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Geotechnical Elements and Models in OpenSees 
Pedro Arduino 
University of Washington, Seattle 
OpenSees Days Portugal 2014, 
Workshop on Multi-Hazard Analysis of Structures using OpenSees 
University of Porto, Porto, Portugal 
Thursday July 3, 2014
Type of Geotechnical Problems that can be solved using OpenSees 
Static Problems 
Deformation analyses (1D, 2D, or 3D) 
Consolidation problems (diffusion problems) 
Soil-structure interaction problems 
Shallow foundations (e.g. bearing capacity, settlements) 
Pile foundations (e.g. vertical and lateral capacity) 
Dynamic (earthquake problems) 
Free-field analysis 
Liquefaction induced problems 
Soil structure interaction problems (e.g. response of pile foundations, bridge bents, or complete structures embedded in soils to earthquake excitations)
What do we need?? 
Solid elements to characterize the soil domain (continuum). 
Appropriate boundary conditions to accurately represent the soil domain boundaries. 
Robust constitutive models to characterize the soil stress-strain response under monotonic and cyclic loading conditions 
Interface elements to capture the interaction between the soil and adjacent structures. 
Everything else you are learning in this workshop (i.e., how to create beam elements, apply loads and boundary conditions, record results, perform the analysis, etc.
Outline 
Elements (for solids) 
Single-phase 
Multi-phase (coupled) finite elements 
Zero length element 
Material models 
Elastic 
Elasto-plastic Continuum Models 
Elasto-plastic Uniaxial models 
Boundary conditions 
Equal DOF 
Absorbent boundaries 
Interface elements 
2D, 3D node-to-node contact elements 
Beam-contact elements
Elements (solids) 
Single-phase formulations 
To capture the response of dry soils (or total stress analysis) need one single phase 
Phase 1 – soil skeleton 
Multi-phase formulations 
To capture the response of saturated soils (effective stress analysis)  need two phases 
Phase 1  soil skeleton 
Phase 2  pore water 
Zero-Length element 
To capture interface response between solid and beam elements, and to apply absorbent boundary conditions
Elements Single Phase Formulation 
Small deformation solid elements 
2-D quadrilateral elements (4, 9 nodes) 
3-D solid elements, brick (8, 20 nodes) 
n1 
n2 
n3 
n4 
n2 
n1 
n3 
n4 
n6 
n5 
n7 
n8 
quad (4 node) 
stdBrick (8 node)
Elements quad element definition 
n1 
n2 
n3 
n4 
quad (4 node) 
element quad $eleTag $n1 $n2 $n3 $n4 $thick $type $matTag 
<$press $rho $b1 $b2> 
Must define first all the required arguments. In particular: 
Nodes $n1, $n2, $n3, $n4 and 
Material type $matTag 
The arguments in <…> are optional
Elements Multi-Phase Formulations 
Fully coupled u-p elements (2D & 3D) 
Fully coupled u-p-U elements (3D) for small deformations 
Degrees of Freedom (DOFs) are: 
u  solid displacement, on 
P  pore fluid pressures, on 
U  pore fluid displacements, on 
n1 
n2 
n3 
n4 
quadUP 
n1 
n2 
n3 
n4 
n5 
n6 
n7 
n8 
n9 
9_4_quadUP
Elements quadUP element definition 
element quadUP $eleTag $n1 $n2 $n3 $n4 $thick $type $matTag $bulk $fmass $hPerm $vPerm <$b1 $b2 $t> $bulk  combined undrained bulk modulus Bc=Bf/n $fmass  fluid mass density $hperm & $vperm  horiz. And vert. permeability 
n1 
n2 
n3 
n4 
quadUP
Elements Efficient formulations 
n1 
n2 
n3 
n4 
n2 
n1 
n3 
n4 
n6 
n5 
n7 
n8 
quad (4 node) 
stdBrick (8 node) 
Standard 2D and 3D solid Elements 
n1 
n2 
n3 
n4 
n2 
n1 
n3 
n4 
n6 
n5 
n7 
n8 
SSPquad (4 node) 
SSPBrick (8 node) 
Stabilized Single Point 2D and 3D Solid Elements
Elements Efficient formulations 
n1 
n2 
n3 
n4 
n2 
n1 
n3 
n4 
n6 
n5 
n7 
n8 
SSPquad (4 node) 
SSPBrick (8 node) 
Stabilized Single Point 2D and 3D Solid Elements 
n1 
n2 
n3 
n4 
n2 
n1 
n3 
n4 
n6 
n5 
n7 
n8 
SSPquad-up (4 node) 
SSPBrick-up (8 node) 
UP - Stabilized Single Point 2D and 3D Solid Elements
Elements zerolength element 
Connects two points at the same coordinate 
n1 
n2 
n3 
n4 
element zeroLength $eleTag $n1 $n2 –mat $matTag1 $matTag2 … -dir $dir1 $dir2 … <-orient $x1 $x2 $x3 $yp1 $yp2 $yp3> 
zero-length element 
solid element 
n5 
n6 
beam element
Material Models 
Linear Elastic Material model (nDMaterial) 
To characterize the response of the soil (or other continuum) in its elastic regime 
Elasto-Plastic Material models (nDMaterial) 
To characterize the nonlinear stress-strain response of soils 
Elasto-plastic Uniaxial models 
To characterize the interface response between soil and structural elements (uniaxialMaterial).
