type or you can start with the emulsion type and get the film design from the characteristics and etc. This model gives the photo engineer a center point for the start of factorial experiments which will lead to the final product. The desired characteristics include toe, shoulder, slope (contrast or gamma), speed (ISO rating), grain and sharpness.

Using the discussion from the last Photo Engineering thread, we know we need a negative film material with an average mid scale gamma (contrast) or slope (change in density / change in exposure) of about 0.6 so lets use that as our average.

Normally, emulsions come in two types. One type is monodisperse (modern style) and the other is polydisperse (early style). Monodisperse means that all of the crystals are the same type and have the same size (approximately) and polydisperse means that all of the crystals have different shapes and sizes. It can be shown (and also be reasoned out logically) that a polydisperse emulsion will have a lower contrast than a monodispersed emulsion. The argument goes thusly: since every grain in a polydisperse emulsion differs, the response of each grain to light varies and gives a different speed for a given exposure. This type of curve is very often bowed due to having some types of grain predominate and therefore this skews the response to light based on a measure called size / frequency distribution. The actual curve may bow upward or downward depending on this size / frequency distribution. This type of emulsion was the only type that could be made in the early years of photographic product manufacturing. It resulted from the making of Single Run (SR) emulsions where Silver Nitrate solution was run into salt and gelatin. Since the salt content varied due to the formation of a precipitate, the type of grain varied from the start of the run until the finish of the run. It is characteristic of many films from the 30s, 40s and 50s. A single emulsion could be tailored to give almost the curve desired, but with sacrifices in mid scale contrast in one way or another. Often, the result was a film with no clear shoulder or a very soft toe.

BTW, for those mathematicians out there, all emulsions, when measured by counting the size of a grain and the frequency they occur in the actual emulsion make up “Size Frequency Curves”. These curves follow a Gaussian distribution in most cases which is a traditional bell shaped curve. The narrower the curve, the more monodisperse it is and the broader this curve, the more polydisperse. Contrast is related to the width of this curve.

These polydisperse emulsions predominate in most all textbooks up through the first half of the 20th century, particularly those of Wall and those of Baker.

In the attached electron micrographs, the first picture on the left is a polydisperse emulsion with many grain sizes and shapes. It has an inherently low contrast. The middle photomicrograph is a monodisperse emulsion with an octahedral crystalline form. The right photomicrograph shows a cubic emulsion with expitaxy. This exotic emulsion has been first formed as a monodisperse cube and then decorated with the 'ears' on each corner. For more detail see Mees and James, or Haist.

In the 50s and onward, Run Salt (RS) emulsions became the norm and resulted in very straight line curves but high contrast. These emulsions were made by running Silver Nitrate and a separate salt solution into a solution of salt and gelatin. Since the resultant mixture stayed at the same approximate salt concentration from start to finish, the grains were very similar in size and shape. The emulsions made this way were monodisperse. All grains in a monodisperse emulsion reacted pretty much the same to light due to their similarity. The problem was that these emulsions had latitudes that were too short for negative films due to this high contrast. It was found though that by blending such emulsions into one mix and coating them, the result was finer in grain and sharper with a very straight mid scale curve, a sharp toe and a sharp shoulder. In effect, you mixed a fast, medium and slow component. To get an ISO 400 film, the mid scale would be where the correct exposure would be placed and this would be made of an ISO 400 emulsion. The toe would be made up of an ISO 800 emulsion, and the shoulder would be made up of an ISO 200 emulsion. In effect, the starting emulsions coated at silver levels sufficient to achieve a contrast of 1.8 and a Dmax of 3.0 would be coated at 1/3 of the silver level each such that the final silver level of the 3 part blend would be sufficient to achieve a density of 3.0, but the contrasts of each component would be 1/3 the value, and so the result would be a contrast of 0.6, the desired value. This is due to the fact that an emulsion with a contrast of 1.8 and Dmax of 3.0 at say 3000 mg / square meter would have a Dmax of 1.0 if coated at 1000 mg / square meter. The contrast would be about 0.6. Thus the blend of 3 emulsions would result in a film that is the sum of 3 emulsions but with each component coated at 1/3 the level needed to achieve the desired Dmax.

