صفحات

۱۳۸۷ خرداد ۱۴, سه‌شنبه

STRESS

STRESS


MECHANICS


                study of the action and effect of forces on bodies.


                "The Science of Motion"


 


Newton�s First Law of Motion- (Law of Inertia)


A body at rest will remain at rest and a body of motion will remain in motion unless acted upon by an outside force; i.e., a free body moves without acceleration.               


Newton�s Second Law- (Law of Acceleration)-


Force equals the mass times the acceleration.           F=ma    


Newton�s Third Law-


A directed force i....................s


STRESS


MECHANICS


                study of the action and effect of forces on bodies.


                "The Science of Motion"


 


Newton�s First Law of Motion- (Law of Inertia)


A body at rest will remain at rest and a body of motion will remain in motion unless acted upon by an outside force; i.e., a free body moves without acceleration.             


 


Newton�s Second Law- (Law of Acceleration)-


Force equals the mass times the acceleration.           F=ma  


 


Newton�s Third Law-


A directed force is counteracted by an equal force in the opposite direction.


 


 


FORCE-


    vector quantity with both magnitude and direction.      


    Force= (mass) (acceleration)               F=ma


 


Body Forces-


    forces that result from action of a field at every point within the body. E.g. gravity


Surface Forces-


    forces that act on the specific surface area in a body.


 


 


STRESS


Stress       s              Force per unit area or the intensity of Force             s=F/A


                                    


            Stress units: 1 bar= 105 Pa= 1 atm; 1 kbar=108 Pa = 100 MPa                         


            1 pascal = one pascal is one kilogram per meter per second squared;


that is, 1 Pa = 1 kg � m-1 � s-2.


1 MPa= 106 pascals


 


 


 


CLASSIFICATION OF STRESS


Compressive Stress           By convention, Geologists consider compressive stress as Positive


     (+)                                   (this designation is opposite to that used by engineers)


 


Tensile Stress                     By convention, Geologists consider tensile stress as Negative


   ( - ) 


 


Normal Stress     sh            Stress directed perpendicular to a given plane


 


Shear Stress        st            Stress directed parallel to a given plane


 


Principal Stresses              3 orthogonal stress axes directed perpendicular to


                                            principal planes upon which no shear stress exists.


             s 1 >s 2 >s 3


                        s 1 = maximum compressive stress axis


         s 2= intermediate stress axis


        s 3=  minimum compressive stress axis


 


Principal Planes         Planes with no shear stress.


                                    Contain 2 principal stress axes and normal to 3rd axis


 


Stress Field                 Total distribution of stress within a rock body


 


Components of Stress:


the orientation and magnitude of the stress state of a body can be defined by 9 components within the Cartesian coordinate system, defined by 3 mutually perpendicular axes:


                        In the direction of:


                                                                x                              y                              z


Stress on face normal to x:                s xx                                       s xy                                       s xz


 


Stress on face normal to y:                s yx                                       s yy                                      s yz


 


Stress on face normal to z:                s zx                                        s zy                                       s zz


               


Note that we can define the stress state based on 6 independent stress vector components:


s xx , s yy , s zz (Normal stresses) and s xy , s yz , s xz (shear stresses)                   



 


 


 


 


 


 


ISOTROPIC VS. ANISOTROPIC STRESS


Isotropic Stress      


    All 3 principal stress axes of equal magnitude (s 1 =s 2 =s 3) defining a sphere.


  


    Non-Deviatric Stress- Stress equal in all directions . s1= s2=s3.e.g. hydrostatic stress.


For any non-deviatric stresses, no shear stresses exist.


s1= s2=s3 can have any orientation, as stress equal in all orientations


 


    Non-Deviatric Stress- Two predictions can be made from non-deviatric (static ) stresses:


1. no change in shape (no shear stress; no shear strain)


2. causes volume (decrease) changes and increases density


 


       Mean Stress         sm          


             Average stress of the three principal axes       (s 1 + s 2+ s 3)/3


 


    Hydrostatic Stress= mean stress=  s1+ s2+s3


                                                                    3


 


Anisotropic Stress         Unequal Stress    


    At least one principal stress has a magnitude not equal to other principal stresses


 


    Deviatric Stress- sdev     directed stress;


        One or more stress axes are not equal to the other two.


            Compressive Stress - denoted as a positive (+) force


            Tensile Stress - denoted as a negative (-) force


            Normal Stress- (sn) force applied perpendicular to a plane.


            Shear Stress- (st ) force applied parallel to a plane (ccw=pos; cw=neg); max at 450.


                         Transpression- shear plus compressison                 


         Transtension- shear plus tension


 


    Deviatric Stresstwo predictions:


 1. there will be shear strain as a result of stress


 2. shear strain will result in distortion (change in shape)


i.e., Causes Shape Changes     


 


        Deviatric Stress- Directed stress;


            component of stress that remains after mean stress is removed.


 


EFFECTIVE STRESS & FLUID PORE PRESSURE-


Effective Stress=  normal stress minus the pore fluid pressure.


Picture (459x367, 9.7Kb)


 


 


 


 


 


 


Fluid Pore Pressure (Pf)- hydrostatic pressure exerted by interstitial water.


 


 


STRESS STATES:


 


Total Stress                       stotal= sm + sdev.


 


General Triaxial Stress     s 1 >s 2 >s 3 and not equal to 0


 


Biaxial Stress                      one principal stress axis equals 0


 


Uniaxial Tension                s 1 =s 2 =s 3 < 0


 


Uniaxial Compression        s 1 =s 2 =s 3 > 0


 


Hydrostatic Stress                s 1 =s 2 =s 3


 


Lithostatic Stress                  s 1 =s 2 =s 3;


                                                stress exerted on a point at depth overlain by a body of rock


 


Homogeneous Stress         


 Stress at any point in the body is of equal magnitude and direction.


 Magnitude & orientation of the stress ellipsoids are the same throughout the rock body


 All principal stresses have same orientation and magnitude; less complex, less common.


s 1 , s 2 , s 3  are not (generally) equal; i.e., homogeneous stress is not necessarily isotropic.


 


Inhomogeneous Stress      


    Stress is of different magnitude and/or orientation at different points in a body;


    More complex stress conditions within rock body; difficult to analyze; common.


 


 


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Return to: GEOLOGY 320 MAIN PAGE

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