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发表于 2008-3-28 09:07:19
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来自: 中国天津
线性静力分析:定义专题: H/ Q- b! `+ ]9 B* F% z& ` x" m
Displacement in the radial direction:; S* k$ \ X+ J- O: G
Select “Axis1” and then define displacement plot in X-direction (radial to the axis). Select deformation scale=17 ?. m5 Y w/ f; [% [% u- X, |$ Z
Right-click on the displacement plot icon “plot2” and then select”List selected”9 V- C* g/ F0 P) |9 Y3 _1 ~
Average displacement of “pole piece lower” = -0.0019504” (decrease in radius)3 w7 v# Q4 u) k2 b
Average displacement of “pole piece upper” = 0.007896 “ (increase in radius)1 `$ p( ^( T$ o% M+ Q
Sum of these 2 displacement = 0.009846” ~Initial interfernce of 0.01”
6 J2 ?+ `- x$ w( |Hoop Stress (tangential):
. }8 ~5 I, v. bSelect “Axis1” and then define stress plot in Y-direction (radial to the axis). Select deformation scale=1
, s* [7 _& G4 MRight-click on the stress plot icon “plot2” and then select”List selected”' ?% y2 W' g6 Q( P
Negative stress on “pole piece lower” (compression)
+ d- \# j A% g) R$ r* P, y* HPositive stress on “pole piece upper” (tension)
! {% s! _7 g: s- ?线性静力分析:定义材料属性( Y' w4 P, a# H! K
Simulate parts which are separated by large gaps
. }. ]$ o, p% p$ ]4 `+ _6 N( rFirst run the model with small displacement option and look at the results
9 v$ j3 R6 y/ x; M/ O If you see that there is a change in the orientation of the contact surfaces during loading or if the results doesn’t look realistic, use large deflection option: Q' _$ d4 S7 y4 `7 ^" R& l
& z9 ~! N# U2 K, `3 } L线性静力分析:网格划分
& c+ z8 G4 y+ X. H3 dOpen “RectangleGap.sldasm”) J5 R ]- P% w0 V
Define a static study “smallcontact”+ o3 p6 g5 N. W- ^) B( y, a+ a
Apply material “Alloy steel” to both parts! o' G# u1 m, D3 T! Z' H
Apply a pressure of 725 psi on the top face: |0 C# ]7 p0 d1 u3 g0 j/ Q* g
Select the two front faces and then apply restraint. Select Flat face option and then select “Normal to face”
4 [6 Y5 ~: B% P- pFix the left semi-circular face
5 ]% r. }+ p5 XHide the loads/bc symbols
) P& K" `: u: R: O, a, [Define “Surface” contact between the top face of the bottom leg and the perpendicular face
" b+ k4 G7 A) Q9 jCreate mesh and run
: z) X- e# s8 z' b9 K% iDefine a stress plot with scale factor = 1. Look at the contact surface. - E2 ^8 d& J) A+ L. j: S* z
线性静力分析:定义约束0 o/ U4 A% p2 ~, G/ [
Define a new static study “LargeDisp”
, z) d( @9 G# f8 RDrag’n drop the material and loads/bc folders from “small contact” study9 {5 b3 N6 ]% |& I, ^
Right-click on the study name and click on properties. Select “Large displacement contact” option.
8 R: s; O0 Y* w! V& |7 k7 B0 `5 j" ZRun the analysis2 I/ ]% i8 Q9 d' v
Define a stress plot with scale factor = 1. Look at the contact area.