In actual practice, it was found that absorber dyes increased sharpness by reducing internal reflections off of grains. Therefore, in the example above, one might actually use ISO 1600, 800 and 400 emulsions to achieve a mid range of 400. This final, hypothetical film would have much increased sharpness. In fact, at one time, two Kodak products were the same film, but the High Acutance 100 film was merely the 200 film with 1 stop equivalent of acutance dye in it to improve sharpness dramatically. It had the grain of the 200 speed film though.

Design problems cropped up in both early and new type emulsions.

The old type emulsions often were difficult to repeat in terms of curve shape, so the bumps and humps and bows varied from batch to batch. But, the new emulsions did not entirely solve the problem. If the emulsions varied by even a tiny amount in speed or contrast, then a set of 2 bumps arose in the characteristic curve of the film where each emulsion component overlapped. In both types of emulsions (old and new), if the different grains had different makeup such as iodide content, then the grains could equilibrate during keeping in some fashion and this could lead to changes during the life of the film resulting in poor keeping. In the new monodispersed emulsions, it was found that mixing grains with the same composition and placement of chemicals was more optimum, and therefore the modern emulsions kept better.

It can be shown that faster films have higher grain. This is simply due to the cross section of the crystal. The larger the crystal, the more likely it is to catch a photon of light. But there is a tradeoff. The old triangle of characteristics of photographic materials bites us here. That triangle is speed-grain-sharpness. You can have any two of these, but not all 3 from a given film formula. Most often, you only get one of these. So, if you go up in speed, grain gets worse and sharpness may or may not change. Usually though it gets worse. You can increase the level of silver halide that you coat, and sharpness gets a little better up to a point and then turbidity rears its ugly head and you begin to lose speed and sharpness due to internal reflections. Then you must add the acutance dyes, but this causes another speed loss. So you see, a film designer is in a vicious cycle here that can only be resolved by making many coatings of the emulsion(s) with different levels of silver and addenda to optimize speed and grain.

The only way out of this cycle is to find a method by which a given grain size can be kept as is, and the speed of an emulsion can be increased by some other method. This is what is called a speed grain improvement. You get more speed out of a fixed grain size. That is next on the agenda.
 

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Kirk Keyes

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In the 50s and onward, Run Salt (RS) emulsions became the norm and resulted in very straight line curves but high contrast. These emulsions were made by running Silver Nitrate and a separate salt solution into a solution of salt and gelatin. Since the resultant mixture stayed at the same approximate salt concentration from start to finish, the grains were very similar in size and shape. The emulsions made this way were monodisperse. QUOTE]

Do you have a RS formula we could try out?

I assume the silver and halide solutions should be made to the same molar concentration for this? How much excess halide should be with the gelatin? The excess halide is there to make sure there is never an excess of silver in the pot, right?

Kirk
 
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Kirk;

I posted one here a few months back.

However, the run salt and silver are always the same molar concentration.

A general rule is that if you want to go from an SR emulsion to an RS emulsion, you remove from the kettle the amount of salt equivalent to silver. The remainder stays in the kettle with the gelatin. Then, the salt removed from the kettle is made up to the same molar concentration as the silver and they are run into the salt + gelatin at the same molar rate.

This is a starting point, not a formula.

PE
 

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Excellent, thanks PE.
 

Kirk Keyes

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OK - so for a iodide emulsion, we would want to take all of the iodide out of the gelatin mixture and put it into the RS solution for the halide? Or since the iodide is going to immediately precipitate out regardless of where it is, can we leave it in the pot with the gelatin?

Also, if we say, a formula (like something from Baker, 2nd Ed, p 82, converted to KBr) that has in solution A:
Water - 50 ml
Gelatin - 2.5 g
KBr - 8.0 g
KI - 0.1 g

and a solution B:
AgNO3 - 5.2 g
Water - 5 ml
NH4OH (28%) - about 6 ml, as needed.

