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7.3 Non-Threaded Fasteners: Keys, Pins, Clevises, Retaining Rings, Rivets, Lugs & Anchors

Key Takeaways

  • Parallel keys fail by shear (τ=2TdwL\tau = \frac{2T}{dwL}) or side bearing (σb=4TdhL\sigma_b = \frac{4T}{dhL}); for square keys with Ssy=0.577SyS_{sy} = 0.577 S_y, bearing needs about 15.5%15.5\% more length than shear.

  • Clevis pin connections must be verified against five independent failure modes: pin double shear, pin bending (under gap clearance), bearing on tang and fork, net-section eye tension, and edge shear tearout.

  • Retaining ring (snap ring) axial thrust capacity is dictated by the weaker of two limits: groove wall plastic yield bearing or ring shear/dishing, with corner chamfers on the retained component creating severe prying failure if allowable radii are exceeded.

  • Riveted structural joints fail via rivet shear, plate bearing, net-section tension across hole patterns, or edge tearout (e≥1.5de \ge 1.5 d), with joint efficiency defined as the ratio of allowable joint capacity to unpunched plate tensile strength.

  • Lifting hardware follows its own standards: ASME BTH-1 sets Nd=2.00N_d = 2.00 (Category A) or 3.003.00 (Category B), and ASME B30.26 shackles carry a design factor of at least 5 with a 30%30\% derating for side loads of 6∘6^\circ to 45∘45^\circ.

Last updated: October 2026

7.3 Non-Threaded Fasteners: Pins, Rivets, Retaining Rings & Keys

While threaded fasteners provide clamping preload and straightforward disassembly, mechanical assemblies depend extensively on non-threaded fasteners for positive torque transmission, precise spatial alignment, axial shaft retention, and permanent structural joining. These components include parallel and square shaft keys, splines, machine pins, clevis joints, retaining rings (snap rings), and structural rivets. Each fastener presents unique kinematic constraints, localized stress concentrations, and multi-mode structural failure criteria.


Parallel and Square Shaft Keys (ANSI B17.1)

Shaft keys are demountable mechanical elements inserted at the interface between a rotating shaft and a mounted component (such as a gear, pulley, sprocket, or flexible coupling) to provide positive torsional connection while preventing relative rotational slip.

                         Square Key Shaft-Hub Interface
                                [ Hub Body ]
                       +------------------------------+
                       |       Hub Keyseat            |
                       |         +----------+         |
                       |         |   Key    |         |
      -- Shaft Centerline ------>| - - - - -| <-------+-- Horizontal Shear Plane
                       |         | (w x h)  |         |   Area A_s = w * L
                       |         +----------+         |
                       |       Shaft Keyseat          |
                       +------------------------------+
                               [ Solid Shaft ]

Standard Key Dimensions & Geometry

According to ANSI B17.1, keys are standardized based on nominal shaft diameter dd:

  • Square Keys: Standard practice for shafts up to d=6.5 ind = 6.5\text{ in} (165 mm165\text{ mm}). The nominal key width ww and height hh are equal: w=h≈d4w = h \approx \frac{d}{4}
  • Rectangular (Flat) Keys: Used for shafts larger than 6.5 in6.5\text{ in} or for thin-walled hubs where deep keyways would weaken the hub. The width remains w≈d/4w \approx d/4, while the height is reduced to h≈d/6h \approx d/6.

Keyway Types & Stress Concentration Factors

Cutting a keyseat into a cylindrical shaft creates sharp re-entrant corners, introducing severe geometric stress concentrations that reduce the shaft's torsional and bending fatigue endurance:

  • Profile Keyway: Cut with an end mill plunging radially and traversing axially. Its sharp ends produce high stress concentration; Shigley's first-iteration estimates for an end-mill keyseat (bottom radius r/d≈0.02r/d \approx 0.02) are Kt≈2.14K_t \approx 2.14 in bending and Kts≈3.0K_{ts} \approx 3.0 in torsion.
  • Sled-Runner Keyway: Cut with a disc milling cutter that runs out gradually at the ends. The gradual runout lowers the bending stress concentration to about Kt≈1.7K_t \approx 1.7, which is why sled-runner seats are preferred near highly stressed shaft sections.