Material Models nDMaterial  Elastic 
Small deformation elasticity 
Linear isotropic 
Nonlinear isotropic 
Cross anisotropic 
Elastic Isotropic Material 
nDMaterial ElasticIsotropic $matTag $E $v
Material Models nDMaterial -Elasto-Plastic (Small Deformations) 
J2-Plasticity Material (von Mises) 
Drucker-Prager Material (UW) 
Cam-Clay Material (Berkeley, UW) 
MutiYield Materials (San Diego) 
Manzari-Dafalias (new) (UW)
Material Models nDMaterial - J2Plasticity 
von-Mises type 
nDMaterial J2Plasticity $matTag $K $G $sig0 $sigInf $delta $H 
sd 
sd-inf 
sd-0 
ed 
Von-Mises Yield Surface 
Stress-strain curve
Material Models nDMaterial MultiYield Materials 
Material models based on Multiyield Plasticity (Mroz et al., Prevost et al.) 
Two types 
Pressure Independent Multi-yield (for total stress analysis) 
Pressure Dependent Multi-yield (captures well the response of liquefiable soils) 
Developed by Elgamal et al. at UCSD 
http://cyclic.ucsd.edu/opensees/
Material Models – nDMaterial PressureDependentMultiYield 
15 parameters!!?? 
nDMaterial PressureDependMultiYield $matTag $nd $rho $refShearModul $refBulkModul $frictionAng $peakShearStra $refPress $pressDependCoe $PTAng $contrac $dilat1 $dilat2, $liquefac1 $liquefac2 $liquefac3 <$noYieldSurf=20 <$r1 $Gs1 …> $e=0.6 $cs1=0.9 $cs2=0.02 $cs3=0.7 $pa=101>
Material Models nDMaterial PressureDependentMultiYield 
nDMaterial PressureDependMultiYield $matTag $nd $rho $refShearModul $refBulkModul $frictionAng $peakShearStra $refPress $pressDependCoe $PTAng $contrac $dilat1 $dilat2, $liquefac1 $liquefac2 $liquefac3 <$noYieldSurf=20 <$r1 $Gs1 …> $e=0.6 $cs1=0.9 $cs2=0.02 $cs3=0.7 $pa=101>
Material Models nDMaterial PressureDependentMultiYield02 
nDMaterial PressureDependMultiYield02 $matTag $nd $rho $refBulkModul $frictionAng $peakShearStra $refPress $pressDepenCoe $PTAng $contrac1 $contrac3 $dilat1 $dilat3 <$noYieldSurf=20 <$r1 $Gs1 …> $contrac2=5.0 $dilat2=3.0 $liquefac1=1.0 $liquefac2=0.0 $e=0.6 $cs1=0.9 $cs2=0.02 $cs3=0.7 $pa=101>
Material Models nDMaterial PressureIndependentMultiYield 
nDMaterial PressureIndependMultiYield $matTag $nd $rho $refShearModul $refBulkModul $cohesi $peakShearStra $frictionAng $refPress=101 $pressDependCoe=0. <$noYieldSurf=20 <$r1 $Gs1 …>>
Material Models - nDMaterial 
Other Models under development 
nDMaterial BoundingCamClay  (Clays) 
nDMaterial Manzari-Dafalias  (Sands) 
b b b α α bμ  
d d d α α dμ  
s / p 1 
s / p 2 s / p 3 
O 
n 
  
b 
d 
n 
• 
• 
 
• 
 + 
yield surface 
bounding surface 
critical surface 
dilatancy surface 
b 
 α 
c 
 α 
d 
 α r  
• _ 
Bounding Surface Model
Material Models - nDMaterial Manzari-Dafalias (2004) 
Conventional Triaxial Test CTC Undrained 
Dense Sand 
Loose Sand 
Confinement 
Displacement
Material Models - nDMaterial Manzari-Dafalias (2004) 
Cyclic Constant Mean Stress TC Undrained 
Confinement 
Cyclic Shear Stress 
K=0 
K=Ko