4 o) a1 P ~" W线性静力分析:定义载荷
! z" V4 v4 `: Y; QSimulate heat resistance between parts for thermal analysis
/ U/ b' u# {6 w3 o! y8 n' q Account for heat resistance of thin parts without actually modeling them!- q0 b$ j: F3 N* \6 f* m' C5 d
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线性静力分析:求解+ S. _0 e2 @, ^
Open “Thermal contact resistance_transistor.sldasm”3 F# [8 `, L1 G& Q; Z/ ^
Explode the model and set preferred units to “SI” and temperature units to “Kelvin”
6 s5 j$ c0 O/ A) KDefine a thermal study “NoRes”
; S8 D8 Y3 n8 J1 dApply material “AISI 304” for “Voltage regulator” and “Copper” for Heat sink6 K" ~8 {. j* O7 t7 T8 e, ^
Define “Surface” contact with No resistance between the contact faces/ N# a6 h( G2 y( {- d
Apply convection to all the faces of the model except the contact faces7 X: ?; M$ W) T" u/ ^9 ^
Film coefficient = 250 W/(m^2.K)
! h: [1 J, ~8 h5 D# [# |3 H4 iBulk temperature = 298 K$ O9 D0 H. U; q! |+ e: W
线性静力分析:观察结果
& M0 b; @! G2 O) }: cApply Heat power = 25 W for “Voltage regulator”
$ ?/ M+ H l9 C9 XMesh with default settings and run the analysis
9 u* y+ j' w" e/ z9 fNotice the temperature distribution of the heat sink
: t5 o" I+ _% r7 m& lDistributed Resistance:
& F+ C5 m7 ?! Q, {1 x' k7 dDefine a new thermal study “DistRes”
% x3 A$ `2 y4 y! z2 B! Q1 A4 hDrag’n drop “Material” folder and Loads/Bc folder from NoRes study to DistRes study
% u: b3 ?3 ~- I$ LEdit contact pair definition and define distributed resistance = 0.005 K.m^2/W
" A: K/ G' Y# H" gTotal resistance = Distributed resistance X Contact area = 0.005 X 0.0003392 = 14.7 K/W
( t: |8 s* ^) R6 x5 g( `Run the study “DistRes”
: d% u9 [+ R, ^1 a( X% }- MNotice the temperature distribution of the heat sink
' z8 \/ u8 l6 [# hThermal Contact Example (Cont’d)
% R8 y" ?- n5 c5 U! NProbe the temperature value* n# h* K: \8 n1 g% W$ C$ \
Define a thermal plot with mesh
! @) y: o3 M/ z- B+ aRight-click the plot icon and select Probe$ _" X5 V$ ?5 b& u2 ~
Pick all the nodes on the edge of both the parts# Y0 m8 E' X9 z/ i6 P [# M
Click on the Plot icon to view the temperature variation from the top face of the voltage regulator to the bottom of the heat sink! B5 G2 W/ D, F3 J, [
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Thermal Contact Example (Cont’d)4 `; {4 ~( U ~4 b; {4 j
Total Resistance:- X( X& w w5 L \4 Y$ A
Define a new thermal study “TotalRes”
4 Q |* U$ ?! {3 A* y5 \Drag’n drop “Material” folder and Loads/Bc folder from NoRes study to TotalRes study& e+ e9 T1 e a
Edit contact pair definition and define Total resistance = 25 K/W $ |$ b" ^2 }8 C
Run the study “TotalRes”; W4 u0 ?! t( n2 w( C' V1 W
Notice the temperature distribution of the heat sink
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Load Simulation: Remote Loads6 y. _/ P C* ^* N/ W0 S
Remote Loads
5 @8 ?: Q% g+ n4 W3 ^ QDirect Transfer
J- \6 _) ^$ u. B/ iFlexible surface$ q9 m& E9 M. T8 q1 ~
Applied as equivalent force & moment5 |0 V9 b d( s! M( p9 b( z7 F+ G- ^
Rigid Beam
+ i$ l9 U7 ^, ]; c% [. cRigid surface) m/ M" y0 M: G( k9 H
Remote Restraint
; ]* u) M& Z, WRigid connection* u& F2 S/ R! q- D
Model effect of a rigid virtual part between two faces
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$ q/ R/ X9 K! X( X0 ^Remote Load Example
% R4 T, a5 \- I; T0 U9 x+ m" jOpen “RemoteLoadExample.sldasm”
7 N+ u( ?% |( a" f4 I P" g; FDefine a static study “Remote”
' Z" e9 Q/ ~) O) J1 dApply material “Alloy steel”; I8 C3 v( ^, Z% i8 \# R& m/ U
Fix the flat face
' m4 p; T, ^$ l+ U4 C7 p, p, ]Select “Coordinate system1” and the end face of the cantilever. Define remote load of 10N in the X direction.
& v7 Z: w3 W0 J2 O; c( c% uCreate mesh and run. # `) J$ a1 L0 y5 t- ~
Double-click on “Plot1” under the stress folder0 @4 h1 y5 A' {$ o
Animate the results9 i q# a* B/ D( R( k
Compare the plot results of “Remote” study with “Axial Tension” study2 }8 e1 d" M7 u% T0 @' z3 Q, H+ e
f, p% L/ j$ E0 r: G+ a: @Motion Load Transfer Using Remote Loads
+ E+ l* l6 `& G$ t* `+ V, x0 sGo to SW Add-in and click “COSMOS/Motion”& s5 l6 h. x1 q# u1 S' p9 w, A1 G
Open “LoadTransferModel_With_Result.sldasm”
+ s2 Y- B6 k; F( h) @- ]3 IPlay the animation and save the load file for frame # 300
) f5 }6 i2 u/ m x- T' G$ Y ?Delete the motion results
* A, o( V4 z( e' \& l2 ?Go to CW menu, Import Motion Load and open this load file from “MotionLoadTransfer” directory+ o! c- E7 N/ K& ]0 H' C# A
Select all the loads related to crank-1 and then click OK.
