The classic potential energy curve of chemistry hides a fundamental truth: bonds mean short distances, but short distances don't mean bonds |
Every field has its set of great philosophical dilemmas. For
physics it may be the origin of the fundamental constants of nature, for
biology it might be the generation of complexity by random processes. Just like
physics and biology chemistry operates on both grand and local scales, but the
scope of its fundamental philosophical dilemmas sometimes manifests itself in
the simplest of observations.
For me the greatest philosophical dilemma in chemistry is
the following: It is the near
impossibility of doing controlled experiments on the molecular level. Other
fields also suffer from this problem, but I am constantly struck by how
directly one encounters it in chemistry.
Let me provide some background here. Much of chemistry is
about understanding the fundamental forces that operate within and between
molecules. These forces come in different flavors: strong covalent bonds (dictated by the sharing of electrons), hydrogen bonds (dictated by weak electrostatic interactions), strong charge-charge interactions (dictated by attraction between unlike charges), hydrophobic effects (dictated by the interaction between 'water-loving' and 'water-hating' parts of molecules) etc. The net interaction or repulsion between two
molecules results from the sum total of these forces, some of which may be
attractive and others might be repulsive. Harness these forces and you can
control the structure, function and properties of molecules ranging from those
used for solar capture to those used as breakthrough anticancer drugs.
Here’s how the fundamental dilemma manifests itself in the
control of all these interactions: it is next to impossible to perform
controlled experiments that would allow one to methodically vary one of the
interactions and see its effect on the overall behavior of the molecule. In a
nutshell, the interactions are all correlated, sometimes intimately so, and it
can be impossible to change one without changing the other.
The fundamental dilemma is evident in many simple
applications of chemistry. For instance, my day job involves looking at the crystal structures of proteins involved in disease and then designing small organic molecules which bind to and block such proteins. For binding to their target protein, these small molecules exploit many different interactions including hydrogen
bonds, charge-charge interactions and hydrophobic effects to bring about a net
lowering of their interaction energy with the protein. The lower this
interaction or "free energy" the better the interaction. Unfortunately, while one
can visualize the geometry of the various interactions by simply looking at the crystal structure, it is very difficult to
say anything about their energies, for to do so would entail varying an
interaction individually and looking at its effects on the net energy. Crystal
structures thus can be very misleading when it comes to making a statement
about how tightly a small molecule binds to a protein.
Let’s say I am interested in knowing how important a
particular hydrogen bond in the small molecule is. What I could
do would be to replace the atoms comprising the hydrogen bond with non hydrogen-bonding atoms and then
look at the change in the affinity of the resulting molecule for the protein, either computationally or experimentally. Unfortunately
this change also impacts other properties of the molecules; its molecular
weight, its hydrophobicity, its steric or spatial interactions with other molecules. Thus,
changing a hydrogen bonding interaction also changes other interactions, so how
can we then be sure that any change in the binding affinity came only from the loss of the hydrogen bond? The matter gets
worse when we realize that we can’t even do this experimentally; in my
colleague Peter Kenny’s words, an individual interaction between molecules such
as a hydrogen bond is not really an experimental observable. What you see in an
experiment is only the sum total, not the dissection into individual parts.
There have of course been studies on ‘model systems’ where the
number of working parts is far less than those in protein-bound small
molecules, and from these model systems we have gotten a good sense of the
energies of typical hydrogen bonds, but how reliably can we extend the results
of these systems to the particular complex system that we are studying? Some of
that extrapolation has to be a matter of faith. Also, model systems usually
provide a ranges of energies rather than a single value and we know that even a tiny change in the energy of binding can
correspond to a substantial loss of effective blocking of a protein, so the margin of error entrusted to us is slim indeed.
It is therefore very hard, if not impossible, to pin down a
change in binding affinity resulting from a single kind of interaction with any
certainty, because changing a single interaction potentially changes all
interactions; it is impossible to perform the truly controlled experiment, a concept which has been at the heart of the scientific method.
Sometimes these changes in other interactions can be tiny and we may get lucky,
but the tragedy is that we can’t even calculate with the kind of accuracy we
would like, what these tiny increments or reductions might be. The total
perturbation of a molecule’s various interactions remains a known unknown.
The roots of the problem run even deeper. At the most elemental level, all interactions between molecules are simply a function of one of the four fundamental forces known in nature - the electromagnetic force. Of the four basic forces, gravity is too weak to play a role, while the strong and weak nuclear forces don't usually apply to molecular interactions since such interactions only involve the sharing of electrons. It is the electromagnetic force that is thus ascendant in mediating every single molecular interaction in the universe. When we divide this force up into hydrogen bonds, electrostatic interactions, hydrophobic interactions etc. what we are doing is imposing an artificial division on an indivisible fundamental force, purely for our convenience. It's a bit like the parable of the blind men and the elephant - there is only one electromagnetic force, just like there is only one elephant, but each of us describing that force divides it up into multiple flavors. No wonder then that we are led astray when we think we are doing a controlled experiment, since whenever we think we are varying one flavor or another we are actually varying the same basic parameter and not its independent components. That is because there are no independent components in the true sense of the term.
