Retaining Ring Groove Calculator

Retaining Ring Groove Calculator

Groove diameter, width, depth and the ring’s radial cling for DIN 471 external and DIN 472 internal rings, with BOTH thrust limits — the ring’s own shear and the groove material’s yield — computed at either maker’s safety factors, the governing one identified, and the corner radius on the retained part derating it. For DIN 471 geometry the groove almost always governs, which is not what most people expect.

Retaining ring groove

Size and materials → groove and thrust capacity
DIN 471 external rings are tabulated here from Ø3 to Ø60; DIN 472 internal rings from Ø10, so the smallest sizes have no internal equivalent.
An external ring’s groove diameter is SMALLER than the shaft and an internal ring’s is LARGER than the bore, but the depth is (|difference|)/2 either way.
DIN 471 and 472 rings are C60 or C75 spring steel at 47–54 HRC, so roughly 1,500–1,800 MPa tensile and 900–1,100 MPa in shear. 900 is a conservative figure and it is an input because the makers’ own numbers differ.
The shaft or housing, not the ring. About 250 MPa for mild steel, 350 for a medium-carbon shaft, 600+ for a hardened one, 100–250 for aluminium alloy. This is usually the number that decides the answer.
Two named makers publish the same two formulas with different factors on the shear term. Both are offered; neither is averaged.
The part the ring is holding. A radius or chamfer larger than the ring’s own edge break lets the load push the ring up the radius and out of the groove — and Rotor Clip’s own example puts the loss at 72%. Zero means a square-cornered part.
Take this from the ring’s own datasheet. Smalley publish maximum GROOVE-bottom radii of 0.005 in (0.13 mm) up to 1 in diameter and 0.010 in (0.25 mm) above, which is a different dimension but the same order — and the derating is proportional either way.
Not a circuit: the groove in section on the left, and the two thrust limits as bars on the right. The shaft is the block across the middle and the notch in its top face is the groove. The whole section is scaled by the RING THICKNESS, which keeps the one ratio that decides the answer — thickness against groove depth — true at every size, and makes the groove depth visible at all: it is 2 to 3% of the shaft diameter, so a section at the shaft's own scale would show a scratch. How far the ring stands out of the groove is drawn nominally, because that needs the ring's radial width and this page does not carry it. The hatched block is the ring. To its left is the retained part, and its CORNER RADIUS is the thing this drawing exists for: turn the corner-radius input up and watch the square corner become a curve the ring can climb, with an arrow appearing for the radial component that comes with it — the part of the axial thrust that is now pushing the ring OUT of a groove only a few hundredths of the shaft deep. Rotor Clip put the cost of a maximum allowable radius at 72% of the capacity. The two bars are the ring's own shear limit and the groove material's yield limit, both scaled against whichever is larger, so the shorter bar is the answer: for DIN 471 geometry it is almost always the groove, which means a retaining ring failure is usually the shaft giving way rather than the ring cutting.
11,545NExample

A DIN 471 ring on a Ø30 mm shaft, 900 MPa ring shear, 350 MPa shaft yield, Rotor Clip’s safety factors, square-cornered part

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Two limits, and the smaller one wins

groove depth = |shaft or bore − groove Ø| / 2  ·  P_ring = π · D · T · S_s / F_ring  ·  P_groove = π · D · depth · σ_y / F_groove  ·  capacity = min(P_ring, P_groove) × R_max / R_corner
D
shaft or bore diameter. Both limits are proportional to it, so the RATIO between them does not depend on size — only on the ring thickness against the groove depth
T
ring thickness. It is one to three times the groove depth, which is why the ring rarely governs
depth
groove depth, computed as half the difference between the shaft or bore and the groove diameter. Two to three per cent of the diameter — these grooves are shallow
S_s, σ_y
the ring’s shear strength and the GROOVE material’s yield strength. Two different parts, and the second is usually the weaker
F
safety factors, and the two makers disagree: Rotor Clip use 4 on ring shear and Smalley 3, both use 2 on groove yield. Both are on the selector; neither is averaged
R_max / R
the corner-radius derating. Rotor Clip’s own example loses 72% of the capacity at the maximum allowable radius, which is the single largest effect on this page

