One common criticism of modern Physics (i.e., Relativity and Quantum Mechanics) is that it is counter-intuitive. This is not unexpected: our evolutionary history in no way requires that we have an innate understanding of the mechanisms underpinning the Universe at all scales. That said, this criticism is not uniquely limited to modern Physics. In this post I explore concepts that we often take for granted today, and how those could have seemed counter-intuitive to people of earlier times.
Pythagoras' theorem
Or, more generally, 'Applicability of mathematical laws to the Universe'.
Every kindergartener is intimately familiar with Pythagoras' theorem that equates the square of the length of the hypotenuse of a right triangle to the sum of the squares of the length of its two other sides. This theorem was proved - using principles of logic, induction, etc. - by Euclid in Elements, Book 6, Proposition 31. (It was already known to be 'true', in various guises, for at least a millennia preceding Euclid.) Over time we have accumulated multiple proofs for this theorem and newer proofs continue to be discovered.
All extant proofs of Pythagoras' theorem ultimately rest on the 'truth' of Euclid's postulates which, in turn, rely on the implicit definitions of point, line, plane etc. none of which have any counterparts in the physical world. These latter concepts reside solely in the platonic world of Geometry and have only very approximate, if that, representations in the real world. Ergo, there is no intuitive reason why Pythagoras' theorem should hold for right triangles drawn on, say, a flat surface. If it does, the only way to build certainty is via experience. Historically, many cultures had determined to their satisfaction that Pythagoras' theorem did hold in practice within the limits of measurement accuracy they could bring to bear on it. (This hasn't changed in the modern world with fancier tools and precision.) Nevertheless, why this should be the case in the first place remains a mystery and is certainly not intuitive.
This very consideration also holds for other mathematical laws which appear to (unreasonably) govern the evolution of the Universe. A fuller discussion is in Wigner's "The Unreasonable Effectiveness of Mathematics in the Natural Sciences".
Galilean relativity
I consider both concepts discussed under this section as the pinnacle of pre-Newtonian physics. Galileo's investigations into the motion of bodies and the insights he developed as a result mark a turning point in physics: from a more common sense model of how the world works to one that seemingly defied common sense but was, nevertheless, demonstrably closer to truth.
The upshot of this section is that the laws of motion are the same for all inertial frames of reference.
Inertia
Or, 'Moving things keep moving'.
Kindergarteners first learn the concept of inertia when they imbibe Newton's first law of motion. However, it was Galileo who originally deduced this intrinsic property of a material body by rolling down balls on ramps. (His experiments and the deductions he used makes for an amazing narrative. But that's for another time.)
Simply put, Galileo's law of inertia states that a body set into motion continues to move at a constant speed in a straight line until an external (unbalanced) force acts on it. This also applies to bodies at rest as a special case of moving bodies (i.e., speed = 0).
Surely, this is counter-intuitive! Every day experience objects to this law. However, to our credit, we can rationalise away any objections by noting that it is drag (air resistance, friction, etc.) that slows down moving objects. Most people nowadays have no qualms extrapolating this rationalisation to the limiting case when all drag vanishes - even though this condition is not something we can achieve in practice. Nevertheless, the law of inertia is in no way an intuitive construct borne out of everyday experience.
Space is relative
Or, 'No privileged frames of reference'.
Galileo used the example of a person cloistered inside a 'smoothly moving' boat (i.e., one moving at a constant speed in a straight line, without turbulence or jerks) to argue that the laws of motion are the same in all inertial frames. (That's how we'd state it in modern lingo.) In other words, no inertial observer is privileged in the universe and all inertial frames can lay an equal claim to be 'at rest' and thus qualify as 'reference frames'. Put another way, there is no absolute rest frame in the universe. Space is relative to the (inertial) observer.
In the modern world many of us have had the good fortune of travelling in planes at cruising altitude at which point every passenger is completely oblivious to the fact that the plane has a high speed relative to the ground (unless, they look out of the window). We've also seen astronauts & objects in the International Space Station freely floating with respect to each other - apparently stationary - even though we all know that the ISS is in orbit around the Earth. (It would take Einstein's insight to reveal that a stable orbit around a gravitating body is effectively in 'free fall' and equivalent to an inertial frame of Galilean physics.)
