The Seam-Shifted Revolution Is Headed for the Mainstream
Hey there! I want to give you a heads up about this article, because it doesn’t fit into a normal genre I write. Today, I won’t be telling you some new insight about a player you like, or creating some new nonsense statistic that tries to pull meaning from noise. This is a story about how baseball analysis is changing right before our eyes. A group of scientists and baseball thinkers are redefining the way we think about pitch movement, and I think it’s worth highlighting even if I don’t have anything to add to the conversation yet, because this new avenue of research is going to be front and center in Statcast-based analysis over the next few years.
“Seam-shifted wake,” as Andrew Smith, a student of Dr. Barton Smith (no relation) coined it, is a source of pitch movement that the first attempts at understanding the physics of a pitched baseball overlooked. It has already changed the way that coaches and pitchers approach pitch design, and due to recent data advances, it’s about to be everywhere. So let’s go over how we got here, to this newly observable way that pitchers deceive hitters, by starting at the beginning and working forward.
At its core, baseball is a game about one person trying to throw a ball past another person. There are other trappings — bases and baserunners, umpires, a strike zone, the mythology of Babe Ruth, and a million other sundry things. At the end of the day, though, everything starts with the pitcher trying to throw a ball past the batter.
Accordingly, baseball analysis over the years has focused on describing the flight of that ball. For a time, that simply meant describing the shape of pitches — they don’t call them curveballs for nothing. The next step was velocity — radar guns let us appreciate fastballs numerically rather than merely aesthetically.
In the past 15 years, the amount and scope of pitch-level analytical data has exploded. First, PITCHf/x quantified pitch location and movement. When we report a pitcher’s chase rate or how often a batter swings at pitches in the strike zone, it’s because the location where each pitch crosses the plate is recorded and logged. When we say a pitcher has eight inches of horizontal break on their slider, it’s because new technology allows us to measure it.
When Statcast debuted in 2015, it added another wrinkle: radar tracked the spin rate of each pitch in flight, putting a numerical value on something that had previously been only qualitative; a pitcher’s ability to generate movement through spin. Doctor Alan Nathan has written several authoritative studies discussing the value of this spin data.
One of Dr. Nathan’s key insights — one shared by many R&D departments across baseball but most eloquently explained here — was that raw spin rate doesn’t all lead directly to movement. If you’ve heard this part before, please feel free to skip ahead — you can Control+F to the words “frustratingly complex.” If you haven’t, though, let’s detour in this article full of detours to a quick discussion of spin.
Picture a car driving straight down a road. The tires on the car spin as the car moves, and if the car isn’t turning, the axis they spin around is pointed directly sideways (think of the car’s axels), perpendicular to the car’s forward movement. That’s called transverse spin. A baseball thrown with this spin — a perfectly backspinning fastball, say — creates movement due to the Magnus effect.
When people talk about fastballs rising, what they mean is that their transverse spin creates lift via the Magnus effect, making them fall less than a ball thrown with no spin would. When they talk about curveballs plummeting, it’s the same force applied in a different direction. Transverse spin — tire spin — creates movement via the Magnus effect.
Next, picture a football thrown with a perfect spiral. This spin, gyroscopic spin, doesn’t create movement via the Magnus effect. If you threw a baseball this way, the ball would still spin, but not in a way that creates Magnus-based movement; the relative angle between axis and flight path determines whether Magnus forces are created. In practice, most pitches are thrown with a mixture of gyroscopic and transverse spin. The exact composition of spin depends on grip, release, arm angle, and myriad other things the pitcher controls.
Here was a new insight: how much total spin a pitcher can generate is useful, but it’s largely useful for talking about what that pitcher can do, not what they’re currently doing. The higher the percentage of spin that is transverse (or “active”), the more Magnus-based movement a pitcher can generate.