Failure Modes: Direct Shear vs. Compressive Bearing

When a shaft of diameter dd transmits torque TT, the tangential force FF acting at the shaft surface (r=d/2r = d/2) is:

F=Td/2=2TdF = \frac{T}{d/2} = \frac{2 T}{d}

This force must be resisted by the key across two primary independent failure modes: horizontal shear and side compressive bearing.

1. Direct Horizontal Shear Failure

The tangential force FF attempts to shear the key along the horizontal interface separating the shaft keyseat from the hub keyseat. The shear area is As=wLA_s = w L, where ww is key width and LL is effective key length:

τ=FAs=2Td⋅w⋅L≤Ssyn\tau = \frac{F}{A_s} = \frac{2 T}{d \cdot w \cdot L} \le \frac{S_{sy}}{n}

Using the Distortion Energy (von Mises) yield criterion for ductile steel (Ssy=0.577SyS_{sy} = 0.577 S_y):

Lshear=2Tnd⋅w(0.577Sy)L_{\text{shear}} = \frac{2 T n}{d \cdot w (0.577 S_y)}

2. Compressive Bearing Failure

The tangential force compresses the vertical sides of the key. Half the key height (h/2h/2) is embedded in the shaft keyseat, and half (h/2h/2) is embedded in the hub keyway. The projected compressive bearing contact area is Ab=(h/2)LA_b = (h/2) L:

σb=FAb=2T/d(h/2)L=4Td⋅h⋅L≤Sycn≈Syn\sigma_b = \frac{F}{A_b} = \frac{2 T / d}{(h/2) L} = \frac{4 T}{d \cdot h \cdot L} \le \frac{S_{yc}}{n} \approx \frac{S_y}{n}

Solving for the minimum required length to prevent compressive crushing:

Lbearing=4Tnd⋅h⋅SyL_{\text{bearing}} = \frac{4 T n}{d \cdot h \cdot S_y}

Comparing Shear vs. Bearing for Square Keys (w=hw = h)

Taking the ratio of required lengths for a standard square key where w=hw = h:

LbearingLshear=4Tnd⋅w⋅Sy2Tnd⋅w(0.577Sy)=42/0.577=2×0.577=1.155\frac{L_{\text{bearing}}}{L_{\text{shear}}} = \frac{\frac{4 T n}{d \cdot w \cdot S_y}}{\frac{2 T n}{d \cdot w (0.577 S_y)}} = \frac{4}{2 / 0.577} = 2 \times 0.577 = 1.155

Note

Under the Distortion Energy theory (Ssy=0.577SyS_{sy} = 0.577 S_y), compressive bearing is slightly more critical than direct shear, requiring an approximately 15.5%15.5\% longer key. Under the conservative Maximum Shear Stress (Tresca) theory (Ssy=0.50SyS_{sy} = 0.50 S_y), the ratio is exactly 1.01.0, meaning a square key exhibits identical resistance to shear and bearing.

In practice the key length is usually close to the hub length, commonly about 0.75d0.75d to 1.5d1.5d. Keys much longer than about 1.5d1.5d do not share load evenly, because shaft twist concentrates the load at one end.


Alternative Keys & Involute Splines

      Woodruff Key                   Involute Spline Profile
    +--------------+                        /\      /\      /\
    |              |                       /  \    /  \    /  \
    \              /                      /    \__/    \__/    \
     \____________/                       -- Circular Pitch P --
   (Semicircular Rocking)                (Self-Centering, High Torque)

1. Woodruff Keys

Woodruff keys are semicircular discs that fit into matching curved slots broached or milled into the shaft. Because the key can rock within its semicircular bed, it easily accommodates tapered shafts and self-aligns with matching hub tapers. However, the deep seat cut for a Woodruff key removes more shaft material than a straight keyway, which weakens the shaft; Woodruff keys are therefore favored for smaller shafts, tapered shaft ends and lighter-duty drives.