Worked example

A DIN 471 ring on a Ø30 mm shaft, 900 MPa ring shear, 350 MPa shaft yield, Rotor Clip's safety factors, square-cornered part
The groove: d2 = 28.60 mm on a 30 mm shaft, so the depth is (30 − 28.60)/2 = 0.70 mm — 2.3% of the shaft diameter. Groove width 1.60 mm against a 1.50 mm ring, so there is 0.10 mm of axial slack
Ring shear limit = π × 30 × 1.50 × 900 / 4 = 31,809 N
Groove yield limit = π × 30 × 0.70 × 350 / 2 = 11,545 N
The GROOVE governs, by a factor of 2.76. That is not an accident of these numbers: the crossover needs σ_y/S_s = (T/depth) × (2/4) = 1.07, so this shaft would have to yield at 964 MPa before the ring became the weaker part. At Ø20 the same calculation asks for 1,080 MPa and at Ø6 for 2,100 MPa, which is more than the ring's own shear strength — so on the small sizes the groove governs no matter what you make the shaft of
So the capacity is 11,545 N, about 11.5 kN, and the failure to expect is the groove wall deforming
Now put a 0.5 mm radius on the retained part against a 0.25 mm allowable: the derating is 0.25/0.5 = 0.5, so 5,773 N — half the capacity for a corner nobody dimensioned. Rotor Clip's own example is worse: 5,950 lb square-cornered against 1,650 lb at the maximum allowable radius, a 72% loss
The ring's radial cling here is (28.60 − 27.90)/2 = 0.350 mm. That 0.35 mm of grip is what holds the ring in when a radius on the retained part tries to lift it out — and it is what centrifugal force works against on a rotating assembly

Two limits, two makers, and which one actually governs

LimitFormulaSafety factorWhat it means
The ring’s own shear capacityP_r = G_f · π · D_s · T · S_s / F_sRotor Clip: 4. Smalley: 3 recommendedThe ring is being pushed out of its groove and has to shear across its own thickness. T is the ring thickness, S_s its shear strength. The two makers publish the same formula with different factors, and both are offered above rather than averaged.
The groove material’s yieldP_g = G_f · π · D_s · d · σ_y / F_sBoth makers: 2The ring is bearing on the groove wall and the wall is yielding. d is the GROOVE DEPTH, σ_y the yield strength of the shaft or housing. This is the limit that governs almost every DIN 471 installation.
Which governsThe smaller of the two — Smalley: “the actual load capacity is the lesser of the two”—Set them equal and the crossover condition is σ_y / S_s = (T / d) · (F_groove / F_ring). With Rotor Clip’s factors that is (T/d)/2, and T/d for DIN 471 runs from 4.0 at Ø3 to 1.33 at Ø60. So below about Ø30 the crossover would need a groove material STRONGER in yield than the ring is in shear, which does not happen: the groove always governs. Above Ø35, with a ring and a shaft of comparable hardness, the ring can be the weaker part.
What neither formula covers——Smalley say it plainly: the formulas “do not take into account any dynamic or eccentric loading”. A ring loaded off-axis, or by an impact, or by a part that can cock in its bore, is outside both of these. So is fatigue. So is a ring that has been installed and removed more than once.
The useful conclusion is the third row. For DIN 471 geometry — a groove 2 to 3% of the shaft diameter deep against a ring one to three times that thickness — the GROOVE is the weaker part at every size up to about Ø30, whatever materials you choose, because the crossover would require the shaft to be stronger in yield than the ring is in shear. That reframes the whole failure mode: a retaining ring failure is usually the shaft’s groove wall deforming and letting the ring climb out, not the ring cutting. Which is why the corner radius on the retained part matters so much. This page sizes a part; it does not certify one. Where the answer carries a consequence — a load path, a lifting duty, a pressure boundary, a fastener holding something that can fall — confirm it against the design code that governs the application, and against the manufacturer’s own rating, before relying on it.