Material Models Elasto-plastic Uniaxial models 
To capture interface response between solid (soil) and beam elements (pile) 
Py Tz Qz Uniaxial Materials 
•PySimple1 
•TzSimple1 
•QzSimple1 
•PyLiq1 
•TzLiq1
Material Models - uniaxialMaterial PySimple1 
uniaxialMaterial PySimple1 matTag $soilType $pult $Y50 $Cd <$c> 
y 
p 
pult (Reese 1974) 
y50 (API 1993) 
$soilType  =1 Matlock (clay), =2 API (sand) $pult  ultimate capacity of p-y material $Y50  displ. @ 50% of pult Cd  drag resistance (=1 no gap, <1 gap) $c  viscous damping 
Cd=1.0 
Cd=0.3
Material Models - uniaxialMaterial TzSimple1 & QzSimple1 
uniaxialMaterial TzSimple1 matTag $tzType $tult $z50 <$c> 
$tzType =1 Reese & O’Neill (clay), =2 Mosher (sand) $tult  ultimate capacity of t-z material $z50  displ. @ 50% of tult $c  viscous damping 
uniaxialMaterial QzSimple1 matTag $qzType $qult $z50 <$suction $c> 
$qzType =1 Reese & O’Neill (clay), =2 Vijayvergiya (sand) $qult = ultimate capacity of q-z material $z50 = displ. @ 50% of qult $suction  uplift resistance = suction*qult $c viscous damping
Material Models - uniaxialMaterial PyLiq1 
uniaxialMaterial PyLiq1 $matTag $soilType $pult $Y50 $Cd $c $pRes $solidElem1 $solidElem2 
$soilType  =1 Matlock (clay), =2 API (sand) 
$pult  ultimate capacity of p-y material 
$Y50  displ. @ 50% of pult 
Cd  drag resistance (=1 no gap, <1 gap) 
$c  viscous damping 
$pRes  residual (minimum) p-y resistance as ru=1.0 
$solidElem1 & $solidElem2  solid elements from which PyLiq1 will obtain effective stresses and pore pressures
Material Models - MuniaxialMaterial PyLiq1
Boundary Conditions 
EqualDof 
Same lateral deformation 
equalDOF $rNodeTag $cNodeTag $dof1 $dof2 … 
$rNodeTag  master node $cNodeTag  slave node $dof1 $dof2 …  constrained dof’s
Absorbent/transmitting Boundaries 
Lysmer (1969) 
1. set DampP 755 
2. set DampN 1216 
3. uniaxialMaterial Elastic 1 0 $DampP 
4. uniaxialMaterial Elastic 2 0 $DampN 
5. node 1 16.0 0.0 
6. node 2 16.0 0.0 
7. element zeroLength 1 1 2 -mat 1 2 
-dir 1 2 –orient 1 –2 0 2 1 0 
Quad Element 
P P 
N S 
C b V 
C a V 
 
 
 
 
zeroLength Element & 
uniaxial material
Interface Elements Contact Elements in OpenSees 
Beam-Solid Model 
Solid-Solid Model 
Fiber element 
Moment curvature response for single shaft
Interface elements Contact Elements in OpenSees 
3D Node-to-Surface Element 
2D Node-to-Line Element 
3D Beam-to-Solid Element 
3D End-Beam-to- Solid Element 
Master node 
Slave node 
tn 
g
element SimpleContact2D $eleTag $iNode $jNode $sNode $lNode $matTag $gTol $fTol 
$eleTag  unique integer tag identifying element object $iNode $jNode  master nodes $sNode  slave node $lNode  Lagrange multiplier node $matTag  unique integer tag associated with previously- defined material object $gTol  gap tolerance $fTol  force tolerance 
Master node 
Slave node 
Interface elements Contact Elements in OpenSees
Many more capabilities currently under development!!