2. Taper & Gib-Head Keys

Taper keys feature an axial taper of 1/8 in/ft1/8\text{ in/ft} (1:961:96) along their top face, matching an internal taper in the hub keyway. When driven in axially, the key wedges firmly against the shaft and hub, transmitting torque while simultaneously providing axial retention without setscrews. Gib-head keys include an integral hammer head to allow extraction. Limitation: The radial wedging force introduces shaft eccentricity, causing dynamic runout and vibration in high-speed machinery.

3. Involute Splines (ANSI B92.1)

Splines consist of multiple integral longitudinal teeth machined along the external circumference of a shaft, mating with internal broached teeth in a hub. Modern machinery universally favors involute splines over straight-sided (parallel) splines:

  • Pressure Angles: Standardized at 30∘30^\circ, 37.5∘37.5^\circ, or 45∘45^\circ.
  • Self-Centering Action: Under torque, the 30∘30^\circ or 45∘45^\circ involute tooth flanks generate equalizing radial forces that center the hub precisely on the shaft axis.
  • Reduced Stress Concentration: Rounded tooth fillets and shallow tooth depth yield far lower stress concentrations than rectangular keyways.
  • Torque Capacity Formula: T=12pDmhLNtkeT = \frac{1}{2} p D_m h L N_t k_e where pp is the allowable bearing pressure (much lower for sliding splines than for fixed splines), DmD_m is the pitch diameter, hh is active radial tooth engagement height, LL is engaged spline length, NtN_t is the number of teeth, and ke<1k_e < 1 is a load-sharing factor that accounts for spacing errors, because not every tooth carries its full share.

Machine Pins: Dowel, Taper, Roll & Cotter

Machine pins serve two distinct functional roles: precision semi-permanent spatial alignment and direct shear load transfer.

        Dowel Pin                   Roll / Spring Pin               Cotter Pin
     +-------------+                 /-------------\                  __
     |  Hardened   |                |   Slotted     |                /  \
     |  & Ground   |                | Spring Steel  |               | || |
     +-------------+                 \-------------/                |_||_|
   (Precision Locate)              (Tolerance Absorbing)          (Nut Retain)
  • Dowel Pins: Solid cylindrical pins manufactured from alloy steel, case- or through-hardened (Rc50–60R_c 50\text{--}60), and precision ground to tight diametral tolerances (±0.0001 in\pm 0.0001\text{ in}). Used in reamed holes to accurately fix the relative spatial position of split housings, gearbox casings, and die plates before tightening clamping bolts.
  • Taper Pins: Feature a standard uniform taper of 1/4 in/ft1/4\text{ in/ft} (1:481:48). When driven into matched reamed tapered holes, they wedge solidly, resisting loosening while allowing rapid disassembly.
  • Roll / Spring Pins: Formed by rolling high-carbon spring steel into a slotted or coiled tubular cylinder. Manufactured intentionally oversize, they compress elastically when driven into standard drilled holes. The continuous radial expansion spring force holds the pin firmly in place without precision reaming, absorbing shock loads and thermal expansion.
  • Cotter Pins: Split-shank wire pins inserted through transverse drilled holes in clevis pins or castle nuts, with the split tines flared outward to provide a positive mechanical retention stop.

