Latest / Mechanical Engineering Made Simple / (#65) Gears Cams Bearings Precision Fits Failure
Transcript
- 0:00Welcome back, design junkies to Mechanical Engineering Made
- 0:02simple. Today we're we're undertaking a
- 0:04really critical deep dive into the very core of machine design.
- 0:08We're talking about the components that control motion,
- 0:11transmit power, and, you know, most importantly, manage all the
- 0:15stress and longevity. That's right.
- 0:16Gears, cams, bearings, linkages, the works.
- 0:20A whole vocabulary. Our analysis is coming from some
- 0:22seriously dense engineering handbooks.
- 0:25I mean, they focus intensely on the geometry, the manufacturing,
- 0:29and the sometimes brutal calculations you need to make
- 0:32sure these things actually survive.
- 0:34So our mission today is really to pull out the functional
- 0:37essence of these parts. Yeah, and to show you why every
- 0:39single moving part is a small hard won victory against the
- 0:43physics of failure. What becomes immediately clear,
- 0:46and you see it right away in the sources, is that it doesn't
- 0:49matter if you're looking at a simple little detent or a, you
- 0:52know, full on aerospace actuator.
- 0:54The design is just this massive balancing act.
- 0:57Every millimeter, every angle, every material choice has to be
- 1:01absolutely precise. There's no room for error.
- 1:04OK, so let's start with rotational power.
- 1:06Let's start with gears. The fundamental language of
- 1:08gears and 1st we have to define tooth size that really splits
- 1:13into two major systems. Metric and US.
- 1:16Right. In the metric world, we use
- 1:17what's called the module, and it's actually pretty simple.
- 1:20It's just the gears pitch diameter in millimeters divided
- 1:24by the number of teeth, OK. Straightforward enough, but in
- 1:26the US customary system we use the diameterial pitch.
- 1:29And this is one that always, always trips people up.
- 1:32OK, it's inverse. Totally inverse.
- 1:35It's the ratio of the number of teeth per inch of pitch
- 1:38diameter. So the physically larger the
- 1:40gear tooth is, the smaller the diametral pitch number becomes.
- 1:44It feels completely backwards. It does, but that's just how the
- 1:47ratio works. And that demand for precision,
- 1:50it flows right into the manufacturing process.
- 1:53You can't just cut the stuff out of a block of metal, no.
- 1:56Absolutely not. To create a gear face that can
- 1:58withstand constant high load, you're talking about highly
- 2:01specialized operations. You need milling then maybe
- 2:05hobbing for spur gears, or end milling and shaping for internal
- 2:08gears. And some things, like bevel
- 2:11gears need their own specialized machines.
- 2:14Exactly. And it's not just gears.
- 2:16It's astonishing when you look at something like a standard
- 2:19roller chain sprocket, right? They have to adhere strictly to
- 2:22ANI standard geometry. The dimensions aren't just
- 2:26picked, they are derived from these complex equations based on
- 2:29the pitch, which we call P and the number of teeth N.
- 2:34So every single curve is mathematically defined.
- 2:37To the thousandth of an inch. I mean take 1/2 inch pix roller
- 2:40chain. The source gives a minimum
- 2:42seating curve value of .317 inches.
- 2:46It's calculated down to that level because if that contact
- 2:49point is even slightly off. You just destroy the chain.
- 2:51You destroy the chain in the sprocket.
- 2:53It's a rapid failure which, you know, leads us right into
- 2:55material selection. Because the material has to
- 2:57handle those forces. Precisely.
- 2:59For something low speed, light load, sure.
- 3:01You might get away with engineering plastics, acedal,
- 3:04polycarbonate, things like that. But for any serious power
- 3:06transmission. You immediately jump to heat
- 3:09treated ferrous and non ferrous alloys, no question.
- 3:12And this is where it gets really interesting because this
- 3:14quality, both material manufacturing, it's all
- 3:18quantified by the AGMA quality numbers, yes.
- 3:21And this is where you get a just a profound insight into the
- 3:25mechanical hierarchy of the world.
- 3:27AGMA numbers define exactly how accurate your gear manufacturing
- 3:31has to be, so. Give us an example.
- 3:32What's the range look like? OK, think about a simple
- 3:35agricultural bailing machine. It might be perfectly functional
- 3:38with quality numbers between, say, 5:00 and 7:00.
- 3:41OK. So that's pretty loose
- 3:42tolerance. Very loose, but then you jump
- 3:44into something sensitive like electronic instrument control
- 3:48and guidance systems. That's a whole different ball
- 3:50game. It is.
- 3:51Suddenly you need quality numbers from 10 all the way up
- 3:54to 14. The tolerance just tightens
- 3:57massively. And what's at the very top end?