DIN 471 external rings — every groove dimension

ShaftRing thickness s (mm)Groove Ø d2 (mm)Groove depth (mm)Groove width m (mm)Axial slack m − sMin distance to the shaft end n (mm)Ring free inside Ø d3 (mm)Radial cling (mm)Groove depth ÷ shaft
Ø30.402.800.1000.500.100.302.700.0500.0333
Ø40.403.800.1000.500.100.303.700.0500.0250
Ø50.604.800.1000.700.100.304.700.0500.0200
Ø60.705.700.1500.800.100.505.600.0500.0250
Ø80.807.600.2000.900.100.607.400.1000.0250
Ø101.009.600.2001.100.100.609.300.1500.0200
Ø121.0011.500.2501.100.100.8011.000.2500.0208
Ø161.0015.200.4001.100.101.2014.700.2500.0250
Ø201.2019.000.5001.300.101.5018.500.2500.0250
Ø251.2023.900.5501.300.101.7023.200.3500.0220
Ø301.5028.600.7001.600.102.1027.900.3500.0233
Ø351.5033.001.0001.600.103.0032.200.4000.0286
Ø401.7537.501.2501.850.103.8036.500.5000.0313
Ø502.0047.001.5002.150.154.5045.800.6000.0300
Ø602.0057.001.5002.150.154.5055.800.6000.0250
The groove-depth column is computed as (d1 − d2)/2 and that identity is how this table’s columns were verified: a first fetch returned the headers offset by one, and only the depth relation identified the right mapping. It holds on all fifteen rows here and all ten of the internal table. Three other columns are worth reading. The axial slack, m − s, is 0.10 mm for rings up to 1.75 mm thick and 0.15 above — that is how much the retained part can move before the ring takes load, and it is not nothing on a precision assembly. The radial cling, (d2 − d3)/2, is how far the ring’s free inside diameter sits below the groove diameter: that is the grip which resists the ring being lifted out, and it is the quantity centrifugal force works against on a rotating assembly. And the last column shows how shallow the groove is: 2 to 3% of the shaft diameter, which is why the groove material is usually the weaker part. These dimensions come from a published standard’s table, not from a formula. The standard itself is cited below and the printed values are attributed to the catalogue they were taken from; a different publisher may round differently in the last digit.

The corner radius on the retained part — how these actually fail

ConditionEffect on capacitySource
Square-cornered part against the ringFull capacity. The load is carried on the ring’s flat face and the reaction is a pure axial thrustThe condition both formulas assume
A corner radius or chamfer on the retained part, within the maker’s maximumReduced, in proportion: P″ = P′ · R_max / R. Part of the axial load is now a radial component trying to lift the ring out of the grooveRotor Clip publish the derating directly
A corner radius at the maximum the maker allowsRotor Clip’s own worked example: a Series HO-100 ring “which abuts a square-cornered part … has a static thrust capacity of 5,950 lbs. The same ring, seated next to a part having the maximum allowable corner radius or chamfer, has an allowable load of 1,650 lbs.” That is a loss of 72%Rotor Clip
A corner radius LARGER than the maker allowsOutside the published data, and this is the failure mode. The radial component grows with the radius; past some point it exceeds what the ring’s cling into the groove can resist and the ring rolls out of the groove under load, releasing whatever it was holdingThe mechanism follows from the geometry; the derating relation above only applies up to the maximum
A radius in the GROOVE BOTTOMA different quantity with a similar effect: a generous groove-bottom radius reduces the flat wall the ring bears against. Smalley publish maximum groove-bottom radii of 0.005 in up to 1 in diameter and 0.010 in aboveSmalley
This is how retaining rings fail, and it is not by shearing. The ring sits in a shallow groove — 2 to 3% of the shaft diameter — and it is held there by its radial cling, which this page computes. A square-cornered retained part turns the thrust into a pure axial load on the ring’s face. Put a radius or a chamfer on that part and some of the thrust becomes a radial force trying to lift the ring out. Rotor Clip’s numbers put the cost of a maximum allowable radius at 72% of the capacity; exceed the maximum and you are outside the data with a ring that can roll out of its groove. On a drawing, the corner of the part that abuts a retaining ring is a dimension that needs stating, not leaving to the machinist. This page sizes a part; it does not certify one. Where the answer carries a consequence — a load path, a lifting duty, a pressure boundary, a fastener holding something that can fall — confirm it against the design code that governs the application, and against the manufacturer’s own rating, before relying on it.