Clevis Joints: Multi-Mode Failure Criteria

A clevis joint connects an actuator rod (male tang/eye) to a mounting bracket (female fork) via a cylindrical clevis pin, accommodating pure angular pivoting in a single plane. When an axial tensile load PP is applied, the joint must be analyzed against five distinct structural failure modes:

                         Clevis Joint Failure Planes
                                      P
                                      ^
                                      | (Tang / Eye)
                           +----------+----------+
                           |         (O)         | <-- Mode 4: Net Tension
                           +----+-----------+----+
                                |   (Pin)   |      <-- Mode 5: Tearout
                       +--------+-----------+--------+
       Mode 1:         |  Fork  |   Tang    |  Fork  |
     Double Shear ===> |  Ear   |    Eye    |  Ear   | <=== Mode 1: Double Shear
                       +--------+-----------+--------+
                           |                     |
                           v                     v
                          P/2                   P/2

1. Mode 1: Pin Double Shear

The cylindrical pin is supported on both sides by the fork ears while the center tang pulls in the opposite direction. The pin must shear across two transverse circular cross sections:

τ=P2Apin=P2(πdp24)=2Pπdp2≤Ssyn=0.577Syn\tau = \frac{P}{2 A_{\text{pin}}} = \frac{P}{2 \left(\frac{\pi d_p^2}{4}\right)} = \frac{2 P}{\pi d_p^2} \le \frac{S_{sy}}{n} = \frac{0.577 S_y}{n}

2. Mode 2: Pin Bending

If manufacturing clearances create a gap gg between the tang and each fork ear, or if the plates are thick, the pin acts as a beam subjected to bending. Assuming uniform bearing pressure across the tang and across each ear of thickness tforkt_{\text{fork}}:

Mmax⁡=P2(ttang4+g+tfork2)=P8(ttang+4g+2tfork)M_{\max} = \frac{P}{2}\left( \frac{t_{\text{tang}}}{4} + g + \frac{t_{\text{fork}}}{2} \right) = \frac{P}{8}\left( t_{\text{tang}} + 4 g + 2 t_{\text{fork}} \right) σbending=Mmax⁡(dp/2)I=32Mmax⁡πdp3≤Syn\sigma_{\text{bending}} = \frac{M_{\max} (d_p/2)}{I} = \frac{32 M_{\max}}{\pi d_p^3} \le \frac{S_y}{n}

3. Mode 3: Bearing Stress on Pin and Holes

Compressive contact stress develops along the projected diametral contact areas:

  • Bearing on Center Tang: σb,tang=Pdpttang≤Sy,tangn\sigma_{b,\text{tang}} = \frac{P}{d_p t_{\text{tang}}} \le \frac{S_{y,\text{tang}}}{n}
  • Bearing on Fork Ears: σb,fork=P2dptfork≤Sy,forkn\sigma_{b,\text{fork}} = \frac{P}{2 d_p t_{\text{fork}}} \le \frac{S_{y,\text{fork}}}{n}

4. Mode 4: Net Section Tension Across Eye Hole

The eye cross-section is reduced by the pin hole diameter dpd_p:

σt=P(w−dp)ttang≤Sutn\sigma_t = \frac{P}{(w - d_p) t_{\text{tang}}} \le \frac{S_{ut}}{n}

5. Mode 5: Edge Shear Tearout

If the pin hole is placed too close to the end of the tang, the pin will tear out a plug along two parallel shear planes. With aa measured from the hole center to the end of the tang, each plane has length of roughly a−dp/2a - d_p/2:

τtearout=P2(a−dp/2) ttang≤Ssyn\tau_{\text{tearout}} = \frac{P}{2 (a - d_p/2)\, t_{\text{tang}}} \le \frac{S_{sy}}{n}

To prevent tearout, standard design guidelines require a≥1.5dpa \ge 1.5 d_p.


Retaining Rings (Snap Rings) & Axial Retention

Retaining rings (snap rings) are stamped or wire-formed spring steel rings fitted into shallow circumferential grooves machined into shafts (external rings) or housing bores (internal rings) to axially position bearings, gears, and pins.