I’ve attempted to be careful in mentioning that the movement we’re talking about here is specifically break created by the Magnus effect. You can model a ball’s total break as that produced by this interaction, but that’s just a model. Reality remains frustratingly complex, however, and as it turns out, baseballs move in ways that don’t fit into a tidy equation that can be solved using only spin, initial direction, and gravity.
A group of researchers led by Dr. Smith have spent years exploring, quantifying, and explaining a separate force, which Smith calls “seam-shifted wake.” In a series of posts, Smith was able to produce variable movement despite exactly identical spin orientation and magnitude by changing the location of the baseball’s seams. From there, he delved into the intricacies that led to this heretofore undiscovered source of movement. Researchers at Driveline Baseball appear to have been doing the same work in parallel, and published their own research on it late last year.
This leads us to a major breakthrough in the way that we can talk about spin. Before 2020, league-wide data on spin axis was inferred based on movement. In other words, analysts, myself included (though I’m more of an overzealous layperson and less of a scientist), measured the movement of the ball relative to its initial path. From there, they calculated the angle that would produce Magnus-based movement agreeing with the way the ball actually moved.
On an individual basis, pitchers already knew this wasn’t a perfect description of reality. By fixing high-speed cameras on their own deliveries, they could directly observe spin axis as the ball left their hand, and it didn’t always match up with what the movement-based angle calculations inferred. At a league level, however, those cameras didn’t exist. If you wanted a spreadsheet with every pitch thrown in 2019, your spin data was inferred, not observed.
In 2020, Statcast began collecting data with Hawkeye cameras. Those cameras could simply observe the axis of the ball at release, rather than inferring it based on movement. The two numbers don’t always agree. Why not? Seam-shifted wake! Smith, Nathan, and Harry Pavlidis published a pitch-level investigation that tracked the disagreement between observed angle (what the camera sees) and inferred angle (the movement-based calculation).
MLB and Baseball Savant now release graphics that show this divergence, as explained by this excellent article. Between this new data and Smith’s ongoing investigations, there’s plenty to unpack when thinking about pitch movement, but one thing is for sure: working out movement based on Magnus acceleration isn’t a complete picture of what’s happening between the mound and the plate.
Analysis of this data is still in its infancy, but the ramifications are potentially huge. Take just one example: spin mirroring, the idea that batters have trouble distinguishing between spin that moves in exactly opposite directions, relies on measuring the angle of spin. If you use pre-2020 data, however, you’re using the inferred angle, which is in some cases notably different from the way the ball actually spins.
The purported reason for this mirroring is that spin in opposite directions is visually indistinguishable. The problem is that the inferred spin axis data we were using to look for mirrored pitches didn’t always correctly match reality. If a ball leaves a pitcher’s hand with a 12:00 spin orientation only for seam-shifted wake to create horizontal movement, it might end up with an inferred spin orientation of, say, 10:00. Visually, however, the 12:00 spin is what a batter would see.
Well, maybe it’s what the batter would see. There’s even more confusion, though, because hands, baseballs, and all of reality exist in three dimensions, but we currently only record two. A pitch with 12:00 spin orientation but plenty of gyroscopic spin won’t resemble a pitch with 12:00 orientation and no gyroscopic spin from the batter’s perspective, depending on seam orientation. Heck, seam orientation changes what spin looks like as well. There’s far more to spin mirroring than what we can currently divine from publicly available data.
Over the next few years, I expect to see a raft of new research into seam-shifted wake, seam orientation, and how the two interact. There’s the pure physics research, working out how exactly turbulence created by seam movement can impact the ball’s flight. There’s data on how the wake works in practice; do pitches with more deviation between implied and inferred spin axes perform better? Do some pitchers succeed largely due to this effect? Eno Sarris is already looking into some of these questions, just to give one example.
I hope to do some of this research myself, and I’m sure that others at FanGraphs do as well. I’ve been spending a fair amount of my free time playing around with this data, and there’s still far more to learn. If there’s one lesson I’d take away from all of this though, it’s that we shouldn’t expect this next revolution in public-side analysis to be the last word.