DIN 472 internal rings — the same dimensions, the other way round

BoreRing thickness s (mm)Groove Ø d2 (mm)Groove depth (mm)Groove width m (mm)Axial slack m − sMin distance to the bore mouth n (mm)Ring free outside Ø d3 (mm)Radial cling (mm)
Ø101.0010.400.2001.100.100.6010.800.200
Ø121.0012.500.2501.100.100.8013.000.250
Ø161.0016.800.4001.100.101.2017.300.250
Ø201.0021.000.5001.100.101.5021.500.250
Ø251.2026.200.6001.300.101.8026.900.350
Ø301.2031.400.7001.300.102.1032.100.350
Ø351.5037.001.0001.600.103.0037.800.400
Ø401.7542.501.2501.850.103.8043.500.500
Ø502.0053.001.5002.150.154.5054.200.600
Ø602.0063.001.5002.150.154.5064.200.600
An internal ring’s groove diameter is LARGER than the bore and its free outside diameter is larger than the groove, so it grips outward — the mirror of the external case, and the depth is still half the difference. The same groove-width allowance applies: 0.10 mm over the ring thickness up to 1.75 mm and 0.15 above. Two practical differences from the external case are worth naming. An internal ring has to be COMPRESSED to fit, so it is loaded in the opposite sense during assembly, and over-compressing it past its elastic limit leaves it permanently loose. And a bore is usually the softer of the two parts in an assembly, so the groove yield limit tends to govern even more strongly than it does on a shaft. These dimensions come from a published standard’s table, not from a formula. The standard itself is cited below and the printed values are attributed to the catalogue they were taken from; a different publisher may round differently in the last digit.

What this page refuses to compute, and why

WhatWhy not
A maximum RPM for the ringRefused. The mechanism is real and Smalley state it: “failure happens when these centrifugal forces are great enough to expand and lift the retaining ring from the groove.” But Smalley decline to publish a general formula and ask that critical applications be referred to their engineers. The closed form that IS published elsewhere carries a “factor for number of turns (1 turn = 1.909, 2 turns = 3.407, 3 turns = 4.958)”, which makes it a SPIRAL-WOUND ring formula rather than a stamped-circlip one — and the worked example printed beside it did not reproduce from the equation as transcribed, by a factor of about eighty. Two reasons to refuse: wrong kind of ring, and arithmetic that does not close. What this page gives instead is the radial cling, which is the quantity centrifugal force works against.
DIN 471’s own F_N and F_R load columnsNot reproduced. The standard tabulates a groove load and a ring load, and distributors reprint them — but no fetch in this batch returned them together with the material assumptions and the safety factor that make them meaningful. A load figure whose basis is unknown is worse than none, particularly on a page where the whole point is which of two limits governs. The computed route is used instead, with both makers’ factors offered and the material strengths as inputs.
Dished and bowed ringsNamed but not computed. DIN 471 and 472 have bowed (Form B) and dished variants whose purpose is to take up the axial slack the table above shows — m − s, 0.10 to 0.15 mm — by acting as a light spring. That eliminates the rattle and the impact loading a loose ring sees, at the cost of a lower thrust capacity, because part of the ring’s section is now doing spring work. The thrust figures on this page are for the flat form.
Fatigue, impact and eccentric loadingOutside both published formulas. Smalley: they “do not take into account any dynamic or eccentric loading”, and recommend testing for abusive conditions. A ring holding a part that can cock in its bore is loaded eccentrically whatever the catalogue says.
Installation and re-useA ring that has been expanded past its elastic limit during assembly is permanently loose, and nothing on this page can tell you whether it has been. Internal rings are the more vulnerable because they are compressed to fit. Use the right pliers, and do not re-use a ring that matters.
The RPM refusal is the significant one, because the question is real: centrifugal force does lift rings out of grooves, and it is a published failure mode. What is not available is a formula for THIS kind of ring that reproduces its own worked example. Rather than print one that does not, the page names the mechanism, computes the cling that resists it, and says to ask the maker — which is what the maker themselves say to do. This page sizes a part; it does not certify one. Where the answer carries a consequence — a load path, a lifting duty, a pressure boundary, a fastener holding something that can fall — confirm it against the design code that governs the application, and against the manufacturer’s own rating, before relying on it.