The roots of the problem run even deeper. At the most elemental level, all interactions between molecules are simply a function of one of the four fundamental forces known in nature - the electromagnetic force. Of the four basic forces, gravity is too weak to play a role, while the strong and weak nuclear forces don't usually apply to molecular interactions since such interactions only involve the sharing of electrons. It is the electromagnetic force that is thus ascendant in mediating every single molecular interaction in the universe. When we divide this force up into hydrogen bonds, electrostatic interactions, hydrophobic interactions etc. what we are doing is imposing an artificial division on an indivisible fundamental force, purely for our convenience. It's a bit like the parable of the blind men and the elephant - there is only one electromagnetic force, just like there is only one elephant, but each of us describing that force divides it up into multiple flavors. No wonder then that we are led astray when we think we are doing a controlled experiment, since whenever we think we are varying one flavor or another we are actually varying the same basic parameter and not its independent components. That is because there are no independent components in the true sense of the term.
This inability to perform the truly controlled experiment is thus what I call
the great philosophical dilemma of chemistry. The dilemma not only makes the
practical estimation of individual interactions very hard but it leads to
something even more damning: the ability to even call an interaction an 'interaction' or 'bond' in the first place. This point was recently driven home to me
through an essay penned by one of the grand old men of chemistry and
crystallography – Jack Dunitz. Dunitz’s point in the essay is that we are often misled by
‘short’ distances between atoms observed in crystal structures. We ascribe these distances to
‘attractive interactions’ and even ‘bonds’ when there is little evidence that
these distances are actually attractive.
Let’s backtrack a bit to fundamentals. The idea of ascribing
a short distance to an attractive interaction comes from the classic van der
Waals potential energy curve (figure above) that is familiar to anyone who has taken a college
chemistry class. The minimum of this curve corresponds to both the shortest
distance (called the van der Waals distance) between two molecules and the
lowest energy, typically taken to signify a bond. However this leads to a false
equivalence that seems to flow both ways: van der Waals distances correspond to
bonds and bonds correspond to van der Waals distances.
In reality the connection only flows one way. Bonds do correspond to short distances but
short distances do not necessarily correspond to bonds. So then why do we
observe short distances in molecules in the first place? Again, Dunitz said it
very succinctly in a previous review: simply because ‘Atoms have to go somewhere’. The fact is that a crystal structure
is the net result of a complex symphony of attractive and repulsive
interactions, a game of energetic musical chairs if you will. At the end, when
the dust has settled everyone has to find a chair, even if it means that two
people might end up uncomfortably seated on the same chair. Thus, when you see
a short distance between two atoms in a crystal, it does not mean at all that
the interaction between them is attractive. It could simply mean that other interactions between other atoms are attractive and that those
two atoms have simply then settled where they find a place, even if the interaction
between them may be repulsive.
The message here is clear: it is folly to describe an interaction as ‘attractive’ simply because the distance is short. This applies especially to weaker interactions like those between aromatic (benzene) rings. I am always wary when I see a benzene ring from a small molecule nicely sandwiched between another benzene ring in a protein and hear the short distance between the two described as a ‘stacking interaction’. Does that mean there is actually an attractive stacking interaction between the two? Perhaps, but maybe it means simply that there was no other place for the benzene ring to be. How could I test my hypothesis? Well, I know that varying the substituents or groups of atoms attached to benzene rings is known to vary their energies of interaction with other benzene rings. So I ask the chemist to make some substituted versions of that benzene ring. But hold on! Based on the previous discussion, I just remembered that varying the substituents is not going to just change the stacking energy; it’s also going to change other qualities of the ring that mess up the other interactions in the system. It’s that problem with performing controlled experiments all over again - welcome to the fundamental dilemma of chemistry.
The message here is clear: it is folly to describe an interaction as ‘attractive’ simply because the distance is short. This applies especially to weaker interactions like those between aromatic (benzene) rings. I am always wary when I see a benzene ring from a small molecule nicely sandwiched between another benzene ring in a protein and hear the short distance between the two described as a ‘stacking interaction’. Does that mean there is actually an attractive stacking interaction between the two? Perhaps, but maybe it means simply that there was no other place for the benzene ring to be. How could I test my hypothesis? Well, I know that varying the substituents or groups of atoms attached to benzene rings is known to vary their energies of interaction with other benzene rings. So I ask the chemist to make some substituted versions of that benzene ring. But hold on! Based on the previous discussion, I just remembered that varying the substituents is not going to just change the stacking energy; it’s also going to change other qualities of the ring that mess up the other interactions in the system. It’s that problem with performing controlled experiments all over again - welcome to the fundamental dilemma of chemistry.
The fundamental dilemma is why it is so hard to understand
individual interactions in chemical systems, let alone exploit them for
scientific or commercial gain. We see it in a myriad of chemical experiments, from investigating the effects of structural changes on the rates of simple chemical reactions to investigating the effects of structural changes on the metabolism of a drug. We can’t change one component without changing
every other. There may be cases where these other changes might be
minuscule, but in reality the belief that they may be minuscule in a particular
case will always remain a matter of faith than of fact.
The fundamental dilemma then is why drug design, materials designs and every other kind of molecular design in chemistry is so tricky. It is why so much of complicated chemistry is still trial and error, why observations on one system cannot be easily extrapolated to another, and why even supercomputers are not yet able to nail down the precise balance of forces that dictate the structure and function of specific molecules. In a nutshell, the fundamental dilemma is why chemists are always ignorant and why chemistry will therefore always be endlessly fascinating.
The fundamental dilemma then is why drug design, materials designs and every other kind of molecular design in chemistry is so tricky. It is why so much of complicated chemistry is still trial and error, why observations on one system cannot be easily extrapolated to another, and why even supercomputers are not yet able to nail down the precise balance of forces that dictate the structure and function of specific molecules. In a nutshell, the fundamental dilemma is why chemists are always ignorant and why chemistry will therefore always be endlessly fascinating.