Los factores influyen al nivel de la satisfacción laboral:

theoretical models of the contact pressure distribution, (a)

(a)

Figure

Figure

The shear stress under compression loading for the circular asperity is shown in and the shear stresses were observed to increase dramatically after 20

Figure

following sliding contact. When an oval asperity was modelled (

stress was shown to increase over that observed for the circular asperity. The stress increased further after contact sliding was applied to the model as well as a change in the stress distribution. Wh

debris model the maximum von Mises stress of 110 MPa on the CoCrMo material section occurred at a depth of 0.003 ×

4.8. Theoretical

From

theoretical models of the contact pressure distribution, (a)

(a)

Figure 4

Figure

The shear stress under compression loading for the circular asperity is shown in and the shear stresses were observed to increase dramatically after 20

Figure

following sliding contact. When an oval asperity was modelled (

stress was shown to increase over that observed for the circular asperity. The stress increased further after contact sliding was applied to the model as well as a change in the stress distribution. Wh

debris model the maximum von Mises stress of 110 MPa on the CoCrMo material section occurred at a depth of 0.003 ×

. Theoretical

From the maximum contac

theoretical models of the contact pressure distribution,

4.40

Figure 4.41

The shear stress under compression loading for the circular asperity is shown in and the shear stresses were observed to increase dramatically after 20

Figure 4.40

following sliding contact. When an oval asperity was modelled (

stress was shown to increase over that observed for the circular asperity. The stress increased further after contact sliding was applied to the model as well as a change in the stress distribution. Wh

debris model the maximum von Mises stress of 110 MPa on the CoCrMo material section occurred at a depth of 0.003 ×

. Theoretical

the maximum contac

theoretical models of the contact pressure distribution,

40. Shear stress of circular asperity (a) before 20

41. Oval asperity von Mises stress (a) before 20

The shear stress under compression loading for the circular asperity is shown in and the shear stresses were observed to increase dramatically after 20

40b). The shear stress distribution becomes asymmetrical about the centre of contact following sliding contact. When an oval asperity was modelled (

stress was shown to increase over that observed for the circular asperity. The stress increased further after contact sliding was applied to the model as well as a change in the stress distribution. Wh

debris model the maximum von Mises stress of 110 MPa on the CoCrMo material section occurred at a depth of 0.003 ×

. Theoretical

the maximum contac

theoretical models of the contact pressure distribution,

. Shear stress of circular asperity (a) before 20

. Oval asperity von Mises stress (a) before 20

The shear stress under compression loading for the circular asperity is shown in and the shear stresses were observed to increase dramatically after 20

b). The shear stress distribution becomes asymmetrical about the centre of contact following sliding contact. When an oval asperity was modelled (

stress was shown to increase over that observed for the circular asperity. The stress increased further after contact sliding was applied to the model as well as a change in the stress distribution. When linear elastic cortical bone material properties were applied to the circular debris model the maximum von Mises stress of 110 MPa on the CoCrMo material section occurred at a depth of 0.003 ×

. Theoretical

the maximum contac

theoretical models of the contact pressure distribution,

. Shear stress of circular asperity (a) before 20

. Oval asperity von Mises stress (a) before 20

The shear stress under compression loading for the circular asperity is shown in and the shear stresses were observed to increase dramatically after 20

b). The shear stress distribution becomes asymmetrical about the centre of contact following sliding contact. When an oval asperity was modelled (

stress was shown to increase over that observed for the circular asperity. The stress increased further after contact sliding was applied to the model as well as a change in the stress en linear elastic cortical bone material properties were applied to the circular debris model the maximum von Mises stress of 110 MPa on the CoCrMo material section occurred at a depth of 0.003 ×

