24-57 F2 the component of force acting on the driven Geneva wheel shaft due to the torque M2t, kN lbf Fig.. 24-57 F2ðmaxÞ maximum force pressure at the point of contact between the roll
Trang 1For external ratchet
For internal ratchet
The ratio of a=d (internal ratchet)
The module
The bending moment on pawl
The bending stress
The diameter of pawl pin
2þ th
s
ð24-272Þwhere th¼ thickness of hub on pawl
Trang 224.9 GENEVA MECHANISM
a¼ r1
sin center distance, m (in)
F1 the component of force acting on the crank or the driving shaft
due to the torque, M1t, kN (lbf ) (Fig 24-57)
F2 the component of force acting on the driven Geneva wheel shaft
due to the torque M2t, kN (lbf ) (Fig 24-57)
F2ðmaxÞ maximum force (pressure) at the point of contact between the
roller pin and slotted Geneva wheel, kN (lbf )
FðmaxÞ the component of maximum friction force at the point of
contact due to the friction torque M2t, on the driven Genevawheel shaft, kN (lbf )
FiðmaxÞ the component of maximum inertia force at the point of contact
due to the inertia torque on the driven Geneva wheel shaft,
kN (lbf )
i¼z 2
J polar moment of inertia of all the masses of parts attached to
Geneva wheel shaft, m4(in4)
k the working time coefficient of the Geneva wheel
M1t total torque on the driver or crank, N m (lbf in)
M2t total torque on the driven or Geneva wheel, N m (lbf in)
M2ti inertia torque on the Geneva wheel, N m (lbf in)
M2t friction or resistance torque on Geneva wheel, N m (lbf in)
r1 radius to center of driving pin, m (in)
r2 radius of Geneva wheel, m (in)
r02 distance of center of semicircular end of slot from the center of
Geneva wheel, m (in)
ra outside radius of Geneva wheel, which includes correction for
finite pin diameter, m (in)
rp pin radius, m (in)
Rr¼r2
r1 radius ratio
t total time required for a full revolution of the driver or crank, s
ti time required for indexing Geneva wheel, s
tr time during which Geneva wheel is at rest, s
z number of slots on the Geneva wheel
crank angle or angle of driver at any instant, deg (Fig 24-54)
2a angular acceleration, m/s2(ft/s2)
angular acceleration of Geneva wheel, m/s2(ft/s2)
m angular position of the crank or driver radius at which the
product! 2a is maximum, degangle of the driven wheel or Geneva wheel at any instant, deg
(Fig 24-54)
¼r1
a the ratio of the driver radius to center distance
efficiency of Geneva mechanism
Trang 3locking angle of driver or crank, rad or deg
ratio of time of motion of Geneva wheel to time for one
revolution of driver or crank
¼360
2z semi-indexing or Geneva wheel angle, or half the anglesubtended by an adjacent slot, deg (Fig 24-54)
crank or driver angle, deg (Fig 24-54)
! ¼2n
60 angular velocity of driver or crank (assumed constant), rad/s
!1,!2 angular velocities of driver or crank and Geneva wheel,
FIGURE 24-54 Design of Geneva mechanism.
The angular velocity (constant) of driver or crank
Gear ratio
The semi-indexing angle or Geneva wheel angle or
half the angle subtended by two adjacent slots
The angle through which the Geneva wheel rotates
EXTERNAL GENEVA WHEEL
The angle of rotation of driver through which the
Geneva wheel is at rest or angle of locking action
Trang 4The center distance (Fig 24-55)
The radius ratio
The ratio of crank radius to center distance
The relation between crank angle and Geneva wheel
angle
VELOCITY
The angular velocity of the Geneva wheel
The maximum angular velocity of Geneva wheel at
!2¼ sinð=zÞðcos sin =zÞ
1 2 sinð=zÞ cos þ sin2=z!1 ð24-283bÞ
!2ðmaxÞ¼
ddt
max
1 !1
¼
sinz
1 sinz
FIGURE 24-55 External Geneva mechanism.
Trang 5The angular acceleration,a 2a, of Geneva wheel
For angular velocity and angular acceleration curves
for three-slot external Geneva wheel with driver
velocity,!1¼ 1 rad/s
The maximum angular acceleration of Geneva wheel
which occurs at ¼ ðmaxÞ
The angular acceleration of Geneva wheel at start and
a 2a¼ sinð=zÞ cos2ð=zÞ sin
1 2 sinð=zÞ cos þ sin2ð=zÞ!