Every revolution in data collection around pitching leads to more questions. Anyone who thinks their knowledge is final, that their plan for measuring pitch movement is perfect, eventually falls victim to one of the key limitations of every model: models only approximate reality, they don’t replace it.
If your model of spin axis involves only the Magnus effect, seam-shifted wake won’t exist for you. If your model of a hitter’s skill involves only his swinging strike rate and production on contact, you’ll miss any adjustments he makes in two-strike counts, because count-aware hitting doesn’t exist for you. These aren’t the same things — one’s a physical model and one’s an abstraction — but they both have one identical feature: they can’t account for what they don’t include.
With that caveat aside, the new era of movement analysis is going to be exciting. We’ve long wondered how some sinker- and changeup-heavy pitchers keep batters off balance despite middling velocity and movement. Smith’s research suggests that those two pitches, particularly when thrown with gyroscopic spin, can create meaningful non-Magnus movement. Why can’t batters square up Kyle Hendricks? The ball moves strangely!
In a year, we might think very differently about all kinds of different pitches, in the same way that measuring spin gave us new information about four-seam fastballs. We’ll certainly think differently about changeups, because we’re woefully short of ways to analyze their strange movement now. No matter how you slice it, we’ll be looking at the same kinds of pitches and thinking new things about them. It’s an exciting time to be learning new things about baseball, and we have physicists, cameras, and baseball laboratories to thank for it.
Update: this article has been updated to reflect the fact that Andrew Smith, not Dr. Barton Smith, coined the term “seam-shifted wake.”
Ben is a writer at FanGraphs. He can be found on Bluesky @benclemens.
thanks Ben, I’ve been lazily waiting for someone to write this exact article since I started seeing the term pop up recently, and you came through! Cheers
Yes! I just started seeing this about 3 months ago and I have been trying to piece things together since then. It’s great to have this.
One of the best articles I’ve ever read on FanGraphs, Ben. Thanks so much. It’s OK if you don’t have the answers. The journey provides all of the fun, anyway.
Are we going to see a resurgence of the knuckleball with this technology? You heard it here first.
I came here to say the same thing. So you heard it here second, I guess?
Screwballs too.
I hurt my elbow just reading this comment. 🙂
And the disillusionment of the average baseball fan continues apace, until there are no fans left except Fangraphs readers.
I’m probably wrong, but I don’t see it that way. Ben said it best at the beginning of the article. Baseball is, in essence, a pitcher trying to throw a ball past a batter. All the rest of this stuff is trappings for those of us who can’t just enjoy the simple pleasure of that match-up without digging into ridiculous levels of detail.
Or the people making millions off those matchups.
Some people like knowing how things work, others just care that they do. Tbere’s room for both.
Thank you for this Ben.
I feel confident every pitcher knows that seam orientation matters for how a ball moves and looks to a batter, just like spin axis & spin amount. Pitchers all over the world get different results just from changing their seam orientation. For example, some pitchers try to avoid their slider forming the “red dot” pointing at the hitter’s eyes, which can be changed with just orientation of seams. But it feels like alchemy…guessing.
It seems like the tricky part is making sense of the chaos inherent in fluid dynamics (air behaves like a low density liquid for these purposes). Now we have the cameras to capture and computers to crunch real world data at a level where we might see to what extent this movement can be controlled and predicted vs. the knuckleball (chaotic) effect — are there really just too many variable inputs? I suspect yes but it’s not necessarily a binary, and this will be really cool to follow.
Not just controlled and predicted but, more importantly, instantly fed back to the pitchers and pitching coaches. The process of learning a new pitch or tweaking an existing pitch will move faster when you’ve got data that can measure precisely what the effect of those tweaks are after just a few throws.
tangentially… one of these days an organization is going to use this new tech to enable pitchers to throw consistent and devastating knuckleball-type things, and hitters will just be helpless.
