Chapter 1
On the Internal Environment of Animal Cells
James S. Clegg
Tables of Contents
I. Introduction
II. Thin Section Electron Microscopy and Cell Fractionation
III. Are the Aqueous Compartments Concentrated Solutions?
A. The Devaux Effect
B. Cell Stratification
C. The Reference Phase Technique
D. Section Summary
IV. High Voltage Electron Microscopy
V. Water and Micromolecules in the Aqueous Compartments
A. Micromolecules
B. Intracellular Water.
C. Intracellular Interfaces
1. Surface Area
2. The Influence of Surfaces on Adjacent Water.
3. Significance to Compartmentation
VI. On the Concept of âLevels of Biological Organizationâ
Acknowledgments
References
I. Introduction
Compartmentation is one of the most pervasive features of biological systems,1 so it should come as no surprise to observe it within cells. A question much more difficult to answer, and therefore more interesting, concerns the extent to which it occurs. Friedrich1 has referred to âmicrocompartmentationâ as metabolite sequestration by coupled enzymes in which the dimensions of the compartment take on those of the metabolite plus surrounding boundaries of the participating enzymes. The other authors in this book will, no doubt, offer their own views of that term, but I will use it as given above because it allows some interesting consequences to emerge, transcending the metabolic context within which the phenomenon is usually discussed.
That microcompartmentation exists is beyond doubt, and the abundant evidence for it will unfold in this book, as it has in others.2-5 However, we should ask, how widespread is its occurrence within the cell? It seems worthwhile to consider that question against a backdrop of the broader question of the nature of intracellular organization. That is my major task in this chapter. Because the approach taken here will be more global than the usual detailed description of the bits and pieces of cells, it may take on a vitalistic air which, however, I hope to avoid by select choice of good experimental evidence. Therefore, what follows should in no way be considered to be a âreviewâ of the literature. In fact, it comes closer to being a review of reviews.
I will begin by considering results obtained from two powerful and very widely used techniques, confessing at the outset that I think we may have been deceived by what they have revealed.
II. Thin Section Electron Microscopy and Cell Fractionation
What has the use of these methods told us about the eukaryotic cell? Figure 1 shows a typical result obtained from thin section electron microscopy (TS-EM). Many of us were raised on these images, and they are so familiar that they stir little interest per se. Moreover, it is clear that TS-EM has been invaluable in our attempts to understand cell structure, but consider that they reveal only about 25% of the mass and volume that actually exist in an intact living cell. Understandably, cell biology has concentrated on what can be seen, and that has been profitable, but is it not also important to ask about the remainder â the vast majority? What is it actually like in all those "empty spaces" that are not revealed by TSEM? For convenience, we can refer to the latter as reflections of the existence of what I will call the aqueous compartments, the "soluble phases" of the nucleus, cytoplasmic membrane-bounded organelles, and the intervening aqueous cytoplasmic space, often called "cytosol", a term with several meanings.5 It is widely appreciated that TS-EM tells us nothing about these compartments, since they are washed away during the preparative procedures. Thus, we will stop here for the moment and turn to cell fractionation.
Table 1 illustrates what happens typically when cells are disrupted in a "suitable" buffer. These particular data are taken from the work of Lahav et al.,6 but literally thousands of similar studies would reveal a similar outcome; a very large proportion of the cellâs proteins (and other macromolecules) are released, remaining in solution when the homogenate is centrifuged at very high speeds. This result has led to the tempting possibility that these materials were also soluble when in the intact cell. Indeed, many seem to have yielded to temptation: that interpretation has, with some caution at times, been widely applied. While few would argue that cell fractionation provides quantitative, unambiguous evidence for the actual intracellular location of a given molecule, I believe it is fair to say that the "soluble phases" from cell fractionation are commonly perceived to be an approximation of reality. Setting that dubious assumption aside for the moment, let us return to the images from TSEM (Figure 1).
Figure 1. Transmission electron photomicrograph of a thin section of a mouse L-929 cell (A) at an original magnification of Ă 13,500. An enlarged area of the cytoplasm (original magnification Ă 48,500) is shown in (B). Details of preparation are given in reference 30. Provided by Murali Pillai.
It is easy to understand how the "blank spaces" in the images from TS-EM have been translated into the "soluble phases" of cell fractionation, and vice versa. That interpretation generates the impression that a relatively sharp boundary exists between the ultrastructure we can see, and the surrounding "structureless solution", which is presumably composed of a crowded collection of macromolecules, metabolites, inorganicions, and, of course, water. Moreover, much of the metabolic activity of cells is assigned to that location, since the soluble phase contains many enzymes. The question of prime importance is whether evidence from methods other than TS-EM and cell fractionation support that generally accepted paradigm.
Table 1 Protein and DNA Contents of Subcellular Fractions of Rat Liver Cellsa
| Total homogenate (%) |
Fraction | Protein | DNA |
Nuclei | 12 | 91 |
Mitochondria | 14 | 6 |
Mixed (2,4) | 8 | 4 |
Microsomes | 15 | 0 |
Soluble | 56 | 0 |
In the remainder of this article I will refer to evidence from a variety of sources and cell-types that should, in my view, compel us to discard that widely held conception of the organization and function of the eukaryotic cell. I believe that impression is not only incorrect, but also misleading, because it deludes us into believing that we know something about cells that we actually do not. Having accepted the burden of proof, it now becomes necessary to sample the evidence, and "sample" is the correct term.
III. Are the Aqueous Compartments Concentrated Solutions?
I believe the answer is no, and we have had reason to suspect that for at least half a century. Let us examine one early example, the work done by Chambers and Kopac in the late 1930s and reviewed by Chambers in 1940.7 They introduced oil droplets into echinoderm eggs and observed their behavior. Their 48-year-old results and interpretations are still revealing.
A. The Devaux Effect
Chambers and Kopac observed that droplets of various kinds of oil would spontaneously coalesce with the eggs, entering the cytoplasm. Alternatively, the droplets were injected, with similar results; if the cytoplasm was not injured, the oil drops remained perfectly spherical. However, if the cytoplasm was intentionally damaged, the droplet would then undergo a surface crinkling, known as the "Devaux effect". It was pointed out that this crinkling occurs when proteins in solution are absorbed at an oil-water interface at monolayer coverage concentrations.
Kopac and Chambers proposed reasonably that the absence of the Devaux effect in undamaged cells reflected the absence of significant concentrations of diffusible proteins of the size that would absorb onto the droplets. Moreover, Kopac devised a way to evaluate protein absorption on the droplets. That was accomplished by the "drop retraction" method in which an introduced droplet, retained by the injecting micropipette, was partially withdrawn back into the pipette. He reasoned that if some protein had been absorbed, but less than a monolayer, then the Devaux effect would, in principle, suddenly occur when the volume of the droplet was reduced to the critical level. Kopac calculated that an oil droplet 10 Îźm in diameter, of 3.14 Ă 10-6 cm-2 surface area, would require only about 3 Ă 10-6Îźg of pr...