. Theoretical

the maximum contac

theoretical models of the contact pressure distribution,

. Shear stress of circular asperity (a) before 20

. Oval asperity von Mises stress (a) before 20

The shear stress under compression loading for the circular asperity is shown in and the shear stresses were observed to increase dramatically after 20

b). The shear stress distribution becomes asymmetrical about the centre of contact following sliding contact. When an oval asperity was modelled (

stress was shown to increase over that observed for the circular asperity. The stress increased further after contact sliding was applied to the model as well as a change in the stress en linear elastic cortical bone material properties were applied to the circular debris model the maximum von Mises stress of 110 MPa on the CoCrMo material section occurred at a depth of 0.003 ×

. Theoretical

the maximum contac

theoretical models of the contact pressure distribution,

. Shear stress of circular asperity (a) before 20

. Oval asperity von Mises stress (a) before 20

The shear stress under compression loading for the circular asperity is shown in and the shear stresses were observed to increase dramatically after 20

b). The shear stress distribution becomes asymmetrical about the centre of contact following sliding contact. When an oval asperity was modelled (

stress was shown to increase over that observed for the circular asperity. The stress increased further after contact sliding was applied to the model as well as a change in the stress en linear elastic cortical bone material properties were applied to the circular debris model the maximum von Mises stress of 110 MPa on the CoCrMo material section occurred at a depth of 0.003 ×

. Theoretical M

the maximum contac

theoretical models of the contact pressure distribution,

. Shear stress of circular asperity (a) before 20

. Oval asperity von Mises stress (a) before 20

The shear stress under compression loading for the circular asperity is shown in and the shear stresses were observed to increase dramatically after 20

b). The shear stress distribution becomes asymmetrical about the centre of contact following sliding contact. When an oval asperity was modelled (

stress was shown to increase over that observed for the circular asperity. The stress increased further after contact sliding was applied to the model as well as a change in the stress en linear elastic cortical bone material properties were applied to the circular debris model the maximum von Mises stress of 110 MPa on the CoCrMo material section occurred at a depth of 0.003 ×

Model

the maximum contact pressure results obtained using theoretical models of the contact pressure distribution,

. Shear stress of circular asperity (a) before 20

. Oval asperity von Mises stress (a) before 20

The shear stress under compression loading for the circular asperity is shown in and the shear stresses were observed to increase dramatically after 20

b). The shear stress distribution becomes asymmetrical about the centre of contact following sliding contact. When an oval asperity was modelled (

stress was shown to increase over that observed for the circular asperity. The stress increased further after contact sliding was applied to the model as well as a change in the stress en linear elastic cortical bone material properties were applied to the circular debris model the maximum von Mises stress of 110 MPa on the CoCrMo material section occurred at a depth of 0.003 × h

odel

t pressure results obtained using theoretical models of the contact pressure distribution,

4.8. Theoretical Models and Lubrication Theory Application

. Shear stress of circular asperity (a) before 20

. Oval asperity von Mises stress (a) before 20

The shear stress under compression loading for the circular asperity is shown in and the shear stresses were observed to increase dramatically after 20

b). The shear stress distribution becomes asymmetrical about the centre of contact following sliding contact. When an oval asperity was modelled (

stress was shown to increase over that observed for the circular asperity. The stress increased further after contact sliding was applied to the model as well as a change in the stress en linear elastic cortical bone material properties were applied to the circular debris model the maximum von Mises stress of 110 MPa on the CoCrMo material section

ha, where

odels

t pressure results obtained using theoretical models of the contact pressure distribution,

4.8. Theoretical Models and Lubrication Theory Application

. Shear stress of circular asperity (a) before 20

. Oval asperity von Mises stress (a) before 20

The shear stress under compression loading for the circular asperity is shown in and the shear stresses were observed to increase dramatically after 20

b). The shear stress distribution becomes asymmetrical about the centre of contact following sliding contact. When an oval asperity was modelled (

stress was shown to increase over that observed for the circular asperity. The stress increased further after contact sliding was applied to the model as well as a change in the stress en linear elastic cortical bone material properties were applied to the circular debris model the maximum von Mises stress of 110 MPa on the CoCrMo material section