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Geotechnical Elements and Models in OpenSees

  • 1. Geotechnical Elements and Models in OpenSees Pedro Arduino University of Washington, Seattle OpenSees Days Portugal 2014, Workshop on Multi-Hazard Analysis of Structures using OpenSees University of Porto, Porto, Portugal Thursday July 3, 2014
  • 2. Type of Geotechnical Problems that can be solved using OpenSees Static Problems Deformation analyses (1D, 2D, or 3D) Consolidation problems (diffusion problems) Soil-structure interaction problems Shallow foundations (e.g. bearing capacity, settlements) Pile foundations (e.g. vertical and lateral capacity) Dynamic (earthquake problems) Free-field analysis Liquefaction induced problems Soil structure interaction problems (e.g. response of pile foundations, bridge bents, or complete structures embedded in soils to earthquake excitations)
  • 3. What do we need?? Solid elements to characterize the soil domain (continuum). Appropriate boundary conditions to accurately represent the soil domain boundaries. Robust constitutive models to characterize the soil stress-strain response under monotonic and cyclic loading conditions Interface elements to capture the interaction between the soil and adjacent structures. Everything else you are learning in this workshop (i.e., how to create beam elements, apply loads and boundary conditions, record results, perform the analysis, etc.
  • 4. Outline Elements (for solids) Single-phase Multi-phase (coupled) finite elements Zero length element Material models Elastic Elasto-plastic Continuum Models Elasto-plastic Uniaxial models Boundary conditions Equal DOF Absorbent boundaries Interface elements 2D, 3D node-to-node contact elements Beam-contact elements
  • 5. Elements (solids) Single-phase formulations To capture the response of dry soils (or total stress analysis) need one single phase Phase 1 – soil skeleton Multi-phase formulations To capture the response of saturated soils (effective stress analysis)  need two phases Phase 1  soil skeleton Phase 2  pore water Zero-Length element To capture interface response between solid and beam elements, and to apply absorbent boundary conditions
  • 6. Elements Single Phase Formulation Small deformation solid elements 2-D quadrilateral elements (4, 9 nodes) 3-D solid elements, brick (8, 20 nodes) n1 n2 n3 n4 n2 n1 n3 n4 n6 n5 n7 n8 quad (4 node) stdBrick (8 node)
  • 7. Elements quad element definition n1 n2 n3 n4 quad (4 node) element quad $eleTag $n1 $n2 $n3 $n4 $thick $type $matTag <$press $rho $b1 $b2> Must define first all the required arguments. In particular: Nodes $n1, $n2, $n3, $n4 and Material type $matTag The arguments in <…> are optional
  • 8. Elements Multi-Phase Formulations Fully coupled u-p elements (2D & 3D) Fully coupled u-p-U elements (3D) for small deformations Degrees of Freedom (DOFs) are: u  solid displacement, on P  pore fluid pressures, on U  pore fluid displacements, on n1 n2 n3 n4 quadUP n1 n2 n3 n4 n5 n6 n7 n8 n9 9_4_quadUP
  • 9. Elements quadUP element definition element quadUP $eleTag $n1 $n2 $n3 $n4 $thick $type $matTag $bulk $fmass $hPerm $vPerm <$b1 $b2 $t> $bulk  combined undrained bulk modulus Bc=Bf/n $fmass  fluid mass density $hperm & $vperm  horiz. And vert. permeability n1 n2 n3 n4 quadUP
  • 10. Elements Efficient formulations n1 n2 n3 n4 n2 n1 n3 n4 n6 n5 n7 n8 quad (4 node) stdBrick (8 node) Standard 2D and 3D solid Elements n1 n2 n3 n4 n2 n1 n3 n4 n6 n5 n7 n8 SSPquad (4 node) SSPBrick (8 node) Stabilized Single Point 2D and 3D Solid Elements
  • 11. Elements Efficient formulations n1 n2 n3 n4 n2 n1 n3 n4 n6 n5 n7 n8 SSPquad (4 node) SSPBrick (8 node) Stabilized Single Point 2D and 3D Solid Elements n1 n2 n3 n4 n2 n1 n3 n4 n6 n5 n7 n8 SSPquad-up (4 node) SSPBrick-up (8 node) UP - Stabilized Single Point 2D and 3D Solid Elements
  • 12. Elements zerolength element Connects two points at the same coordinate n1 n2 n3 n4 element zeroLength $eleTag $n1 $n2 –mat $matTag1 $matTag2 … -dir $dir1 $dir2 … <-orient $x1 $x2 $x3 $yp1 $yp2 $yp3> zero-length element solid element n5 n6 beam element
  • 13. Material Models Linear Elastic Material model (nDMaterial) To characterize the response of the soil (or other continuum) in its elastic regime Elasto-Plastic Material models (nDMaterial) To characterize the nonlinear stress-strain response of soils Elasto-plastic Uniaxial models To characterize the interface response between soil and structural elements (uniaxialMaterial).