2ð24-284bÞRefer to Fig 24-56
cos ðmaxÞ¼ þpffiffiffiffiffiffiffiffiffiffiffiffiffi2þ 2 ð24-284cÞwhere
¼14
0 0
10
20
30
2 4 6
Trang 6The ratio of tito t
The ratio of trto t
The sum of angles of ( þ )
The time required for indexing Geneva wheel, in
seconds
The time during which Geneva wheel is at rest, in
seconds
The working time coefficient of Geneva wheel
Ratio of time of motion of Geneva wheel to time for
one revolution of crank or driver
The required speed of the driver shaft or crankshaft
SHOCK OR JERK
The jerk or shock, J2, on Geneva wheel
The jerk or shock at ¼ 0
The jerk or shock at start, i.e.,
The length of the slot (Fig 24-54)
The condition to be satisfied by diameter on which the
driver or crank is mounted
The condition to be satisfied by the diameter on which
Geneva wheel is mounted
z
602n
ð24-290Þ
tr¼zþ 2z
602n
<12
ð24-293Þ
n¼zþ 2z
602tr
ð24-294Þwhere n in rpm
zþ cos
z 1
ð24-298Þ
d1< 2a3¼ 2ða r2Þ ¼ 2a
1 cosz
ð24-299Þor
d1
a < 2
1 cosz
ð24-301Þ
Trang 7TORQUE ACTING ON SHAFTS OF
GENEVA WHEEL AND DRIVER
The total torque acting on Geneva wheel shaft
The torque on the shaft of crank or driver
The efficiency of Geneva mechanism
INSTANTANEOUS POWER
The instantaneous power on the crank or driving
shaft
Calculation of average power
The average torque MtiðavÞfor complete cycle
The average torque for first half-cycle
¼ 0.80 to 0.90 when Geneva wheel shaft
is mounted on journal bearings (24-304a)
¼ 0.95 when drive shaft is mounted onrolling contact bearings (24-304b)
¼ 0.75 when the diameter of bearingsurface is larger than the outsidediameter of Geneva wheel (24-304c)
P¼ Mt!
75 103 Customary Metric ð24-305cÞwhere P in hpm, Mtin kgf mm, and! in rad/s
Trang 8The average power required on the crank or driving
shaft
Calculation of maximum power
The maximum torque on the driven shaft of Geneva
FIGURE 24-57 Forces acting on Geneva wheel.
The maximum power required on the shaft of the
Pav¼MtðavÞn
where Pavin hp, MtðavÞin lbf in, and n in rpm
M2tðmaxÞ¼ M2tþ M2tiðmaxÞ ð24-309Þwhere M2tis constant
M2tiðmaxÞ¼ J 2aðmaxÞ¼J 2aðmaxÞ
!2
2n60
Trang 9FORCES AT THE POINT OF CONTACT
(Fig 24-57)
The maximum force at the point of contact between
the roller pin and slotted Geneva wheel
The component of maximum friction force at the
point of contact due to the friction torque M2t on
the driven Geneva wheel shaft
For maximum values of F2i
For design data for external Geneva mechanism
INTERNAL GENEVA WHEEL
The time required for indexing Geneva wheel, s
The time during which Geneva wheel is at rest, s
The ti=t ratio
The tr=t ratio
The working time coefficient of Geneva wheel
The relationship between crank or driver angle and
Geneva wheel angle
¼r1
ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi
1 2 cos þ 2q
Refer to Table 24-25A
ti¼zþ 2z
602n
ð24-314Þ
tr¼z 2z
602n
Trang 10The angular velocity of Geneva wheel
The maximum angular velocity of Geneva wheel
The angular acceleration, 2a, of Geneva wheel
For values of 2aat start and finish of indexing
For curves of angular velocity and angular
accelera-tion of internal Geneva wheel
The contact forces between the slotted wheel and the
pin on the driving crank of the internal Geneva wheel
are calculated in a manner similar to that for the
external Geneva wheel
Materials
Chromium steel 15 Cr65case-hardened to Rc58 to 65
is used for the roller pin on the driver or crank
Chromium steel 40 Cr 1 hardened and tempered to Rc
45 to 55 is used for the sides of slotted Geneva wheel
0 0.2 0.4 0.6 0.8
FIGURE 24-58 Angular velocity and angular acceleration for four-slot internal Geneva wheel.