, where

s and Lubrication Theory Application

t pressure results obtained using

theoretical models of the contact pressure distribution,

4.8. Theoretical Models and Lubrication Theory Application

. Shear stress of circular asperity (a) before 20

. Oval asperity von Mises stress (a) before 20

The shear stress under compression loading for the circular asperity is shown in and the shear stresses were observed to increase dramatically after 20

b). The shear stress distribution becomes asymmetrical about the centre of contact following sliding contact. When an oval asperity was modelled (

stress was shown to increase over that observed for the circular asperity. The stress increased further after contact sliding was applied to the model as well as a change in the stress en linear elastic cortical bone material properties were applied to the circular debris model the maximum von Mises stress of 110 MPa on the CoCrMo material section

, where h

and Lubrication Theory Application

t pressure results obtained using

theoretical models of the contact pressure distribution,

4.8. Theoretical Models and Lubrication Theory Application

. Shear stress of circular asperity (a) before 20

. Oval asperity von Mises stress (a) before 20

The shear stress under compression loading for the circular asperity is shown in and the shear stresses were observed to increase dramatically after 20

b). The shear stress distribution becomes asymmetrical about the centre of contact following sliding contact. When an oval asperity was modelled (

stress was shown to increase over that observed for the circular asperity. The stress increased further after contact sliding was applied to the model as well as a change in the stress en linear elastic cortical bone material properties were applied to the circular debris model the maximum von Mises stress of 110 MPa on the CoCrMo material section

ha is the CoCrMo section height.

and Lubrication Theory Application

t pressure results obtained using

theoretical models of the contact pressure distribution,

4.8. Theoretical Models and Lubrication Theory Application

147

. Shear stress of circular asperity (a) before 20 contact

. Oval asperity von Mises stress (a) before 20 contact

The shear stress under compression loading for the circular asperity is shown in and the shear stresses were observed to increase dramatically after 20

b). The shear stress distribution becomes asymmetrical about the centre of contact following sliding contact. When an oval asperity was modelled (

stress was shown to increase over that observed for the circular asperity. The stress increased further after contact sliding was applied to the model as well as a change in the stress en linear elastic cortical bone material properties were applied to the circular debris model the maximum von Mises stress of 110 MPa on the CoCrMo material section

is the CoCrMo section height.

and Lubrication Theory Application

t pressure results obtained using

theoretical models of the contact pressure distribution, (b)

4.8. Theoretical Models and Lubrication Theory Application

147

. Shear stress of circular asperity (a) before 20 contact

. Oval asperity von Mises stress (a) before 20 contact

The shear stress under compression loading for the circular asperity is shown in and the shear stresses were observed to increase dramatically after 20

b). The shear stress distribution becomes asymmetrical about the centre of contact following sliding contact. When an oval asperity was modelled (

stress was shown to increase over that observed for the circular asperity. The stress increased further after contact sliding was applied to the model as well as a change in the stress en linear elastic cortical bone material properties were applied to the circular debris model the maximum von Mises stress of 110 MPa on the CoCrMo material section

is the CoCrMo section height.

and Lubrication Theory Application

t pressure results obtained using

theoretical models of the contact pressure distribution, (b)

(b)

4.8. Theoretical Models and Lubrication Theory Application

. Shear stress of circular asperity (a) before 20 µ

contact

. Oval asperity von Mises stress (a) before 20 µ

contact

The shear stress under compression loading for the circular asperity is shown in and the shear stresses were observed to increase dramatically after 20

b). The shear stress distribution becomes asymmetrical about the centre of contact following sliding contact. When an oval asperity was modelled (

stress was shown to increase over that observed for the circular asperity. The stress increased further after contact sliding was applied to the model as well as a change in the stress en linear elastic cortical bone material properties were applied to the circular debris model the maximum von Mises stress of 110 MPa on the CoCrMo material section

is the CoCrMo section height.

and Lubrication Theory Application

t pressure results obtained using

theoretical models of the contact pressure distribution, (b)