It will help not at all. The perfect knuckleball is released perfectly still, an incredible achievment. A great knuckleball pitcher can do this half of the time on a good day. His lesser efforts will follow the direction of the rotation, such as it is, one half to one full rotation. The knuckleball that is released so that the ball spins one rotation or so facing the pitcher (like a clock) is universally without movement and hammered. It is totally a feel pitch and analytics cannot help with feel. I’ve caught three knuckleball pitchers and they each gripped the pitch differently.
Got a lot of great links from this fantastic article! One of the most exciting things I’ve read on fangraphs this year.
ROCKING article, Ben!!!! I’d like you thoughts on the following
I think a breakthrough will happen when we discover a way to measure the seam Shiftedness. It may be simple like: the axis of the spin relative to some fixed line (The Plate, the rubber, etc.) However, it is probably multidimensional in that the effect will be a polynomial expression. It’s basically similar to physicists looking for an elusive “Complete Standard Model” – combining all the forces – including gravity.
The dependent variable would be the Effectiveness of a given pitch. The independent variables could include the direction of the axis, the speed of the rotation, the speed toward the batter and many other factors. I’d start by keeping the variable of the batter constant. Use the “average batter, or better yet, use Ben. I dream of FanGraphs creating an equation like this:
Ef = xSpz + ySpny + zAxx + zDrx + some fudge factor (even Einstein needed his “cosmological constant”)
Where
Ef = Effectiveness of the pitch
Sp = velocity of pitch on the vector released from the pitcher’s hand
Spn = Spin rate relative to the axis of spin
Ax = Axis of spin
Dr = directions of release
Hr = Height of the release above the rubber
I leave it to the physicists to factor in Heisenberg’s uncertainty principle and quantum entanglement.
Dang, baseball is SO cool. I’m in AA, but for those of you who don’t have those problems, you may have to toke up to get the real feel of the equation:-).
Wasn’t there a GIF or video somewhere of Javier Vazquez (I think) throwing a pitch that swerved one way, then made a late move in a different way? Not a knuckleball or even a forkball, but something with actual spin.
This would HAVE to be due to seam-shifted wake……
Bugs Bunny?
Jetsy Extrano has it linked below.
This is great! I had no idea that this was a thing, and I love how it’s already being tracked!
My big takeaway from this article was that seam-shifted wake is a thing and is tracked via inferred vs. observed spin axis. So my natural follow-up question is: what causes it? Is it just the laminar effect (where air flow is turbulent on one side and smooth on the other and the ball darts towards the turbulent side, correct?), or are there other types of seam-shifted wake?
Pure layperson speculation on my part, but I would guess that there are all kinds of possible effects from the orientation and frequency of the gyroscopic spin vs the relative orientation and relative rotational frequency of the spin movement of the seams. Some seam spin orientations relative to the gyroscopic spin orientation (e.g., those in the same direction or directly transverse to the gyroscopic spin) and/or rotational frequencies relative to the gyroscopic spin rate (e.g., those at a harmonic multiple or fraction), or perhaps a combo of both, may result in somewhat unpredictable effects, and therefore be difficult to hit. Knuckleballs may be one such example (perhaps not so much because there is little to no gyroscopic spin, but because there is little to no seam spin relative to the gyroscopic spin) that may be replicable at other gyroscopic spin orientations and speeds).
Is this the same aerodynamic effect that Alan Nathan described on that notorious 2011 Freddy Garcia pitch? Like swing bowling in cricket, or scuffing a baseball?
http://baseball.physics.illinois.edu/Garcia1.html
Most thought provoking and well written baseball article I have ever read. Cheers!
It surprises me that this topic has only recently come up in baseball. It’s foundational in bowling a cricket ball.
Granted, the aim in cricket is not so much to get the batter to miss, and more to get the wrong sort of contact (hello, Henry Chadwick!).