Trang 1124.10 UNIVERSAL JOINT
Kct correction factor to be applied to torque to be transmitted
Kct correction factor to be applied to power to be transmitted
l length (also with subscripts), m (in)
Mt torque to be transmitted by universal joint, N m (lbf in)
Mtd design torque, N m (lbf in)
P power to be transmitted by universal joint, kW (hp)
Pd design power, kW (hp)
angle between two intersecting shafts 1 and 2, deg
angle of rotation of the driver shaft 1, deg
angle of rotation of the driven shaft 2, deg
!1,!2 angular velocities of driver and driven shafts respectively, rad/s
SINGLE UNIVERSAL JOINT (Figs 24-59 and
24-61a)
The relation between
The relation between the angular velocities of driving
shaft 1 or driver (!1) to the driven shaft 2 or the
Trang 12The maximum value of!2=!1
The minimum value of!2=!1
The angular acceleration of the driven shaft 2, if!1is
constant
The value of for which the angular acceleration of
the driven shaft is maximum
The power transmitted by universal joint
The design torque of universal joint
The design power of universal joint
For calculation of torque and power transmitted by
universal joint for various angles of inclination
For design data of universal joint
DOUBLE UNIVERSAL JOINT (Figs 24-60
and 24-61b)
The angular velocities ratio for a double universal
joint which will produce a uniform velocity ratio at
all times between the input and output ends
!2
!1
max¼ cos
ð24-326Þwhen sin¼ 0, i.e., ¼ 0, , 2, etc
d2
dt2 ¼d!2
dt ¼ cos 2ð1 sin2 sin2 2!2 ð24-327Þcos 2ðmaxÞ¼ pffiffiffiffiffiffiffiffiffiffiffiffiffi2þ 2 ð24-328Þwhere ¼ ð2 sin2 2
The angular acceleration of driven shaft is maximumwhen is approximately equal to 458, 1358, etc., whenthe arms of cross are inclined at 458 to the planecontaining the axes of the two shafts
Trang 13(b) Double universal joint
di = 10 to 50 (a) Single universal joint di = 6 to 50
Trang 14FIGURE 24-62 Angle between two intersecting
shafts vs correction factor (Kct).
Angle of inclination (β), deg 0
0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0
Trang 15d i×d o
325 rpm
FIGURE 24-65(a) Design curves for single universal joint with plain bearings for
Trang 16USE OF CURVES IN FIGS 24-62 TO 24-65
Worked example 1
A single universal joint has to transmit a torque of
10 kgf m at 1500 rpm The angle between intersectingshafts is 258 The joint is subjected to a minorshock The shock factorðKsÞ is 1.5 Design a universaljoint with needle bearings for a life of 800 h.SOLUTION From Fig 24-62 correction factor for
is Kct¼ 1:2 Design torque¼ Mtd
¼ MtKsKct¼ 10 1:5 1:2 ¼ 18 kgf m (176.5 N m).Speed life ¼ nL ¼ 1500 800 ¼ 120 104rpm h.From Fig 24-64 for Mtd¼ 18 kgf m (176.5 N m) and
nL¼ 120 104rpm h, the size of a single universaljoint isðdi doÞ 40 75 mm
Worked example 2
Design a single universal joint with plain bearings totransmit 2 kW power at 325 rpm The angle betweentwo intersecting shafts is 27.58
SOLUTION From Fig 24-63 correction factorfor CN¼ 0:35 Design power ¼ Pd
¼ ðP=KCNÞ ¼ ð2=0:35Þ ¼ 5:7 kW From Fig 24-65athe size of a single universal joint for Pd¼ 5:7 kWand speed¼ n ¼ 325 rpm is ðdi doÞ 40 75 mm.The permissible torque for this size of joint(Fig 24-65a) is 17.5 kgf m (171.5 N m)
Maximum allowable rotational play Test torque Angular rotational play Tolerance on
FIGURE 24-65(b) Taper pin joint The length of the taper
pin should conform to diameter doin Table 24-25B.