- 3:59Well, if you were engineering something truly demanding like a
- 4:02space navigation sextant and a Star Trekker, you need quality
- 4:06#14 and up. The required accuracy for a
- 4:09mechanism pointing to a star is just.
- 4:13It's a different universe compared to 1 compacting A.
- 4:16It shows that precision isn't just a cost factor.
- 4:18No, it's a mission critical constraint, and that material
- 4:22choice also dictates how you can even machine the part.
- 4:26Machinability is hugely affected by heat treatment.
- 4:29I've heard that some of the high carbon steels are just a
- 4:31nightmare to work with. They are a 4150 grade.
- 4:35Steel is notoriously difficult to machine.
- 4:37You have to specify tempering for steels like 4140 just to
- 4:41make them manageable on the shop floor.
- 4:43And all this is before the system is even running.
- 4:45Once it is, you have to deal with the operational forces.
- 4:48Right, which the designers have to anticipate.
- 4:50A simple spur gear will generate tangential and radial loads, but
- 4:54systems like helical gears or even more so, worm gearing.
- 4:58They introduce that third dimension of.
- 5:00Force, a massive axial load rust and the calculation for the
- 5:04forces in a worm gear system is where things get really complex.
- 5:08You can't just use simple geometry.
- 5:09Not at all. Yeah, you have to factor in the
- 5:12coefficient of dynamic friction and the system's overall
- 5:15efficiency. And that complicates everything,
- 5:17especially selecting the right support bearings, because that
- 5:21friction is what converts the rotational input into a crushing
- 5:25axial load that the bearings have to absorb day in and day
- 5:29out. OK, calculating those continuous
- 5:31forces is hard enough, but what about controlling the timing and
- 5:35the specific path of a movement? That's even harder.
- 5:38It is, and that brings us to the systems that manage selective
- 5:41controlled movements cams. Right, so cams are what convert
- 5:45that simple rotation into something much more complex.
- 5:48Exactly. They're defined as mechanical
- 5:50components that convert continuous Rotary motion into a
- 5:54specific, you know, predetermined translating or
- 5:56oscillating action using a follower.
- 5:58And the absolute dictator of which Cam profile you choose.
- 6:01It's speed. It's always speed.
- 6:03So for low speed movement. You might use something called a
- 6:05uniform velocity motion, but this is actually terrible
- 6:08because when the follower hits the flat part of the Cam, it
- 6:11goes from zero acceleration to maximum acceleration instantly.
- 6:16It's like hitting a wall. The shock is incredible.
- 6:18And that shock is exactly what you're trying to engineer out of
- 6:21the system. 100% uniform acceleration and parabolic
- 6:24motions are better for moderate speeds because they smooth out
- 6:27that transition, but for any kind of high speed application
- 6:31you absolutely must use cycloidal motion.
- 6:34Why is cycloidal motion the go to for high speed?
- 6:38Because it's the only profile that keeps the acceleration
- 6:40curve smooth, the shape is mathematically designed to ramp
- 6:45up and ramp down both the velocity and the acceleration
- 6:47gradually. It prevents those massive G
- 6:50forces from destroying the follower and, you know, the
- 6:53mechanism itself. We see that design battle
- 6:55against shock loads everywhere in Cam design.
- 6:57I was reading that the slope lines defining the rise and fall
- 7:00have to be terminated with a parabolic curve.
- 7:02Specifically to prevent shock loads.
- 7:05If you skip that tiny design detail, your follower mechanism
- 7:08will literally hammer itself apart.
- 7:10It's amazing. Now there are two main types of
- 7:13follower systems right open track and close track.
- 7:15Correct. You have open track cams which
- 7:18require the follower to be held against the Cam surface by a
- 7:20spring. Think of a standard engine valve
- 7:23train. OK, so a spring is pushing it.
- 7:25Back exactly, but then you have close track cams where the
- 7:28follower actually travels inside a groove.
- 7:30This gives you positive action. Meaning no spring is needed.
- 7:33No spring. This is critical in
- 7:36manufacturing machinery because if a spring breaks in an open
- 7:39track system, the whole machine fails immediately.
- 7:42Close track cams eliminate that specific risk.
- 7:45But the challenge with the spring based systems, the open
- 7:48track ones, is what happens at high speeds.
- 7:51You get spring floating. The spring just can't keep up
- 7:54with a Cam profile and the follower loses contact.
- 7:57It literally floats off the surface.
- 7:58How do you fix that? The fix is designing the spring
- 8:01with a natural frequency below the cyclic rate of operation,
- 8:05and often the solution is to put multiple springs in parallel.
- 8:09That's exactly what you see in the complex valve springs of
- 8:12high performance automotive engines.
- 8:13And then on the total opposite end of complexity, you've got
- 8:17the simplest Cam of all. The eccentric Cam the most
- 8:21economical to make. It's often just a round disk
- 8:24that's offset from its center axis.