This give us about 0.0305 mole Ag+, and 0.0672 mole Br- and 6.02-4 mole I-, which is about 2% Iodide in relation to the Silver.

To convert this to a RS formula, we would need to have 0.0367 (0.0672-0.0305=0.0367) moles Br in the pot with the Gelatin, or about 4.37 g KBr, and 3.36 g KBr in the solution that will be added alongside the Silver solution.

For those that don't have the equipment to do additions of 2 different solutions at once, what about adding as large of an excess of KBr to the gelatin solution to make sure there is a large excess of Br floating around? What affect would this have? I know there will be practical issues like the solubility of the KBr in solution with the mix. It looks like KBr has a maximum solubility in water at 20C of about 40%, so for 50 ml of water you could get at most 20g KBr. That increases the concentration of Br in solution relative to the silver being added and will help with the changing concentration somewhat...

I suppose the KBr dropping out of solution when you chill set the emulsion would be a bad thing though...

Using ammonium bromide would allow us more solubility of the bromide and thus allow us to add more bromide, but then that means we need to not dissolve the silver nitrate with ammonia as we don't want too much ammonia during ripening, correct?

Finally, the amount of water used to make Solution A would need to be decreased as you want to control the ultimate amount of water at the end of emulsification. This then increases the concentration of the gelatin in the pot, which also has an effect on the size of the silver halide crystals during emulsification...

OK - not as simple as it seems.
 
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Kirk;

Actually, if you want a uniform bromide addition, then the halide solution added to the pot along with silver should be 0.0367 moles and the total volume should be identical to the volume of part B. If you want a combined bromo-iodide addition, then the total moles of halide should be 0.0367 and either the iodide should go into the kettle, or it should be mixed with the bromide being added with the silver, or it can be added 50/50 in the kettle and the salt solution as long as the total salt used in all parts remains at 0.0672 and total iodide remains at 2% and the total moles of halide being added with the silver is 0.0367 with a volume equal to part B.

Does that make sense to you?

Oh, BTW, since the MWs of AgNO3 and KI are almost identical, you can divide the weight of KI / wt AgNO3 and come up with almost the exact iodide content. Hope this hint helps too. It is close enough for starting calculations and often good enough for final work.

PE
 
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Now, as for practicality, since Potassium Nitrate is forming during precipitation, this changes the ionic strength and therefore the actual concentration and flow rate of the salt have to be adjusted to account for this very real change that is taking place. Usually, the salt is about 5% - 10% more concentrated and the salt flow rate is slightly lower than the silver rate to start, and ramps up ever so slightly so that the overall ionic strength change is compensated for. Go figure that one out.

Have fun with Nernst and Debye Huckle this evening.

PE
 

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PE,

You wrote in your article:

…, if the different grains had different makeup such as iodide content, then the grains could equilibrate during keeping in some fashion….

What do you mean by “equilibrate”, and how could that happen in a set gelatin?

And could you point out more detailed what the difference would be between blending several different emulsions into one and coating them onto each other?
 
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In a set emulsion some grains are in contact with others before and after coating. There is also salt present. If a 10% iodide grain is adjacent to a 1% iodide grain, there can be a tiny exchange of ion in the moist emulsion which leads to a tiny change.

Coating emulsions in one vs two layers increases internal reflections and also the cost of coating.

PE
 

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Coating emulsions in one vs two layers increases internal reflections...

I don't see why “internal reflections” would be an issue – assuming that you'd have coated the two layers with the same type of gelatin (and hence with the same refractive index).
 
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More internal reflections reduce sharpness, a single thicker emulsion will have a higher number of internal reflections. If you use two different layers of emulsion, you can tailor them to contribute different qualities to the final emulsion, much like modern films. It's more complicated than just the gelatin being the same, there is the Ag content, Iodide concentration, etc. Gelatin is not a solid, if it can absorb chemicals (think developer, fixer) then the chemicals in it can move around as well. Since the older films have varied sizes of grains, chemical action will try to find an equilibrium of distribution (like a drop of ink in an aquarium of water). Newer films have grains sizes that are much more even, hence they are already close to equilibrium, and will change less over time.