Trang 1724.11 UNSYMMETRICAL BENDING AND
TORSION OF NONCIRCULAR CROSS-SECTION
MACHINE ELEMENTS
a semimajor axis of elliptical section, m (in)
width of rectangular section, m (in) (in2)
A area of cross section, m2(in)
b semi-minor axis of elliptical section, m (in)
height of rectangular section, m (in)
c distance of the plane from neutral axis, m (in)
thickness of narrow rectangular cross section (Fig 24-68)
e the distance from a point in the shear center S (Table 24-26)
G modulus of rigidity, GPa (MPsi)
I moment of inertia, area (also with suffixes), m4(cm4) (in4)
Iu, Iv moment of inertia of cross-sectional area, respectively, m4
(cm4) (in4)
Jk polar moment of inertia, m4(cm4) (in4)
k1, k2 constants from Table 24-28 for use in Eqs 343) and
(24-344)
Mb bending moment, N m (lbf ft)
Mt twisting moment, N m (lbf ft)
Mbu¼ Mbcos bending moment about the U principal centroidal axis or any
axis parallel thereto
Mbv¼ Mbsin bending moment about the V principal centroidal axis or any
axis parallel thereto
Q the first moment of the section, m4(cm4) (in4)
S the length of the center of the ring section of the thin tube, m
(in)
t width of cross section at the plane in which it is desired to find
the shear stress, m (in)thickness of the wall of the thin-walled section, m
u, v coordinates of any point in the section with reference to
principal centroidal axes
V shear force on the cross section, kN (lbf)
Vy resultant shear force acting at the shear center, kN (lbf)
x the distance of the section considered from the fixed end (Fig
24-73)
x, y coordinates in x and y directions
b bending stress (also with suffixes), MPa (psi)
shear stress (also with suffixes), MPa (psi)
variable thickness of thin tube wall (Fig 24-70), m (in)
angle measured from the V principal centroidal axis, deg
Trang 18For the equations for locating the shear centers of
various thin open sections
ELLIPTICAL CROSS SECTION
Shear stress acting in the x direction on the xz plane
(Fig 24-66)
Shear stress acting in the y direction on the yz plane
(Fig 24-66)
Maximum shear stress on the periphery at the
extremities of the minor axis (Fig 24-66 and Table
24-27)
Minimum shear stress on the periphery at the
extremities of the major axis
Angle of twist (Fig 24-66)
ða2þ b2Þ
Trang 19lRECTANGULAR CROSS SECTION
The maximum shear stress at point A on the
boundary, close to the center (Fig 24-67 and Table
24-27)
Angle of twist (Table 24-27)
NARROW RECTANGULAR CROSS
SECTIONS (Fig 24-68)
Equation for twisting moment (Fig 24-68)
Equation for angle of twist
The maximum shear stress
x y
b
FIGURE 24-67
Trang 20TABLE 24-26
Location of shear center for various cross sections
vy
t f
t f e
x t1 t2
L = Length of Dotted line s
e
x tb th
vy y
ð > 128Þ approx.
Trang 21TABLE 24-26 (Cont.)