Two limits, and the groove is the one that gives way

A retaining ring has two thrust limits and the smaller one wins — and for DIN 471 geometry the smaller one is almost always the groove. Rotor Clip and Smalley publish the same pair of formulas: the ring’s own shear capacity, π·D·T·S_s divided by a safety factor, and the groove material’s yield, π·D·depth·σ_y divided by another. Both scale with the diameter, so which governs depends only on the ring thickness against the groove depth and on the two safety factors. Set them equal and the crossover needs σ_y/S_s = (T/depth)·(F_groove/F_ring). With Rotor Clip’s factors of 4 and 2 that is (T/depth)/2, and T/depth for DIN 471 runs from 4.0 at Ø3 down to 1.33 at Ø60. So below about Ø30 the crossover would require the SHAFT to yield at a higher stress than the ring shears at, which does not happen — the groove governs whatever you make the shaft of. Above about Ø35 with a hardened shaft, the ring can be the weaker part.

That conclusion reframes the failure mode, and it is worth stating because it is not what people expect. A retaining ring failure is usually the groove wall deforming and letting the ring climb out, not the ring cutting through. Which means a harder shaft buys capacity where a better ring does not — and it means the geometry at the groove’s mouth matters more than the ring’s own strength. The two makers also differ on the safety factor for exactly the term that is least often binding: Rotor Clip use 4 on ring shear, Smalley 3. Both are on the selector and neither is averaged.

The corner radius on the retained part is the largest single effect on this page and the one most often left off a drawing. A square-cornered part turns the thrust into a pure axial load on the ring’s flat face. Put a radius or a chamfer on it and part of that thrust becomes a radial component pushing the ring up the radius — out of a groove that is only two to three per cent of the shaft diameter deep. Rotor Clip publish the derating as a straight proportion, P″ = P′·R_max/R, and their own worked example puts the scale of it beyond argument: a Series HO-100 ring “which abuts a square-cornered part … has a static thrust capacity of 5,950 lbs. The same ring, seated next to a part having the maximum allowable corner radius or chamfer, has an allowable load of 1,650 lbs.” A 72% loss, for a corner nobody dimensioned. Exceed the maximum and you are outside the data entirely, with a ring that can roll out under load.

What holds it in is the radial cling, and this page computes it. The ring’s free inside diameter sits below the groove diameter by (d2 − d3)/2 — 0.35 mm on a Ø30 external ring — and that is the grip resisting anything that tries to lift the ring out. It is also the quantity centrifugal force works against on a rotating assembly, which is why it is printed. There is a second small dimension worth reading: the axial slack, groove width minus ring thickness, which DIN sets at 0.10 mm for rings up to 1.75 mm thick and 0.15 mm above. That is how far the retained part can move before the ring takes load, and on a reversing assembly it turns a steady thrust into an impact every cycle. Bowed and dished rings exist to take up exactly that slack, acting as a light spring at the cost of thrust capacity.