                       Retaining Ring Axial Thrust
                                 Retained Component
                                  +--------------+
                                  |              | --> Axial Thrust Load F_r
       Shaft Surface              |              |
       --------------+            +-------+------+  <-- Critical Corner Chamfer
                     | Groove             | Ring |
                     +------+             +------+  <-- Groove Wall Yielding
                            | Depth y     |
                            +-------------+

Failure Modes & Allowable Thrust Capacity

Retaining ring assemblies fail under three distinct mechanisms:

  1. Groove Wall Yielding (FgF_g): The compressive contact stress against the soft shaft or housing material exceeds its yield strength, causing the groove lip to shear or deform plastically: Fg=πdySynF_g = \frac{\pi d y S_y}{n} where dd is nominal shaft/bore diameter, yy is groove depth, and SyS_y is the yield strength of the shaft material.
  2. Ring Shear Capacity (FrF_r): Direct transverse shear across the hardened spring steel ring: Fr=πdtτallownF_r = \frac{\pi d t \tau_{\text{allow}}}{n} where tt is the ring axial thickness and τallow≈0.577Sy\tau_{\text{allow}} \approx 0.577 S_y of the spring steel ring (Rc45–52R_c 45\text{--}52).
  3. Dishing / Prying Failure (Corner Chamfer Effect): Retaining rings rely on sharp, square contact against the retained component. If the retained bearing or gear has a large corner radius or chamfer (RR), the axial thrust load acts eccentrically away from the groove edge. This induces a severe prying bending moment that dishes the ring outward, causing it to pop out of the groove at loads far below its catalog rating. Always install a sharp-cornered square spacer washer between a radiused bearing and a retaining ring.

Riveted Joints & Structural Efficiency

Rivets are permanent fasteners comprising a cylindrical shank with a preformed head. After insertion through aligned holes, the plain end is mechanically upset (bucked) to form a second closing head.

Failure Modes of Riveted Lap & Butt Joints

  1. Rivet Shear: τ=Pm⋅nr⋅(π4d2)\tau = \frac{P}{m \cdot n_r \cdot \left(\frac{\pi}{4} d^2\right)}, where m=1m = 1 for single shear (lap joint) and m=2m = 2 for double shear (butt joint with two cover plates), and nrn_r is the total number of rivets.
  2. Plate Bearing: σb=Pnr⋅d⋅t\sigma_b = \frac{P}{n_r \cdot d \cdot t}, where tt is plate thickness.
  3. Plate Net-Section Tension: σt=P(w−nrowd)t\sigma_t = \frac{P}{(w - n_{\text{row}} d) t}, where nrown_{\text{row}} is the number of rivet holes in the critical fracture row.
  4. Plate Edge Tearout: Avoided by maintaining minimum edge margin e≥1.5de \ge 1.5 d to 2.0d2.0 d.

Joint Efficiency (η\eta)

Joint efficiency is the ratio of allowable joint load capacity to the tensile strength of the solid, unpunched plate:

η=Pallowable jointPsolid plate=Palloww⋅t⋅St\eta = \frac{P_{\text{allowable joint}}}{P_{\text{solid plate}}} = \frac{P_{\text{allow}}}{w \cdot t \cdot S_t}

Well-designed structural rivet joints achieve efficiencies of η≈70% to 85%\eta \approx 70\%\text{ to }85\%.


Lifting Lugs, Shackles & Anchors

Pin-Connected Lifting Lugs

A lifting lug (padeye) is a plate with a pin hole, so it is checked exactly like the clevis tang above: net-section tension beside the hole, shear tear-out beyond the hole, bearing of the pin on the plate, pin shear and bending, and the weld or bolts that attach the lug to the load. ASME BTH-1 (Design of Below-the-Hook Lifting Devices) sets the design factor for such hardware: Nd=2.00N_d = 2.00 for Design Category A and Nd=3.00N_d = 3.00 for Design Category B (service where loads or conditions are less predictable).

Sling geometry raises lug loads. For a symmetric two-leg sling with each leg at angle θ\theta from vertical, each leg carries

T=W2cos⁡θT = \frac{W}{2\cos\theta}

so a 30∘30^\circ leg angle raises leg tension by about 15%15\% over a vertical pick, and a 60∘60^\circ angle doubles it.