Location of shear center for various cross sections
Section Location of shear center Section Location of shear center
b2 e2
e 1 vx
d
C t h
Trang 22TABLE 24-27
Approximate formulas for torsional shearing stress and angle of twist for various cross sections
Shearing stress, lbf/in2 Angle of twist per unit length ,
Trang 23Equation for torque for a cross-section composed of
several narrow rectangles (Table 24-27)
Angle of twist for a cross section composed of several
narrow rectangles
Maximum shear stress
For approximate formulas for torsional shearing
stress and angle of twist for various cross sections
For variation of stress-concentration factor K with
ratio r=c for structural angle (Fig 24-69)
Trang 24HOLLOW THIN-WALLED TUBES
(Fig 24-70)
The equation for the twisting moment
The angle of twist
By membrane analogy the value ofÞ
ds
The equation for the shear stress
The difference in level between DC and AB of
membrane
The equation for twisting moment of thin webbed
tubes (or box beams) (Fig 24-71)
The equations for shear stress
x
S 0
FIGURE 24-70
Trang 25BENDING STRESSES CAUSED BY
TORSION
Torsion of I-beam having one section
restrained from warping
The lateral bending moment in the flanges of an
I-beam subjected to twisting moment at one end, the
other end being fixed, Fig 24-72
The maximum bending moment for long beam
Twisting moment at any section, distance x from the
fixed end
The angle of twist per unit length
The total angle of twist at the free end
Maximum bending moment
C B
Trang 26The angle of twist at free end if l=k > 2:5
The maximum bending moment if l=k > 2:5
The bending stress
For beams subjected to torsion
TRANSVERSE LOAD ON BEAM OF
CHANNEL SECTION NOT THROUGH
SHEAR CENTER (Fig 24-73)
t
F e
s Shear centre b
FIGURE 24-73
Trang 27The direct stress
The bending stress
The maximum longitudinal stress (Fig 24-73b)
For geometrical properties, weight, and nominal
dimensions of beams, channels, T-bars, and equal
and unequal angles
t¼MI
Refer to Tables 24-31 and 24-32 and Figs 24-74 to24-79
Trang 28TABLE 24-30
Formulas for maximum lateral bending moment and angle of twist of beams subjected to torsiona
Maximum lateral bending moment in Type of loading and support flange, lbf in (N m) Angle of twist of beam of length L, rad
L
MbðmaxÞ¼Mt k
2h
cot hL2k 2kL
¼Mt 2JG
L
e w
k Lk
¼Mt JG
L
¼12Mt JG
L
2 k tan h2kL
ðapprox:Þ
a
Formulas given in Table 24-30 can also be used for Z and channel sections.
Trang 364 Lingaiah, K., Machine Design Data Handbook, McGraw-Hill Publishing Company, New York, 1994.
5 Maleev, V L., and J B Hartman, Machine Design, International Text book Company, Scranton,Pennsylvania, 1954
6 Black, P H., and O E Adams, Jr., Machine Design, McGraw-Hill Book Company Inc., New York, 1968
7 Neale, M J., Tribology Handbook, Newnes-Butterworth, London, 1973
8 Bach, Maschinenelemente, 12th ed., P-43
9 Heldt, P M Torque Converters for Transmissions, Chiltan Company, Philadelphia, 1955
10 Newton, K., and W Steeds, The Motor Vehicle, Iliffe and Sons Ltd, London, 1950
11 Steeds, W., Mechanics of Road Vehicle, Iliffe and Sons, Ltd., London, 1960
12 Arkhangelsky, V., et al., Motor Vehicles Engines, Mir Publisher, Moscow, 1971
13 Heldt, P M., High Speed Combustion Engines, 6th ed., Chilton Company, Philadelphia, 1955
14 Thimoshenko, S., and J N Goodier, Theory of Elasticity, McGraw-Hill Book Company, Inc., andKogakkusha Company Ltd., Tokyo, 1951
15 Timoshenko, S., and S Woinowsky-Krieger, Theory of Plates and Shells, McGraw-Hill Book Company, Inc.,New York, 1959
16 Seely, F B., and J O Smith, Advanced Mechanics of Materials, John Wiley and Sons, Inc., 2nd ed., 1959
17 Timoshenko, S., and J M Gere, Mechanics of Materials, Von Nostrand Reinhold Company, New York,1972
18 Goetze, A G Piston Ring Manual, 3rd ed., Burscheid, Germany, 1987
19 Bureau of Indian Standards, New Delhi, India
Trang 37B width of V or U die, m (in)
c chisel edge length, m (in)
d diameter of the hole, m (in)
diameter of the drill, m (in)
depth of cut, m (in)
diameter of milling cutter, m (in)
shell diameter, m (in)
Dm diameter of machined surface, m (in)
Dw diameter of workpiece or job, m (in)
E Young’s modulus, GPa (kpsi)
work done in punching or shearing of material, N m (lbf ft)
