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
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
Two limits, and the smaller one wins
- 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
| Limit | Formula | Safety factor | What it means |
|---|---|---|---|
| The ring’s own shear capacity | P_r = G_f · π · D_s · T · S_s / F_s | Rotor Clip: 4. Smalley: 3 recommended | The 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 yield | P_g = G_f · π · D_s · d · σ_y / F_s | Both makers: 2 | The 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 governs | The 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. |
DIN 471 external rings — every groove dimension
| Shaft | Ring thickness s (mm) | Groove Ø d2 (mm) | Groove depth (mm) | Groove width m (mm) | Axial slack m − s | Min distance to the shaft end n (mm) | Ring free inside Ø d3 (mm) | Radial cling (mm) | Groove depth ÷ shaft |
|---|---|---|---|---|---|---|---|---|---|
| Ø3 | 0.40 | 2.80 | 0.100 | 0.50 | 0.10 | 0.30 | 2.70 | 0.050 | 0.0333 |
| Ø4 | 0.40 | 3.80 | 0.100 | 0.50 | 0.10 | 0.30 | 3.70 | 0.050 | 0.0250 |
| Ø5 | 0.60 | 4.80 | 0.100 | 0.70 | 0.10 | 0.30 | 4.70 | 0.050 | 0.0200 |
| Ø6 | 0.70 | 5.70 | 0.150 | 0.80 | 0.10 | 0.50 | 5.60 | 0.050 | 0.0250 |
| Ø8 | 0.80 | 7.60 | 0.200 | 0.90 | 0.10 | 0.60 | 7.40 | 0.100 | 0.0250 |
| Ø10 | 1.00 | 9.60 | 0.200 | 1.10 | 0.10 | 0.60 | 9.30 | 0.150 | 0.0200 |
| Ø12 | 1.00 | 11.50 | 0.250 | 1.10 | 0.10 | 0.80 | 11.00 | 0.250 | 0.0208 |
| Ø16 | 1.00 | 15.20 | 0.400 | 1.10 | 0.10 | 1.20 | 14.70 | 0.250 | 0.0250 |
| Ø20 | 1.20 | 19.00 | 0.500 | 1.30 | 0.10 | 1.50 | 18.50 | 0.250 | 0.0250 |
| Ø25 | 1.20 | 23.90 | 0.550 | 1.30 | 0.10 | 1.70 | 23.20 | 0.350 | 0.0220 |
| Ø30 | 1.50 | 28.60 | 0.700 | 1.60 | 0.10 | 2.10 | 27.90 | 0.350 | 0.0233 |
| Ø35 | 1.50 | 33.00 | 1.000 | 1.60 | 0.10 | 3.00 | 32.20 | 0.400 | 0.0286 |
| Ø40 | 1.75 | 37.50 | 1.250 | 1.85 | 0.10 | 3.80 | 36.50 | 0.500 | 0.0313 |
| Ø50 | 2.00 | 47.00 | 1.500 | 2.15 | 0.15 | 4.50 | 45.80 | 0.600 | 0.0300 |
| Ø60 | 2.00 | 57.00 | 1.500 | 2.15 | 0.15 | 4.50 | 55.80 | 0.600 | 0.0250 |
The corner radius on the retained part — how these actually fail
| Condition | Effect on capacity | Source |
|---|---|---|
| Square-cornered part against the ring | Full capacity. The load is carried on the ring’s flat face and the reaction is a pure axial thrust | The condition both formulas assume |
| A corner radius or chamfer on the retained part, within the maker’s maximum | Reduced, 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 groove | Rotor Clip publish the derating directly |
| A corner radius at the maximum the maker allows | Rotor 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 allows | Outside 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 holding | The mechanism follows from the geometry; the derating relation above only applies up to the maximum |
| A radius in the GROOVE BOTTOM | A 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 above | Smalley |
DIN 472 internal rings — the same dimensions, the other way round
| Bore | Ring thickness s (mm) | Groove Ø d2 (mm) | Groove depth (mm) | Groove width m (mm) | Axial slack m − s | Min distance to the bore mouth n (mm) | Ring free outside Ø d3 (mm) | Radial cling (mm) |
|---|---|---|---|---|---|---|---|---|
| Ø10 | 1.00 | 10.40 | 0.200 | 1.10 | 0.10 | 0.60 | 10.80 | 0.200 |
| Ø12 | 1.00 | 12.50 | 0.250 | 1.10 | 0.10 | 0.80 | 13.00 | 0.250 |
| Ø16 | 1.00 | 16.80 | 0.400 | 1.10 | 0.10 | 1.20 | 17.30 | 0.250 |
| Ø20 | 1.00 | 21.00 | 0.500 | 1.10 | 0.10 | 1.50 | 21.50 | 0.250 |
| Ø25 | 1.20 | 26.20 | 0.600 | 1.30 | 0.10 | 1.80 | 26.90 | 0.350 |
| Ø30 | 1.20 | 31.40 | 0.700 | 1.30 | 0.10 | 2.10 | 32.10 | 0.350 |
| Ø35 | 1.50 | 37.00 | 1.000 | 1.60 | 0.10 | 3.00 | 37.80 | 0.400 |
| Ø40 | 1.75 | 42.50 | 1.250 | 1.85 | 0.10 | 3.80 | 43.50 | 0.500 |
| Ø50 | 2.00 | 53.00 | 1.500 | 2.15 | 0.15 | 4.50 | 54.20 | 0.600 |
| Ø60 | 2.00 | 63.00 | 1.500 | 2.15 | 0.15 | 4.50 | 64.20 | 0.600 |
What this page refuses to compute, and why
| What | Why not |
|---|---|
| A maximum RPM for the ring | Refused. 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 columns | Not 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 rings | Named 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 loading | Outside 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-use | A 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. |
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.
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.
Related calculators
References
- 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.
- 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%.
- 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.
- 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.
- 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.