- 8:26You see those used for simple rise functions or actuating
- 8:30limit switches and timing devices.
- 8:32Yeah, but you can't run them at high speed.
- 8:34For ultra high speed we have to look at some really advanced
- 8:36systems like the Desmodromic system.
- 8:39This is the system that was famously used by Mercedes-Benz
- 8:42racing engines back in the 50s. It was.
- 8:44It actually used a second Cam to physically force the follower
- 8:48back down. It completely eliminated the
- 8:51need for springs. So if you ever hear a high
- 8:53revving 1950s Grand Prix engine, that really distinct mechanical
- 8:58clatter. That's the sound of springs
- 9:00being completely engineered out of existence.
- 9:02It's the noise of pure positive mechanical action.
- 9:05Amazing. Now when you're designing these
- 9:07Cam profiles, there are other constraints too, right?
- 9:10You have to look at the Contact interface.
- 9:11Oh absolutely, the geometry is critical.
- 9:13You have to make sure the roller radius is smaller than the
- 9:15minimum radius of curvature along the Cam profile.
- 9:19Otherwise you'd actually cut into the Cam itself when you're
- 9:21manufacturing it. You'd undercut it and you also
- 9:24have to calculate the contact stress, which we call S sub S
- 9:28For a material like SAE 4340 steel he treated to Rockwell
- 9:32C50, the Max allowable compressive stress is 220,000
- 9:38PSI. £220,000 per square inch. And if your calculation exceeds
- 9:43that stress limit, you have designed a fatigue failure
- 9:46point. It's guaranteed to break OK.
- 9:48Let's shift from cams to linkages, the building blocks of
- 9:52movement. We all remember the six basic,
- 9:54simple machines, but we're focusing on mechanisms that
- 9:58translate motion in really ingenious ways.
- 10:00And maybe the most dramatic is the toggle joint linkage.
- 10:03This thing is just incredible. It's a mechanism designed
- 10:06specifically to multiply force massively as the linkage angle
- 10:10approaches 90°. The mechanical advantage and the
- 10:12velocity ratio both approach Infinity.
- 10:15That's a trick of geometry. It is the classic examples are
- 10:18the bolt lock action of the Lucre pistol, or you know, giant
- 10:21rock crushing machinery. Both use the toggle to generate
- 10:24thousands of pounds of crushing force with a relatively small
- 10:27input. Then you have the four bar
- 10:28linkage which is just everywhere.
- 10:30Absolutely ubiquitous, just 4 links connected by 4 pivots.
- 10:34You see it in everything from car suspensions to construction
- 10:37equipment. But it looks so deceptively
- 10:39simple. It does, but mathematically its
- 10:42action is extremely complicated. Before the 1950s, figuring out
- 10:46the precise motion for all points was often just trial and
- 10:49error. You'd build a prototype and see
- 10:51what it did. It wasn't until the
- 10:53mathematician Freudenstein developed his geometric
- 10:55relationship that designers had a really robust mathematical
- 10:59tool. That's right, but even then, the
- 11:02sheer difficulty means that mathematical solutions are often
- 11:05approximations at best. Which is why even today, high
- 11:09speed motion analysis is so critical, you have to actually
- 11:12film the prototype. Exactly.
- 11:14You watch the complex actions happening at 12,000 frames per
- 11:17second just to confirm the mechanism is performing the way
- 11:20you thought it would. And this analysis has its own
- 11:22defined vocabulary. You see these letters RP and S?
- 11:25It's a kinematic vocabulary. R is for a revolute joint, which
- 11:28is just simple rotation. P stands for a prism joint,
- 11:32which allows sliding, and S is the sphere joint, your classic
- 11:35ball joint. And these designations let
- 11:37engineers define these incredibly complex 3 dimensional
- 11:41mechanisms. They do, but then there are some
- 11:44linkages like the RSSR linkage that just defied the standard
- 11:49rules of kinematics. The maverick space mechanisms.
- 11:52That's what they're called because they achieved this
- 11:54complex non standard motion that you just can't analyze using
- 11:57basic planar geometry. They're a class of their own.
- 12:00All right, so all of these moving complicated parts, the
- 12:03gears, the cams, the linkages, they all have to be supported.
- 12:07Which brings us to Part 3, Bearings and the science of
- 12:10precision fits. Let's start with the simplest
- 12:12type, the plain bearing, often centered bronze.
- 12:16And their selection comes down to one critical calculation.
- 12:19The PV calculation the pressure velocity factor P is the
- 12:23pressure on the projected area and V is the surface velocity
- 12:26and designers have to balance these.
- 12:27And this balance is everything. You can't just Max out all the
- 12:30values. No, you can't use the maximum
- 12:32for all three simultaneously. If you run your machine at a
- 12:35super high velocity, you have to lower the load.
- 12:38If you don't, the bearing material will simply melt or
- 12:41disintegrate from the frictional heat.