work done per unit volume of removed, J/mm3
Fa¼ Fx axial component of cutting force, kN (lbf )
Fc cutting force, kN (lbf )
Fhc normal cutting force or the resultant force on a
single point metal cutting tool in the horizontal plane,
kN (lbf )
Fmax maximum force at the punch, kN (lbf )
Fn force normal to F, kN (lbf )
Fn force normal to shear force, kN (lbf )
Fr reaction of the cutting force, kN (lbf )
radial component of the cutting force, kN(lbf )
FR resultant cutting force, kN (lbf )
Fs stripping pressure, kN (lbf )
Ff ¼ Fx feed force, kN (lbf )
Ft¼ Fz¼ Fc tangential component of the cutting force, kN(lbf)
Fy¼ Fr radial component of the cutting force, kN (lbf )
F frictional force on tool face, kN (lbf )
F¼ Fr frictional force of the saddle on lathe bed, kN (lbf )
Trang 38F shear force kN (lbf )
shell height, m (in)
hc height of the lathe center, m (in)
hsw swing over the bed of the lathe, m (in)
K constant of proportionality in Eq (25-31)
coefficient, also with subscripts
L length of cut or perimeter of the cut, m (in)
Lm length of job, m (in)
Pc power at cutting tool, kW (hp)
Pg gross or motor power, kW (hp)
Pf tare power, that is the power required to run the machine at no
load, kW (hp)
Pu¼ Ps unit power or specific power, kW (hp)
Q metal removal rate, cm3/min (in3/min)
rc corner radius, m (in)
rc¼ ðt1=t2Þ cutting ratio
rn nose radius, m (in)
R roughness height,m m (m in)
Ri inside radius of bend, m (in)
s feed rate, mm/rev (in/rev)
sz feed per tooth of milling cutter, mm/tooth
t thickness of material to be punched or sheared, m (in)
thickness of chip, m (in)
depth of cut, m (in)
t1 initial thickness of the chip, m (in)
t2 final thickness of the chip, m (in)
uc number of chamfered threads
v velocity, m/s (ft/min)
vc cutting speed, m/min (ft/min)
vf feed rate, mm/min (in/min)
V cutting velocity, m/min (ft/min)
W work done per unit volume, N m/m3(lbf ft/ft3)
x, v, z machine reference co-ordinate axes
z number of teeth on milling cutter
relief or clearance angle, deg
f side relief or clearance angle, deg
n normal relief or clearance angle, deg
o orthogonal clearance angle, deg
p front or end relief or clearance angle, deg
tr true relief or clearance angle, deg
Trang 39helix angle, deg
rake angle, also with subscripts, deg
f side rake angle, deg
n normal rake angle, deg
o orthogonal rake angle, deg
p back rake angle, deg
gullet angle, deg
" peripheral pitch angle, deg
wedge angle, also with subscripts, deg
chip flow angle, deg
approach angle in Eq (25-104b), deg
c corner angle in Eq (25-104a)
s inclination angle, deg
coefficient of friction
stress, also with suffices, MPa (kpsi)
c compressive stress, MPa (kpsi)
sut ultimate tensile strength, MPa (kpsi)
y yield stress, MPa (kpsi)
shear stress, MPa (kpsi)
nð¼ suÞ resistance of the material to shearing or the ultimate shearing
strength, MPa (kpsi)cutting edge angle, also with subscripts, deg
shear angle, deg
o end cutting edge angle, deg
p principal cutting edge angle, deg
s side cutting edge angle, deg
engagement angle for milling depth, deg
Note: and with subscript s designates strength properties of material used in
the design which will be used and observed throughout this Machine Design Data
Handbook
Other factors in performance or in special aspects are included from time to
time in this chapter and, being applicable, only in their immediate context, are
not given at this stage
Trang 4025.1 METAL CUTTING TOOL DESIGN
25.1.1 Forces on a single-point metal cutting
tool
Nomenclature of metal cutting tool
The normal cutting force or resultant force on a
single-point metal cutting tool in horizontal plane
q
ð25-1Þ
FR¼ ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiF2
t þ F2 hc
Face Major flank
Major cutting edge
FIGURE 25-1 Nomenclature of metal cutting tool.
F r (=F y ) = radial force
F t or F c (=F x ) = tangential cutting force
F R = resultant cutting force on the cutting tool
D w
D m x
...Note: and with subscript s designates strength properties of material used in
the design which will be used and observed throughout this Machine Design Data
Handbook
Other... class="text_page_counter">Trang 40
25.1 METAL CUTTING TOOL DESIGN< /h3>
25.1.1 Forces on a single-point metal cutting
tool
Nomenclature