  • 14. Material Models nDMaterial  Elastic Small deformation elasticity Linear isotropic Nonlinear isotropic Cross anisotropic Elastic Isotropic Material nDMaterial ElasticIsotropic $matTag $E $v
  • 15. Material Models nDMaterial -Elasto-Plastic (Small Deformations) J2-Plasticity Material (von Mises) Drucker-Prager Material (UW) Cam-Clay Material (Berkeley, UW) MutiYield Materials (San Diego) Manzari-Dafalias (new) (UW)
  • 16. Material Models nDMaterial - J2Plasticity von-Mises type nDMaterial J2Plasticity $matTag $K $G $sig0 $sigInf $delta $H sd sd-inf sd-0 ed Von-Mises Yield Surface Stress-strain curve
  • 17. Material Models nDMaterial MultiYield Materials Material models based on Multiyield Plasticity (Mroz et al., Prevost et al.) Two types Pressure Independent Multi-yield (for total stress analysis) Pressure Dependent Multi-yield (captures well the response of liquefiable soils) Developed by Elgamal et al. at UCSD http://cyclic.ucsd.edu/opensees/
  • 18. Material Models – nDMaterial PressureDependentMultiYield 15 parameters!!?? nDMaterial PressureDependMultiYield $matTag $nd $rho $refShearModul $refBulkModul $frictionAng $peakShearStra $refPress $pressDependCoe $PTAng $contrac $dilat1 $dilat2, $liquefac1 $liquefac2 $liquefac3 <$noYieldSurf=20 <$r1 $Gs1 …> $e=0.6 $cs1=0.9 $cs2=0.02 $cs3=0.7 $pa=101>
  • 19. Material Models nDMaterial PressureDependentMultiYield nDMaterial PressureDependMultiYield $matTag $nd $rho $refShearModul $refBulkModul $frictionAng $peakShearStra $refPress $pressDependCoe $PTAng $contrac $dilat1 $dilat2, $liquefac1 $liquefac2 $liquefac3 <$noYieldSurf=20 <$r1 $Gs1 …> $e=0.6 $cs1=0.9 $cs2=0.02 $cs3=0.7 $pa=101>
  • 20. Material Models nDMaterial PressureDependentMultiYield02 nDMaterial PressureDependMultiYield02 $matTag $nd $rho $refBulkModul $frictionAng $peakShearStra $refPress $pressDepenCoe $PTAng $contrac1 $contrac3 $dilat1 $dilat3 <$noYieldSurf=20 <$r1 $Gs1 …> $contrac2=5.0 $dilat2=3.0 $liquefac1=1.0 $liquefac2=0.0 $e=0.6 $cs1=0.9 $cs2=0.02 $cs3=0.7 $pa=101>
  • 21. Material Models nDMaterial PressureIndependentMultiYield nDMaterial PressureIndependMultiYield $matTag $nd $rho $refShearModul $refBulkModul $cohesi $peakShearStra $frictionAng $refPress=101 $pressDependCoe=0. <$noYieldSurf=20 <$r1 $Gs1 …>>
  • 22. Material Models - nDMaterial Other Models under development nDMaterial BoundingCamClay  (Clays) nDMaterial Manzari-Dafalias  (Sands) b b b α α bμ  d d d α α dμ  s / p 1 s / p 2 s / p 3 O n   b d n • •  •  + yield surface bounding surface critical surface dilatancy surface b  α c  α d  α r  • _ Bounding Surface Model
  • 23. Material Models - nDMaterial Manzari-Dafalias (2004) Conventional Triaxial Test CTC Undrained Dense Sand Loose Sand Confinement Displacement
  • 24. Material Models - nDMaterial Manzari-Dafalias (2004) Cyclic Constant Mean Stress TC Undrained Confinement Cyclic Shear Stress K=0 K=Ko