Shackles (ASME B30.26)

Shackles are rated by their rated load (working load limit). ASME B30.26 requires a design factor of at least 55 for shackles rated up to 150 tons (44 above that). Loading a shackle off its in-line axis reduces its rating:

Side-loading angle from in-lineRated-load reduction (B30.26)
0∘0^\circ to 5∘5^\circNone
6∘6^\circ to 45∘45^\circ30%30\%
46∘46^\circ to 90∘90^\circ50%50\%
Over 90∘90^\circNot recommended; consult the manufacturer

Mini-example: A 20 kN20\text{ kN} load is lifted by two sling legs at 30∘30^\circ from vertical, so each leg carries 20/(2×0.866)=11.5 kN20/(2 \times 0.866) = 11.5\text{ kN}. If each leg attaches through a shackle with a rated load of 19.6 kN19.6\text{ kN} (2 t) that is side-loaded 30∘30^\circ, its usable rating is 0.70×19.6=13.7 kN≥11.5 kN0.70 \times 19.6 = 13.7\text{ kN} \ge 11.5\text{ kN}, which is acceptable.

Anchors in Concrete (ACI 318, Chapter 17)

Cast-in anchors (headed studs, hooked bolts) and post-installed anchors (expansion, undercut and adhesive anchors) transfer machine-base loads into concrete. ACI 318 Chapter 17 requires checks of every failure mode and takes the lowest: steel strength in tension and in shear, concrete breakout (a cone-shaped failure whose projected area for a single anchor is 9hef29 h_{ef}^2, extending 1.5hef1.5 h_{ef} on each side of the anchor, where hefh_{ef} is the effective embedment depth), pullout, side-face blowout, bond failure for adhesive anchors, and concrete pryout in shear. Close edge distances and tight anchor spacing overlap the breakout areas and reduce capacity, which is why base-plate anchors are kept away from slab edges.


Worked Engineering Scenario: Drive Key & Clevis Pin Sizing

     Part 1: Shaft Drive Key                Part 2: Actuator Clevis Joint
     =======================                =============================
     Shaft Diameter: d = 2.00 in            Actuator Tension: P = 6,000 lbf
     Power: 50 hp @ 1,750 rpm               Double Shear Pin Sizing
     Key Material: AISI 1018 CD             Pin Material: AISI 1045 CD

Problem Statement

An electric motor drives an industrial centrifugal blower:

  • Part 1 (Drive Key): The motor delivers 50.0 hp50.0\text{ hp} at 1,750 rpm1,750\text{ rpm} through a solid shaft of diameter d=2.00 ind = 2.00\text{ in}. Size a standard square key made of AISI 1018 cold-drawn steel (Sy=54.0 kpsiS_y = 54.0\text{ kpsi}, Ssy=0.577Sy=31.16 kpsiS_{sy} = 0.577 S_y = 31.16\text{ kpsi}) using a design factor of safety n=2.0n = 2.0. Determine the minimum required key length LL for shear and bearing.
  • Part 2 (Clevis Pin): The blower throttle damper linkage is positioned by a hydraulic actuator exerting an axial tensile force of P=6,000 lbfP = 6,000\text{ lbf} on a clevis joint. The clevis pin is fabricated from AISI 1045 cold-drawn steel (Sy=77.0 kpsiS_y = 77.0\text{ kpsi}, Ssy=0.577Sy=44.43 kpsiS_{sy} = 0.577 S_y = 44.43\text{ kpsi}). Using a design factor n=2.5n = 2.5, size the clevis pin diameter dpd_p for double shear, and verify bearing stress on a tang of thickness ttang=0.625 int_{\text{tang}} = 0.625\text{ in}.