- 12:42It's a hard limit. A very hard limit.
- 12:45For example, lead based Babbitt has a maximum PV of 35,000, but
- 12:49PTFE fabric, a more advanced synthetic material, only has a
- 12:53limit of 25,000. These material limitations
- 12:56directly constrain how fast and how heavy your machinery can
- 12:59possibly be. Then we move up to rolling
- 13:02element bearings, your ball, roller, tapered and cylindrical
- 13:05types. Here we're relying on
- 13:07authoritative bodies like the Anti Friction Bearing
- 13:10Manufacturers Association, the ABMA for standards on load
- 13:14ratings and fatigue life. And this is where the cost of
- 13:17miscalculation just becomes brutally clear.
- 13:19It does. There are two critical
- 13:21approximate rules for bearing life that every single engineer
- 13:24has to know. The first one is this.
- 13:26Doubling the bearing load reduces bearing life to 110th.
- 13:30110th not half. 110th That is a monumental penalty for a small
- 13:34increase in load. It's huge, and the second rule
- 13:37is just as important. Doubling the speed reduces
- 13:40bearing life to 1/2. So controlling load and speed
- 13:43isn't just about performance. It's about controlling the
- 13:46maintenance schedule, the downtime, the entire life cycle,
- 13:49cost of the machine itself. The sensitivity brings us to
- 13:53maybe the ultimate constraint in all of mechanical design.
- 13:56The precision fit, the fit of a bearing into its housing, is
- 14:00often the last and most critical step.
- 14:02It really is. EU customary classes of fit
- 14:05range from RC1 which are close sliding fits just for accurate
- 14:09location. All the way U to FN 5.
- 14:10Which are the heavy force fits use for parts that are designed
- 14:13to be highly stressed and never ever move again.
- 14:16Let's use an example, an RC3 precision running fit on a 1 1/2
- 14:20inch nominal shaft. The tolerance window required is
- 14:23just incredibly narrow. The shaft and the hole have to
- 14:25be machined to clearances that are often less than two
- 14:28thousandths of an inch across the entire diameter.
- 14:31That's tighter than a human hair.
- 14:33Tighter than a human hair across the whole part.
- 14:36If you miss that tolerance by even a fraction, the shaft will
- 14:39either seize up from heat expansion or it will vibrate
- 14:42itself to pieces. Immediate fatigue failure.
- 14:45And for the tightest connections the interference or force fits
- 14:48you have to calculate the stresses.
- 14:49You have to. Designers must treat the parts
- 14:52as thick walled cylinders to calculate the internal stresses.
- 14:56This determines how much torque can be transmitted and the axial
- 14:59force you need to physically press them together.
- 15:01And the stress analysis is absolutely critical here.
- 15:04Because the maximum tangential and radial stresses happen right
- 15:07in the contact surfaces, designers have to use stress
- 15:10concentration factors, maybe 1.5 to 2 point O, especially for
- 15:14thick hubs pressed onto a shaft if you neglect those factors.
- 15:18You risk a sudden brittle fracture or a catastrophic
- 15:21fatigue failure somewhere down the line.
- 15:23Absolutely. So our deep dive today has moved
- 15:26us all the way from the generalized motion of gears,
- 15:28through the controlled linear action of cams and linkages and
- 15:32finally into the critical support systems defined by
- 15:34bearings, these hyper precise fits.
- 15:37The complexity forces designers to master combined disciplines.
- 15:41You can't just be a mechanical engineer anymore.
- 15:43You can't. You have to understand
- 15:45mechanical, electrical and electronic systems.
- 15:48And that really is the ultimate insight when you look at modern
- 15:51electromechanical products, whether it's an industrial
- 15:53switch assembly or a high precision titanium camera
- 15:57shutter, It demands that engineers become general
- 16:00practitioners. Yeah, you have to grasp all
- 16:02three disciplines rather than sticking to a narrow specialty.
- 16:06Precision in one area requires mastery in all the others.
- 16:09And this complexity brings us right back to the limitations of
- 16:12pure analysis. You know, we discussed how
- 16:14incredibly difficult it is to mathematically solve the precise
- 16:18motion of something like a four bar linkage.
- 16:20And that difficulty often forces modern engineers to rely on
- 16:24computer aided design and, critically, physical dynamic
- 16:27analysis. So here's the final thought.
- 16:29When you look at any complex machine operating smoothly
- 16:32today, an engine, a robotic arm, a printing press, anything, ask
- 16:36yourself this. Are the specific movements you
- 16:38are watching the result of elegant mathematics that
- 16:42perfectly modeled the entire system from the start?
- 16:44Or were they finely tuned by watching a prototype's slow
- 16:47motion video captured at 12,000 frames per second, with
- 16:50engineers correcting the geometry based on observed
- 16:53physical reality?