4.8. Theoretical Models and Lubrication Theory Application

µm of sliding contact

µm of sliding contact

The shear stress under compression loading for the circular asperity is shown in and the shear stresses were observed to increase dramatically after 20

b). The shear stress distribution becomes asymmetrical about the centre of contact following sliding contact. When an oval asperity was modelled (

stress was shown to increase over that observed for the circular asperity. The stress increased further after contact sliding was applied to the model as well as a change in the stress en linear elastic cortical bone material properties were applied to the circular debris model the maximum von Mises stress of 110 MPa on the CoCrMo material section

is the CoCrMo section height.

and Lubrication Theory Application

t pressure results obtained using

theoretical models of the contact pressure distribution,

4.8. Theoretical Models and Lubrication Theory Application

m of sliding contact

m of sliding contact

The shear stress under compression loading for the circular asperity is shown in and the shear stresses were observed to increase dramatically after 20

b). The shear stress distribution becomes asymmetrical about the centre of contact following sliding contact. When an oval asperity was modelled (

stress was shown to increase over that observed for the circular asperity. The stress increased further after contact sliding was applied to the model as well as a change in the stress en linear elastic cortical bone material properties were applied to the circular debris model the maximum von Mises stress of 110 MPa on the CoCrMo material section

is the CoCrMo section height.

and Lubrication Theory Application

t pressure results obtained using

theoretical models of the contact pressure distribution,

4.8. Theoretical Models and Lubrication Theory Application

m of sliding contact

m of sliding contact

The shear stress under compression loading for the circular asperity is shown in and the shear stresses were observed to increase dramatically after 20

b). The shear stress distribution becomes asymmetrical about the centre of contact following sliding contact. When an oval asperity was modelled (

stress was shown to increase over that observed for the circular asperity. The stress increased further after contact sliding was applied to the model as well as a change in the stress en linear elastic cortical bone material properties were applied to the circular debris model the maximum von Mises stress of 110 MPa on the CoCrMo material section

is the CoCrMo section height.

and Lubrication Theory Application

t pressure results obtained using

theoretical models of the contact pressure distribution,

4.8. Theoretical Models and Lubrication Theory Application

m of sliding contact

m of sliding contact

The shear stress under compression loading for the circular asperity is shown in and the shear stresses were observed to increase dramatically after 20

b). The shear stress distribution becomes asymmetrical about the centre of contact following sliding contact. When an oval asperity was modelled (

stress was shown to increase over that observed for the circular asperity. The stress increased further after contact sliding was applied to the model as well as a change in the stress en linear elastic cortical bone material properties were applied to the circular debris model the maximum von Mises stress of 110 MPa on the CoCrMo material section

is the CoCrMo section height.

and Lubrication Theory Application

the finite element method and theoretical models of the contact pressure distribution, theoretical contact pressure 4.8. Theoretical Models and Lubrication Theory Application

m of sliding contact

m of sliding contact

The shear stress under compression loading for the circular asperity is shown in and the shear stresses were observed to increase dramatically after 20

b). The shear stress distribution becomes asymmetrical about the centre of contact following sliding contact. When an oval asperity was modelled (Figure

stress was shown to increase over that observed for the circular asperity. The stress increased further after contact sliding was applied to the model as well as a change in the stress en linear elastic cortical bone material properties were applied to the circular debris model the maximum von Mises stress of 110 MPa on the CoCrMo material section

is the CoCrMo section height.

and Lubrication Theory Application

the finite element method and

theoretical contact pressure 4.8. Theoretical Models and Lubrication Theory Application

m of sliding contact

m of sliding contact

The shear stress under compression loading for the circular asperity is shown in and the shear stresses were observed to increase dramatically after 20

b). The shear stress distribution becomes asymmetrical about the centre of contact Figure

stress was shown to increase over that observed for the circular asperity. The stress increased further after contact sliding was applied to the model as well as a change in the stress en linear elastic cortical bone material properties were applied to the circular debris model the maximum von Mises stress of 110 MPa on the CoCrMo material section

In document Perfil de la comparación de las satisfacciones de entre los trabajadores de la organización grupo empresarial de la construcción en Villa Clara y La empresa comercializadora de combustibles de Matanzas (página 63-80)