Step-by-Step Mathematical Solution

Part 1: Shaft Drive Key Sizing

  1. Calculate transmitted motor torque TT:
T=63,025×hpN=63,025×50.01,750=1,800.7 lbf⋅inT = \frac{63,025 \times \text{hp}}{N} = \frac{63,025 \times 50.0}{1,750} = 1,800.7\text{ lbf}\cdot\text{in}
  1. Sizing standard square key dimensions for d=2.00 ind = 2.00\text{ in}:
w=h=d4=2.00 in4=0.500 inw = h = \frac{d}{4} = \frac{2.00\text{ in}}{4} = 0.500\text{ in}
  1. Determine tangential force at shaft radius (r=1.00 inr = 1.00\text{ in}):
F=Td/2=1,800.7 lbf⋅in1.00 in=1,800.7 lbfF = \frac{T}{d/2} = \frac{1,800.7\text{ lbf}\cdot\text{in}}{1.00\text{ in}} = 1,800.7\text{ lbf}
  1. Required length for direct horizontal shear (n=2.0n = 2.0, Ssy=31,160 psiS_{sy} = 31,160\text{ psi}):
τallow=Ssyn=31,160 psi2.0=15,580 psi\tau_{\text{allow}} = \frac{S_{sy}}{n} = \frac{31,160\text{ psi}}{2.0} = 15,580\text{ psi} Lshear=Fwτallow=1,800.7 lbf0.500 in×15,580 psi=1,800.77,790=0.231 inL_{\text{shear}} = \frac{F}{w \tau_{\text{allow}}} = \frac{1,800.7\text{ lbf}}{0.500\text{ in} \times 15,580\text{ psi}} = \frac{1,800.7}{7,790} = 0.231\text{ in}
  1. Required length for compressive bearing (n=2.0n = 2.0, Sy=54,000 psiS_y = 54,000\text{ psi}):
σb,allow=Syn=54,000 psi2.0=27,000 psi\sigma_{b,\text{allow}} = \frac{S_y}{n} = \frac{54,000\text{ psi}}{2.0} = 27,000\text{ psi} Lbearing=F(h/2)σb,allow=1,800.7 lbf0.250 in×27,000 psi=1,800.76,750=0.267 inL_{\text{bearing}} = \frac{F}{(h/2) \sigma_{b,\text{allow}}} = \frac{1,800.7\text{ lbf}}{0.250\text{ in} \times 27,000\text{ psi}} = \frac{1,800.7}{6,750} = 0.267\text{ in}
  1. Summary and Specification: Compressive bearing governs, requiring L≥0.267 inL \ge 0.267\text{ in}. To ensure stable hub engagement and prevent key rocking, mechanical practice recommends L≥0.75d=1.50 inL \ge 0.75 d = 1.50\text{ in}. Specify a 0.500 in×0.500 in×1.50 in0.500\text{ in} \times 0.500\text{ in} \times 1.50\text{ in} square key.

Part 2: Actuator Clevis Pin Sizing

  1. Allowable shear stress for clevis pin (n=2.5n = 2.5, Ssy=44,430 psiS_{sy} = 44,430\text{ psi}):
τallow=Ssyn=44,430 psi2.5=17,772 psi\tau_{\text{allow}} = \frac{S_{sy}}{n} = \frac{44,430\text{ psi}}{2.5} = 17,772\text{ psi}
  1. Double shear equation for clevis pin under tensile load P=6,000 lbfP = 6,000\text{ lbf}:
τ=P2Apin=P2(πdp24)=2Pπdp2≤τallow\tau = \frac{P}{2 A_{\text{pin}}} = \frac{P}{2 \left(\frac{\pi d_p^2}{4}\right)} = \frac{2 P}{\pi d_p^2} \le \tau_{\text{allow}}
  1. Solve for required pin diameter dpd_p:
dp≥2Pπτallow=2×6,000 lbfπ×17,772 psi=12,00055,833=0.2149=0.4636 ind_p \ge \sqrt{\frac{2 P}{\pi \tau_{\text{allow}}}} = \sqrt{\frac{2 \times 6,000\text{ lbf}}{\pi \times 17,772\text{ psi}}} = \sqrt{\frac{12,000}{55,833}} = \sqrt{0.2149} = 0.4636\text{ in}

Select standard fractional pin diameter: dp=0.500 ind_p = 0.500\text{ in} (1/2 in1/2\text{ in}).

