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Pressure Vessels and Shrink Fits

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PRESSURE VESSELS AND SHRINK FITS THIN-WALLED PRESSURE VESSELS If the wall thickness is = – PowerPoint PPT presentation

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Title: Pressure Vessels and Shrink Fits


1
Pressure Vesselsand Shrink Fits
2
Thin-Walled Pressure Vessels
  • If the wall thickness is lt 1/10 the inner
    radius, the vessel may be considered thin-walled.
  • In thin walled pressure vessels, the inner and
    outer radii are set equal to r, and the thickness
    is t.

3
Thin-Walled Pressure Vessels
  • The stress is assumed to be uniform throughout
    the thickness. Usually only two stress
    components are significant, axial and tangential.

4
Thin-Walled Stresses (Review)
  • Axial, or longitudinal stress, is
  • Circumferential, or tangential stress, is

(also for a sphere)
5
Thin-Walled Stresses (Review)
  • Stress in the radial direction, ?r, varies
    from -p (p pressure) at the interior of the
    vessel to zero at the exterior (for internally
    pressurized vessels). ?r is usually ltlt than
    either ?? or ?a, and is usually neglected.

6
Thick-Walled Pressure Vessels
  • Thick-walled vessels often operate under much
    higher pressures than thin-walled, and the radial
    stress component cannot usually be ignored.
  • Stresses vary through the wall thickness, unlike
    the assumption for thin-walled vessels.

7
Thick-Walled Nomenclature
a inside radius b outside radius r
arbitrary radius u radial displacement pi
inside pressure po outside pressure ?r radial
stress ?? tangential stress ?z axial stress
8
Thick-Walled, Internal Pressure (po 0)
?? is gt ?r. Note variation with r.
9
Thick-Walled, Internal Pressure
Notes ?r is always compressive max. at r a.
(max at i.d.) ?? is always tensile, also max. at
r a.
10
Thick-Walled, External Pressure (pi 0)
11
Thick-Walled, External Pressure
Notes ?r is always compressive max. at r b.
(max. at o.d.) ?? is also compressive, max. at r
a.
12
Thick-Walled, Axial (or Longitudinal) Stress
?z (pia2 pob2)/(b2 a2)
(For either internal or external pressure)
13
Uses for Thick-Walled Equations
  • Use is for high pressures in a thick walled
    vessel. Straightforward application of formulas.
  • A second use is in the calculation of shrink
    fits, either for assembly or to create very
    strong composite structures. In these cases, the
    contact pressure p between the parts, is treated
    as po or pi in the preceding equations.

14
Shrink Fit Nomenclature
15
Determining Contact Pressure, p
  • In many cases, the designer may choose a
    maximum tangential stress ??. Then, p may be
    solved for (as pi for the hub) using

Watch your as, bs, and cs!
16
Determining Contact Pressure, p
  • Otherwise, the designer may choose to specify
    an interference ?, or the contact pressure p
    itself and then solve for the necessary ? to
    achieve that p.

17
Contact Pressure
If the hub shaft are of the same material, this
condenses to
18
Shrink Fits
  • Once p is determined, assume a friction factor
    f usually 0.15 lt f lt .20. The assembly force F
    to assemble a shrink-fit assembly is given by
    Eq.
  • F 2?bpfL, where L is the length of the fit.
  • Holding Torque T is given by
  • T Fb 2 ?b2fpL

19
Press Fit, Example Steel Shaft Press Fit Onto
Cast Fe Disc
a 25mm b 50 mm c 125 mm L 100 mm Es 210
Gpa ?s .3 Eh 70 Gpa ?h .25
Assumptions max. tangential stress NTX 30 MPa,
contact pressure is uniform, and f 0.15. FIND
radial interference ?, assembly force, torque
capacity.
20
Flywheels
21
Flywheels
  • A flywheel is a typically a disc which rotates
    on a shaft. They are used to smooth out small
    oscillations and to store energy (kinetic energy
    of rotation). Examples cars, hybrids, punch
    press

22
Flywheels
  • Design and analysis is similar to what we have
    covered. An added component is consideration of
    the radial forces developed by the rotation a
    term of ??2 is introduced.
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