  • 25. Material Models Elasto-plastic Uniaxial models To capture interface response between solid (soil) and beam elements (pile) Py Tz Qz Uniaxial Materials •PySimple1 •TzSimple1 •QzSimple1 •PyLiq1 •TzLiq1
  • 26. Material Models - uniaxialMaterial PySimple1 uniaxialMaterial PySimple1 matTag $soilType $pult $Y50 $Cd <$c> y p pult (Reese 1974) y50 (API 1993) $soilType  =1 Matlock (clay), =2 API (sand) $pult  ultimate capacity of p-y material $Y50  displ. @ 50% of pult Cd  drag resistance (=1 no gap, <1 gap) $c  viscous damping Cd=1.0 Cd=0.3
  • 27. Material Models - uniaxialMaterial TzSimple1 & QzSimple1 uniaxialMaterial TzSimple1 matTag $tzType $tult $z50 <$c> $tzType =1 Reese & O’Neill (clay), =2 Mosher (sand) $tult  ultimate capacity of t-z material $z50  displ. @ 50% of tult $c  viscous damping uniaxialMaterial QzSimple1 matTag $qzType $qult $z50 <$suction $c> $qzType =1 Reese & O’Neill (clay), =2 Vijayvergiya (sand) $qult = ultimate capacity of q-z material $z50 = displ. @ 50% of qult $suction  uplift resistance = suction*qult $c viscous damping
  • 28. Material Models - uniaxialMaterial PyLiq1 uniaxialMaterial PyLiq1 $matTag $soilType $pult $Y50 $Cd $c $pRes $solidElem1 $solidElem2 $soilType  =1 Matlock (clay), =2 API (sand) $pult  ultimate capacity of p-y material $Y50  displ. @ 50% of pult Cd  drag resistance (=1 no gap, <1 gap) $c  viscous damping $pRes  residual (minimum) p-y resistance as ru=1.0 $solidElem1 & $solidElem2  solid elements from which PyLiq1 will obtain effective stresses and pore pressures
  • 29. Material Models - MuniaxialMaterial PyLiq1
  • 30. Boundary Conditions EqualDof Same lateral deformation equalDOF $rNodeTag $cNodeTag $dof1 $dof2 … $rNodeTag  master node $cNodeTag  slave node $dof1 $dof2 …  constrained dof’s
  • 31. Absorbent/transmitting Boundaries Lysmer (1969) 1. set DampP 755 2. set DampN 1216 3. uniaxialMaterial Elastic 1 0 $DampP 4. uniaxialMaterial Elastic 2 0 $DampN 5. node 1 16.0 0.0 6. node 2 16.0 0.0 7. element zeroLength 1 1 2 -mat 1 2 -dir 1 2 –orient 1 –2 0 2 1 0 Quad Element P P N S C b V C a V     zeroLength Element & uniaxial material
  • 32. Interface Elements Contact Elements in OpenSees Beam-Solid Model Solid-Solid Model Fiber element Moment curvature response for single shaft
  • 33. Interface elements Contact Elements in OpenSees 3D Node-to-Surface Element 2D Node-to-Line Element 3D Beam-to-Solid Element 3D End-Beam-to- Solid Element Master node Slave node tn g
  • 34. element SimpleContact2D $eleTag $iNode $jNode $sNode $lNode $matTag $gTol $fTol $eleTag  unique integer tag identifying element object $iNode $jNode  master nodes $sNode  slave node $lNode  Lagrange multiplier node $matTag  unique integer tag associated with previously- defined material object $gTol  gap tolerance $fTol  force tolerance Master node Slave node Interface elements Contact Elements in OpenSees
  • 35. Many more capabilities currently under development!!