: i& |9 K0 w' ~Open the part “crank”" ?, H/ `) l2 [3 e* g% k4 b& e K
You’ll see that there is a new study “Frame-300” with motion loads transferred as remote loads
( g }* M! v. K) kApply material “Plain carbon steel”* V- w1 m6 [8 @& W' L. k( P
Go to study properties and select “FFEPlus” solver and “Inertia relief option”. \6 \% P( l. ~1 A! n( w
Run the analysis
: v& l7 _* _8 J2 ?/ PPostprocessing: Results in local CS
/ I3 f3 S& T3 V7 b# f* L! \Plotting : Z4 |1 M9 ~( @% y- Y7 U' l
Listings8 E4 n6 L' ?- B7 B
Reaction forces6 ]6 ] |6 A% _' o5 k9 Z
Postprocessing: Exploded views
; i/ k3 X2 A$ w( BPlot results on SolidWorks exploded views
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Postprocessing: New tools& x$ m! Y8 m, k9 A& @/ o3 v! `
Improved probing with graphing option
" b7 D5 Y$ E% ^) p8 u ]# w5 JList results by Entity
2 \+ I3 ^; l; D* qWeb Reports
0 L0 p2 D' a, S5 Q( L" WInclusion of report templates in the feature tree
9 S6 J( q0 O6 y+ n l5 a, |Saving of report setting8 H$ U8 Z/ t5 T+ n* w* N
Automatic creation of all plots
# g( S2 g+ y; r1 {Report Example
) b& v& s" S# Y9 n! F# t/ }0 o- hOpen “ReportExample.sldasm”+ l; l; O2 d4 @0 g
New option save JPEG files (Right-click on the Study name)
; q) ^8 {- c/ w0 M' Y# KRight-click on Report and click define
a3 j4 q" }& _6 E, IPoint to the logo file “ReportLogo.bmp”
5 p% B: M4 B% ]0 B; QPoint to the right stress AVI and VRML files
; b3 D7 p- U: k2 X& y3 u+ ISelect option “Automatically update all plots in JPEG files”. Click OK.0 Z8 ?3 Z& f+ m, j9 L8 Z
You can also get a print version
$ n/ v# R# L# w- G6 hMaterial' p& H6 S0 `0 x5 [! e5 P4 \
Supports orthotropic material properties for solids and shells 8 J/ D# T, s+ E7 T6 P
Option to use different Material library files
: t m, ?7 [# z( N1 D( X" ENew redesigned material browser utility
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Licensing
4 h' }, C0 o/ CSingle license file for hardware lock & FlexLM security
6 l8 t3 _# `( F* j; GNew License Administrator to manage the license& F" M# x" U0 w# Z* V( q0 w
Support USB port hardware lock
, B: q- g) s2 }Support redundant servers' x3 b. ~% y/ s5 I, m% G
+ m$ W/ j4 W% B* aOther customer enhancements
! K+ N S' v! ]( kAutomatically run analysis after meshing p: g9 s H7 W
Edge pressure for shells" K% q0 c7 d. e$ w4 ]! R
Apply uniform temperature to components7 \) G7 M! x. S4 T0 Q2 G$ s' h, ?
Automatic adjustments of Max & min in plots on update+ a2 k$ ]& B- I2 S4 A
FFEPlus solver for thermal analysis# x8 a; |! W* Q, d6 ~( ]3 b
Increase the limit on number of modes for frequency analysis from 20 to 1006 V* ^) D/ T9 K. e( s5 C
Add symbol for gravity loads0 a) U4 V# j. y5 R3 t
Improve section clipping! `7 D% R7 O3 \' N
Save plots in JPEG format
* p4 W1 v0 l9 s2 R; L" \- vImprove transient thermal animations
7 m" J6 x: k; l, @0 B) E% COption to switch between different languages
Q/ B1 \: O. \& P- o4 ?$ g8 p9 ?Others…" K7 E! ~# k+ ^' S. }5 w" f
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Thank You! |
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