User:Eml5526.s11.team01.roark/Mtg23

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Mtg 23: Wed, 23 Feb 11

Page 23-1

HW 4.6:

FB, P. 74, Problem 3.9

End HW 4.6

HW 4.7:

Calculix (nonlinear FE code, open-source, ABAQUS-like input) : http://dhondt.de/

End HW 4.6

Paraglider Eml5526.s11.roark.figure23-1.svg

Disk Eml5526.s11.roark.figure23-2.svg

Sphere-volume Eml5526.s11.roark.figure23-3.svg

Page 23-2

  1. install cgx (calculix graphics module)
  2. Read manual, sign up with user group to ask questions if any. Also access archive.
  3. Reproduce basic examples: Disk, cylinder, sphere, sphere-volume, airfoil,
  4. Write report for “dummies”: Explain to novices how to install and run CGX (all CGX commands in basic examples, screenshots, …)

DWF p. 22-4

Use (5)-(6) p. 22-1, (1)-(7) p. 22-3, (1)-(6) p. 22-3, (1)-(3) p. 22-4 =>

\displaystyle \underbrace{{{c}_{E}}}_{=0}\cdot \underbrace{\left[ \left( {{\mathbf M}_{EE}}{{g}^{\left( s \right)}}+{{ \mathbf K}_{EE}}g \right)+{{ \mathbf M}_{Ef}}{{\mathbf d}_{F}}^{\left( s \right)}+{{ \mathbf K}_{EF}}{{\mathbf d}_{F}}-{{\mathbf F}_{E}} \right]}_{\ne 0}=0

(1)

DWF-U (unconstrained):

\displaystyle {{\mathbf c}_{F}}\cdot \left[ \underbrace{\left( {{\mathbf M}_{FE}}{{g}^{\left( s \right)}}+{{ \mathbf K}_{FE}}g \right)}_{Known}+{{\mathbf M}_{FF}}{{\mathbf d}_{F}}^{\left( s \right)}+{{ \mathbf K}_{FF}}{{\mathbf d}_{F}}-{{\mathbf F}_{F}} \right]=0\,\,\,\forall {{\mathbf c}_{F}}

(2)

Page 23-3

since \displaystyle {{c}_{F}} is unconstrained, => select arbitrarily

\displaystyle {{\mathbf c}_{F}}=\underbrace{\underset{1,2,...,n}{\mathop{\left\{ 1,0,...,0 \right\}}}\,,\underset{1,2,3,...,n}{\mathop{\left\{ 0,1,...,0 \right\}}}\,,\underset{1,...,n-1,n}{\mathop{\left\{ 0,...,0,1 \right\}}}\,,}_{n\,different\,choices\,for\,{{\mathbf c}_{F}}}

(1)

\displaystyle \underbrace{{{\mathbf{M}}_{FF}}}_{\begin{smallmatrix} 
 \mathbf{M} \\ 
 nxn 
\end{smallmatrix}}\underbrace{{{\mathbf{d}}_{F}}^{\left( s \right)}}_{\begin{smallmatrix} 
 {{\mathbf{d}}^{\left( s \right)}} \\ 
 nx1 
\end{smallmatrix}}+\underbrace{{{\mathbf{K}}_{FF}}}_{\begin{smallmatrix} 
 \mathbf{K} \\ 
 nxn 
\end{smallmatrix}}\underbrace{{{\mathbf{d}}_{F}}}_{\begin{smallmatrix} 
 \mathbf{d} \\ 
 nx1 
\end{smallmatrix}}=\underbrace{{{\mathbf{F}}_{F}}-\left( {{\mathbf{M}}_{FE}}{{g}^{\left( s \right)}}+{{\mathbf{K}}_{FE}}g \right)}_{\begin{smallmatrix} 
 \mathbf{F} \\ 
 nx1 
\end{smallmatrix}}

(2)

\displaystyle \mathbf{M}{{\mathbf{d}}^{\left( s \right)}}+\mathbf{Kd}=\mathbf{F}

(3)

Static: \displaystyle {{\mathbf{d}}^{\left( s \right)}}=\underset{nx1}{\mathop{\mathbf 0}}\,,{{g}^{s}}=0 (since g=constant)

\displaystyle \mathbf{Kd}=\mathbf{F}, \displaystyle \mathbf{F}={{\mathbf{F}}_{F}}-{{\mathbf{K}}_{FE}}g

(4)

Application: FB, p.72, Pb.3.4. \displaystyle \left\{ {{b}_{j}} \right\}=\left\{ {{\left( x-3 \right)}^{j}},j=0,1,...,n \right\} \displaystyle \mathbf{K}={{\left[ {{K}_{ij}};i,j-1,n \right]}_{nxn}}

\displaystyle {{K}_{ij}}=\int_{\alpha }^{\beta }{{{b}_{i}}^{\prime }{{a}_{2}}{{b}_{j}}^{\prime }dx}

(5)

Page 23-4

(7) p. 22-3:

\displaystyle {{K}_{ij}}={{\int_{\alpha }^{\beta }{\underbrace{i\left( x-3 \right)}_{{{b}_{i}}^{\prime }}}}^{i-1}}{{a}_{2}}\underbrace{j{{\left( x-3 \right)}^{j-1}}}_{{{b}_{j}}^{\prime }}dx

(1)

(5)-(6) p. 22-3: \displaystyle \underset{nx1}{\mathop {{\mathbf{K}}_{FE}}}\,=\left[ {{K}_{\underbrace{i}_{row}0}},i=1,...,n \right] , \displaystyle {{K}_{i0}}=\int_{\alpha }^{\beta }{{{b}_{i}}^{\prime }{{a}_{2}}\underbrace{{{b}_{0}}^{\prime }}_{=0}dx}=0


Also (5)-(6) p. 22-3: \displaystyle {{\mathbf{K}}_{FE}}=0=\mathbf{K}_{EF}^{T} and from (4) p. 23-3: \displaystyle \mathbf{F}={{\mathbf{F}}_{F}}

Structure of \displaystyle {{\mathbf{\tilde{K}}}_{\left( n+1 \right)\times \left( n+1 \right)}} (3) p. 22-3

\displaystyle {{\mathbf{\tilde{K}}}_{\left( n+1 \right)\times \left( n+1 \right)}}=\left[ \begin{matrix}
   {{K}_{\infty }} & \underbrace{0...0}_{1\times n}  \\
   \underbrace{\begin{matrix}
   0  \\
   :  \\
   0  \\
\end{matrix}}_{n\times 1} & \mathbf{K}  \\
\end{matrix} \right]

HW 4.8:

Find \displaystyle \tilde{\mathbf M} for FB, p.72, pb.3.4, assuming A=1, E=2, \displaystyle \mathbf m=3 do for n=3. For dynamics, with \displaystyle {{u}^{h}}(\beta ,t)=g(t)=\sin 2t, find \displaystyle \mathbf F(t)

End HW 4.8