Granted, a horseshoe seam is not an equatorial seam.
But if I were a minor-league pitching coach, I might just be encouraging kids to watch video of, say, James Anderson. Or Glenn McGrath in his pomp.
So this predicts two seam and four seam fastballs would move differently? Which has been known for a hundred years or so?
Maybe? I had the same idea as you and almost posted a similar comment, but then realized that if you take a baseball with a 4-seam grip and give it half a revolution of backspin, you’re now at the 2-seam grip. Therefore, that would seem to suggest that there’s no difference.
I think it’s more that pitchers use different finger pressure with the 2-seam grip, which causes the ball to come off the fingers with a different spin orientation.
Don’t think they “interconvert” through backspin actually? A 2-seam (with pure transverse backspin) continues to have two seams pass by for each rotation, while a 4-seam continues to have four. So the Magnus force can differ; this is a traditional explanation for why 4-seams get more rise.
This wake effect is about whether the two ends of the spin axis are different in what seam pattern they present to the airflow. So it says, actually, that while a 2-seam is left-right mirror symmetric, a 4-seam is not, and *could* show lateral movement depending on whether the horseshoe “connectors” are to the right or to the left. I haven’t seen anyone look at whether that happens empirically…
Absolutely fascinating article, thanks!
I do have one question regarding “A pitch with 12:00 spin orientation but plenty of gyroscopic spin won’t resemble a pitch with 12:00 orientation and no gyroscopic spin”
I’m probably just not understanding definitions here, but how can a pitch with 12:00 spin orientation ever have nonzero gyroscopic spin? Or does this mean 12:00 is merely an *initial* spin orientation?
This is annoying to talk about because it’s hard to describe things in three dimensions. Basically, 12:00 is backspin, and 3:00 is sidespin, but all of that is transverse spin. If the axis the ball is spinning around is exactly perpendicular to movement — if the ball is headed in a straight line from the center of the mound to the center of home plate — then you can imagine an all-backspin all-transverse ball as tumbling backwards over itself, with the imaginary line the ball is spinning around pointing directly from first to third base.
Next, imagine tilting the line the ball spins around while leaving the orientation perfectly back-spun. The ball is still spinning as much, but only some of it is perpendicular to the direction of motion — think a line between first base and the opposite dugout. Ignoring seam-shifted wake, the only transverse spin is still straight up, because the ball is still backspinning. Because the axis of rotation and the flight path of the ball aren’t perpendicular, however, not all of the spin creates Magnus movement. If you could move that imaginary axis a full 90 degrees — so that the line the ball is spinning around would be drawn from home to second, the same flight path the ball is on — then you’d get no transverse spin at all, which would mean you couldn’t really describe the movement on a clock face.
TL;DR: Clock face numbers describe spin as if it were in two dimensions and all transverse. Real life is harder because it takes place in three dimensions, so our ways of describing it are lacking.
Thanks, Ben — I think I get it now and that it was a semantics thing. I was taking ’12:00′ to mean not only that the angular momentum vector is parallel to the ground, but also that it is perpendicular to the path. Your usage implies that it means only parallel to the ground, which indeed would allow for 12:00 spin with a non-zero gyro component. Thanks for the clarification!
Yeah the semantics are the worst. Reducing the dimensions on something is confusing, and it definitely took me a little bit to realize that that’s what the spin orientation numbers do.
Thanks, I had this exact same question too. I think it’s clearer if we recognize that the direction of total spin is uniquely defined by the spin axis. So what you were describing was a spin axis pointing (in our baseball coordinate system) from first base to the opposite dugout, and parallel to the ground.
Also, here’s a Driveline article that covers 3d spin direction: https://www.drivelinebaseball.com/2019/09/mastering-the-axis-of-rotation-a-thorough-review-of-spin-axis-in-three-dimensions/
Can this new gadget that directly measures spin rate also tell us the orientation of the seams?