And one refusal, stated rather than glossed. This page does not compute a maximum RPM. The mechanism is real and published — Smalley: “failure happens when these centrifugal forces are great enough to expand and lift the retaining ring from the groove” — but Smalley decline to publish a general formula and refer critical cases to their engineers, and the closed form that IS published elsewhere carries a “factor for number of turns (1 turn = 1.909, 2 turns = 3.407, 3 turns = 4.958)”, which makes it a spiral-wound ring formula rather than a stamped circlip one. Its own worked example also did not reproduce from the equation as transcribed, by a factor of about eighty. Two independent reasons not to print it. DIN 471’s own F_N and F_R load columns are left out for a related reason: no fetch returned them together with the material assumptions and safety factor that make them mean anything, and a load figure with an unknown basis is worse than none on a page whose whole point is which limit governs. For the axial location this ring is an alternative to, the set screw dimensions calculator covers the collar-and-screw route; for a shoulder machined into the shaft instead, the corner radius discussion above is the same geometry; and for locating rather than retaining, the dowel pin and hole calculator.

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Frequently asked questions

What is the thrust capacity of a retaining ring?

The smaller of two numbers: the ring’s own shear capacity, π·D·T·S_s divided by a safety factor, and the groove material’s yield capacity, π·D·(groove depth)·σ_y divided by another. Smalley put it as “the actual load capacity is the lesser of the two”. This page computes both and says which governs. For a DIN 471 ring on a Ø30 shaft with a 900 MPa ring in a 350 MPa shaft, using Rotor Clip’s factors, the ring’s limit is about 32 kN and the groove’s about 11.5 kN — so the groove governs by nearly three to one.

Which fails first, the ring or the groove?

The groove, almost always, on DIN 471 geometry. The crossover condition is that the groove material’s yield strength divided by the ring’s shear strength equals the ring thickness divided by the groove depth, times the ratio of the two safety factors. For DIN 471 the thickness is one to four times the groove depth, and with Rotor Clip’s factors of 4 and 2 that means the shaft would have to yield at up to twice the stress the ring shears at on the small sizes — which cannot happen. So a retaining ring failure is normally the groove wall deforming and the ring climbing out. A harder shaft helps; a better ring does not.

Does a corner radius on the retained part matter?

Enormously, and it is the dimension most often left off the drawing. A square corner puts a pure axial load on the ring’s face. A radius or chamfer turns some of that thrust into a radial force lifting the ring up the radius and out of a groove only 2 to 3% of the shaft diameter deep. Rotor Clip derate in proportion, P″ = P′·R_max/R, and their own example is stark: a Series HO-100 ring rated 5,950 lb against a square-cornered part carries 1,650 lb against one with the maximum allowable radius — 72% gone. Exceed the maximum and you are outside the data with a ring that can roll out under load.

How deep should the groove be?

Use the standard’s groove diameter; do not choose a depth. DIN 471 and DIN 472 specify d2, and the depth is half the difference between the shaft or bore and d2 — 0.70 mm on a Ø30 shaft, which is 2.3% of the diameter. This page computes it for every tabulated size and the identity (d1 − d2)/2 holds on all 25 rows, which is how the table’s columns were verified after a first fetch returned them offset. Cutting a deeper groove is not an improvement: it weakens the shaft in a stress concentration and the ring will not fill it.

Why does this page not give a maximum RPM?

Because no formula was found for this kind of ring that reproduces its own worked example. The mechanism is real — Smalley: “failure happens when these centrifugal forces are great enough to expand and lift the retaining ring from the groove” — but Smalley decline to publish a general formula and refer critical applications to their engineers. The closed form published elsewhere carries a factor for the number of turns, which identifies it as a spiral-wound ring formula rather than a stamped circlip one, and its printed example did not reconcile with the equation as transcribed. What this page gives instead is the ring’s radial cling, which is the grip centrifugal force is working against. For a rotating assembly, ask the maker or use a self-locking form.

What are bowed and dished rings for?