Even so many have a hard time internalising the idea that all inertial frames are equivalent. There is an intuitive need to imagine an 'absolute background' of space - a stage - on which all events occur. Such a background would implicitly define an absolute frame of rest - one that cannot be experienced or revealed by any experiment (involving motions of bodies) according to Galileo.
Sidebar: (Newton's) Absolute space
There is no prohibition in Galilean relativity against the existence of an absolute space. In Galilean relativity, if absolute space exists (and it would be inertial, by definition), it is no more privileged than any other inertial observer moving with respect to it. In other words, absolute space is not experiential and no motion with respect to absolute space can be detected. Newton fully accepted these conclusions from Galilean relativity. He nevertheless postulated an abstract mathematical absolute space as a construction that existed without reference to anything external. In Newton's mind, the relative spaces of all inertial observers existed in this absolute space even though no experiment could detect the latter. A fuller discussion of Newton's views regarding the absolute nature of space (and time) are in DiSalle's "Absolute space and Newton's theory of relativity" (DOI: 10.1016/j.shpsb.2020.04.003).
Note that Newton's laws of motion do not need absolute space. In fact, Newton's laws are invariant under a Galilean transformation (i.e., changing from one inertial frame to another). Only accelerations are absolute.
(Newton's) Absolute time
Or, 'Newton's universal time'.
Kindergarteners get indoctrinated into the cult of absolute time even as they complete a course of study in Newtonian physics. Newton himself listed absolute time as a fundamental assumption in his Principia Mathematica. To quote once again the oft-quoted passage:
Absolute, true, and mathematical time, from its own nature, passes equably without relation to anything external, and thus without reference to any change or way of measuring of time (e.g., the hour, day, month, or year).
However, it's certainly not obvious that people across cultures and eras had an intuitive notion of absolute time. For instance, ancient Indian literature is replete with accounts that entertained the notion of relative time. To take just one example, in the legend of the temple of Jagannath Puri (ref. Skanda Purana), king Indradyumna visits Brahmalok for a day. When he returns to Puri he realises, to his shock, that a full manvantara has passed and that everyone he ever knew or loved has long since died. Granted that such stories relate to time passing differently between realms. Nevertheless, it is worth noting that the possibility of differential passing of time was definitely not alien to earlier minds.
Thus, one cannot rule out the possibility that the notion of absolute time could have seemed counter-intuitive to many people at the dawn of Newtonian mechanics. (Debates surrounding the ontological nature of time date back to millennia - certainly preceding Newton. As an aside, Gottfried Wilhelm Leibniz and George Berkeley - contemporaries of Newton - advocated a relational nature of both space and time.)
Of course, in the modern world, armed with Special Relativity, and certainly with General Relativity, we all appreciate that time is relative, not absolute. Ironically, after a thorough indoctrination in Newtonian physics, when the kindergartener encounters Special Relativity in the 1st grade, they find the relative nature of time to be extremely counter-intuitive.
Gravitational mass
Or, 'Inertial mass is proportional to gravitational charge'.
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Acceleration due to gravity
Or, 'Einstein's happiest thought'.
The fact that inertial mass is proportional to gravitational 'charge' implies that all objects fall to the Earth with the same acceleration. This is a fact amply demonstrable with the least effort in a kindergartener's backyard. (This phenomenon was also known to Galileo. Apocryphally, Galileo did such demonstrations by dropping objects from the Leaning Tower of Pisa.) Nevertheless, contrary to what happens in reality, every kindergartener 'knows' intuitively that heavier objects fall faster than lighter objects! It's a thought that's likely reinforced by the fact that loose sheets of paper or a bunch of feathers coast slowly to the floor compared to, say, a hammer destined for the big toe. This intuition often persists into adulthood - sometimes even in those who've had an unfortunate brush with physics early on and then blocked it completely out of their memory.