  1. Verify bearing stress on center tang (ttang=0.625 int_{\text{tang}} = 0.625\text{ in}):
σb,tang=Pdpttang=6,000 lbf0.500 in×0.625 in=6,000 lbf0.3125 in2=19,200 psi=19.2 kpsi\sigma_{b,\text{tang}} = \frac{P}{d_p t_{\text{tang}}} = \frac{6,000\text{ lbf}}{0.500\text{ in} \times 0.625\text{ in}} = \frac{6,000\text{ lbf}}{0.3125\text{ in}^2} = 19,200\text{ psi} = 19.2\text{ kpsi}
  1. Bearing factor of safety on tang (AISI 1018 steel, Sy=54.0 kpsiS_y = 54.0\text{ kpsi}):
nbearing=Sy,tangσb,tang=54.0 kpsi19.2 kpsi=2.81n_{\text{bearing}} = \frac{S_{y,\text{tang}}}{\sigma_{b,\text{tang}}} = \frac{54.0\text{ kpsi}}{19.2\text{ kpsi}} = 2.81

Because nbearing=2.81>2.5n_{\text{bearing}} = 2.81 > 2.5, the 0.500 in0.500\text{ in} pin and 5/8 in5/8\text{ in} tang assembly are fully verified against double shear and compressive bearing failure.

Test Your Knowledge

A standard square shaft key of width w = h = 0.50 in is machined from a ductile steel with yield strength S_y = 60 kpsi. Assuming the Distortion Energy theory governs shear yield (S_sy = 0.577 S_y), how do the theoretical minimum key lengths required to resist direct shear (L_shear) and compressive bearing (L_bearing) compare under an applied torque T?

A

The key will always fail in shear first, requiring a length L_shear that is twice as long as L_bearing.

B

Bearing needs a slightly longer key (L_bearing = 1.155 L_shear), because only h/2 of the key height carries bearing.

C

Direct shear and compressive bearing require mathematically identical lengths because w = h.

D

Compressive bearing cannot cause failure in a ductile key because hydrostatic triaxial stress completely prevents yielding.

Test Your Knowledge

When an external retaining ring (snap ring) installed on a rotating shaft experiences an axial thrust load from a mounted bearing, what failure mode is triggered if the bearing inner ring features a large corner chamfer or radius?

A

Centrifugal forces cause the retaining ring to expand radially and fly completely off the shaft.

B

Fretting corrosion between the snap ring and groove rapidly welds the two components together.

C

An eccentric prying moment dishes the ring out of its groove, sharply cutting its thrust capacity.

D

The groove undergoes spontaneous hydrogen embrittlement caused by localized contact friction heating.

Test Your Knowledge

A clevis joint connecting a hydraulic actuator rod to a machine frame is subjected to a pure tensile force P. Which of the following correctly describes the stress state and cross-sectional area evaluated when checking the clevis pin for direct shear failure?

A

Double shear: two transverse cross sections (total area 2 * pi * d^2 / 4) resist the load, so tau = 2P / (pi * d^2).

B

The pin is in single shear, meaning one cylindrical cross section resists the load, yielding shear stress tau = 4P / (pi * d^2).

C

The pin experiences pure torsional shear along its longitudinal centerline, with shear stress tau = 16P / (pi * d^3).

D

The pin resists shear through its projected diametral area d * t, yielding shear stress tau = P / (d * t).

Test Your Knowledge

A screw-pin anchor shackle has a rated load (working load limit) of 4.0 metric tons. In service it will be side-loaded at 40 degrees from its in-line axis. According to the ASME B30.26 side-loading table, what is the maximum load the shackle may carry?

A

2.8 t, because side loading between 6 and 45 degrees reduces the rated load by 30%

B

4.0 t, because side loading only matters above 45 degrees

C

2.0 t, because any side loading halves the rated load

D

3.1 t, because the rating scales with the cosine of the side-load angle

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