Taking up the axial slack. A DIN groove is wider than the ring by 0.10 mm for rings up to 1.75 mm thick and 0.15 mm above, so the retained part can move that much before the ring takes load. On a steady thrust that does not matter; on a reversing or vibrating assembly it turns the load into an impact every cycle, and neither published capacity formula covers impact. A bowed or dished ring acts as a light spring across that slack and holds the part against it. The cost is thrust capacity, because part of the ring’s section is doing spring work — so the flat-form figures on this page do not apply to them.

Can I reuse a retaining ring?

Not one that matters. Installing a ring expands an external one or compresses an internal one, and if it goes past its elastic limit it comes off the pliers permanently deformed — with a free diameter that no longer grips the groove. Internal rings are the more vulnerable because compressing is the harder direction to control. Nothing on this page, and nothing in an inspection, can reliably tell you whether a used ring still has its cling. On anything whose failure releases a load, fit a new one.

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References

  1. DIN 471, Retaining rings (circlips) for shafts, and DIN 472 for bores. Cited by number. The groove columns used here are from Westfield Fasteners’ DIN 471 and DIN 472 specification sheets, with rows 3–6 mm independently confirmed against Aspen Fasteners and rows 10 mm and 50 mm against American Ring. Every one of the 25 rows satisfies groove depth = (d₁ − d₂)/2 exactly, which is how the column mapping was established after a first fetch returned the headers offset by one. Material and hardness from American Metric’s catalogue: C60 or C75 spring steel at 47–54 HRC. The standard’s own F_N and F_R load columns are NOT reproduced — no fetch returned them with the definitions and material assumptions that make them meaningful, and a load figure whose basis is unknown is worse than none.
  2. Rotor Clip Company. Formulas: Retaining Ring Load Capacity. The two limits used here, verbatim: ring shear P_r = (G_f × D_s × T × π × S_s) / F_s with “F_s = Safety factor (typically 4)”, and groove yield P_g = (G_f × D_s × d × π × σ_y) / F_s with a safety factor “typically 2”. Also the corner-radius derating, P″_r = (P′_r × R_max) / R, and the worked example that makes the case: “A Series HO-100 ring which abuts a square-cornered part … has a static thrust capacity of 5,950 lbs. The same ring, seated next to a part having the maximum allowable corner radius or chamfer, has an allowable load of 1,650 lbs.” — a loss of 72%.
  3. Smalley Steel Ring Company. Load Capacity. The same two limits with different safety factors: P_R = (π × D × T × S_S) / K with “K = Safety factor (3 recommended)” and P_G = (π × D × d × S_Y) / K with 2 recommended, and the instruction to take “the lesser of the two”. Also that the formulas “do not take into account any dynamic or eccentric loading”, and maximum groove-bottom radii of 0.005 in up to 1 in diameter and 0.010 in above. Two named makers, two different safety factors on the same formula: both are printed here rather than averaged.
  4. On ring speed: Smalley’s RPM Capacity states the mechanism — “failure happens when these centrifugal forces are great enough to expand and lift the retaining ring from the groove” — and declines to publish a general formula, asking instead that critical applications be referred to their engineers. Design World and Motion Control Tips publish a closed form, but it carries a “factor for number of turns (1 turn = 1.909, 2 turns = 3.407, 3 turns = 4.958)”, which makes it a SPIRAL-WOUND ring formula and not a stamped-circlip one; the worked example printed alongside it did not reproduce from the equation as transcribed, by a factor of about eighty. This page therefore states the mechanism and the quantity that resists it — the ring’s radial cling, (d_groove − d_ring inside)/2 — and refuses to compute a speed limit. See the note beside the results.
  5. Aspen Fasteners. Metric DIN 9021 Flat Fender Washers, Metric DIN 433 Flat Washers, Metric DIN 127 Type B Helical Spring Split Lock Washers and Metric DIN 471 External Retaining Rings for Shafts. Distributor specification sheets, used for the printed dimensions those standards are cited for.