Now, did I get that right?
 
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Yes, you did. I just want to add that a single thicker emulsion will have more internal refelctions, but two layers often act as if they have a huge partially reflective mirror between them. So it is a tossup as to which works better. The fast component is usually coated first, then the medium, with the slow one on top if it is done. Usually, B&W films are done in single layers, and color films are done in mulitilayers.

PE
 

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Thanks, projectbluebird and PE for the clarification.
I may have been a bit too much into ultra-fine grain (Lippmann) emulsions - grain size < 30nm - which are completely transparent. Assuming two layers of the same type (same gelatin and same AgX concentration), you wouldn't see any internal reflections. One practical application might be coating a blue-green sensitive layer on top of a red sensitive layer. By the way thickness differences between the two layers wouldn't matter since the refractive index is the same.
 
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Interestingly, a grain has to be absorbant to light at the wavelength needed, in order to have imaging take place, so the grain is not 100% transparent. In fact it cannot be. So, if you were to observe holographic emulsions at the wavelength being used, the emulsion must have some absorption, even if it is UV or IR.

PE
 
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Another factor in this design is the need for identical reciprocity in the 3 components used. If they don't have the same response to HIRF or LIRF then the characteristic curve pulls apart and bumps appear or contrast changes strangely. In addition, the latent image keeping of all 3 emulsions must be the same or you get similar bad things taking place.

PE
 

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Interestingly, a grain has to be absorbant to light at the wavelength needed, in order to have imaging take place, so the grain is not 100% transparent. In fact it cannot be. So, if you were to observe holographic emulsions at the wavelength being used, the emulsion must have some absorption, even if it is UV or IR.

PE

Yes, obviously some degree of (visible light) absorption must take place. I am not sure about the AgX crystals, things can get incredibly complicated with grains substantially smaller than the recording wavelength (Raleigh, Mie scattering)!
I guess the main part of (red-green) light absorption is due to the sensitizing dye. But this is barely noticeable. A coating with 10nm grains, 7um thickness, looks completely transparent to the naked eye. And even at the 633nm recording wavelength there's no absorption measurable (at least not with a common lab power meter). By the way the low light absorption is key to the recording of simple reflection (Denisyuk) holograms: the recording light enters the emulsion and hits the object behind the recording plate. There, it will be reflected, part of it will reenter the emulsion and interfere with the incoming light – making the holographic recording. The more object light reaching the recording plate in that scheme, the better the condition for high diffraction efficiency of the hologram.
 
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Some exitation of something must take place, and that is due to absorption of light. Sensitzing dyes, if present, can absorb a lot of light and that is why they can increase the speed in their primary region of absorption. The layer is thin, the emulsion is small and the energy is very high. This allows the coating to be essentially invisible to the human eye.

PE
 

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Layer thickness aside, the main reason for the “invisibility” undoubtedly is the extremely small grain size. Let's not forget, if you develop this kind of emulsion with a physical or colloidal developer you'll get beautiful yellow filters that absorb light from UV - blue. Looking through such a layer at a point light source, you will notice no haze.
There's practically no absorption at any visible wavelength. For example even at the 633nm recording wavelength for a red sensitive emulsion overall absorption is extremely low – though there must be high absorption on each light hit (spectrally sensitized) AgX crystal.
By the way, the energy levels we're dealing with, are pretty weak most of the time. A great many people are doing their exposures with lasers of a few Milliwatts of power only.
 
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You are taking a Lippmann emulsion (the tiny AgX crystals) and converting them into Carey Lea silver. This is what usually happens when reducing agent is added to a Lippmann emulsion and you can do it to form red, green or blue silver or gray silver. The anti halation layer in film is made by such a process to form gray colloidal silver in gelatin from fine silver halide.

PE
 
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