Backstay Effect Be Included in a Lateral Model and What Is an the Lateral System

Total Page:16

File Type:pdf, Size:1020Kb

Backstay Effect Be Included in a Lateral Model and What Is an the Lateral System Structural PracticeS practical knowledge beyond the textbook ® Figure 1: Modeling options for base condition. ne of the least understood aspects For a typical building with one or more below of modeling building structures is grade levels, the perimeter basement walls create dealing with at- and below-grade a very largeCopyright and laterally components. This includes soil- stiff box. The ground floor Ostructure interaction, but also the question of diaphragm engages this which below-grade structural elements should box and integrates it into Backstay Effect be included in a lateral model and what is an the lateral system. Sticking accurate representation of the base conditions. with the beam analogy, The focus of this article is what is most commonly the result is an effectively larger beam section Basement Modeling in referred to as the backstay effect. Traditionally, lat- below grade. This results in shedding of lateral Tall Buildings eral systems have been viewed as simple cantilever load from the main lateral force resisting system beams fixed at the base. While this analogy is (LFRS) to the basement walls. Overturning and By Nat Tocci, P.E. and Sanya Levi reasonable for the above-grade structure, a more shear are shared between the perimeter walls and accurate analogy would also include the effects magazinecore rather than isolated beneath the building of the below-grade structure,S which behavesT likeR core. ConceptuallyU C this is fairlyT straightforward. U R E a backspan to the cantilever. In this analogy, the The complexity arises in properly modeling the lateral system is viewed as a beam overhanging change in section, and capturing an accurate dis- one support, where that support is created by the tribution of internal forces and external reactions. at-grade diaphragm and foundation walls. The degree to which lateral loads are transferred The backstay effect is not limited to restraint at into the foundation perimeter is dependent on many the grade level. Backstay effects are also seen at set- variables, many of which there is limited certainty Nat Tocci, P.E. is the owner of Tocci backs with changes to the lateral system, the most about, as they are not specified or controlled in Engineering PLLC in New York common example being lower level podiums. They a typical project. It is therefore fair to ask if it is City and can be reached at are often very large in plan and introduce new lat- more conservative to simply ignore any backstay [email protected]. eral elements, and are therefore significantly stiffer effects and model the building core as an isolated Sanya Levi is an engineer at Arup than the set-back structure above. Backstay effects element. However, it can be shown that in many New York and can be reached at are also impacted by multiple basement levels. For cases the backstay effect will create higher demands [email protected]. simplicity of explanation, this article will focus on in some structural elements, in particular shear in the most common example which is the effect of the main LFRS below grade as well as the backstay the ground floor diaphragm in contributing to diaphragms, and therefore cannot be ignored. backstay effects. The concepts can be extended to Figure 1 is a stick diagram presenting some of all conditions where backstay effects occur. the possible options for modeling the base condi- tions of a core wall building. The building is of Backstay Effect height H with a basement of height B. The most traditional model, a simple cantilever, is shown Backstay effects are most noticeable in buildings in Figure 1a. It is clear that the maximum shear with discrete lateral systems, such as shear walls, is V = F. The extreme case of the backstay effect as opposed to distributed lateral systems. Building is shown in Figure 1b. In Figure 1b the ground height is also a major factor in the magnitude of floor diaphragm and perimeter foundation are the backstay effects. For the purposes of illustra- very stiff and are therefore modeled as a pin. tion, this article focuses on a high rise shear wall Statics shows that the maximum shear in the core building with a single basement. now occurs below grade with V = 3H/2B F. The STRUCTURE magazine 23 overall base shear has not changed, but the should also be considered. This component is backstay effect may create conditions with typically small relative to the other elements much higher demands than anticipated in and may possibly be neglected in many cases. certain elements. It can also be shown that In addition, this force is present only in the the base overturning moment in the core compression cycle of loading and should be has been reduced and redistributed to the modeled as such. perimeter foundation walls. Clearly there are many parameters to consider. Although Figure 1b shows dramatic increases In most cases, the best that can be done is to in shear, this is overly conservative for most model all contributing elements and make an conditions. The true restraint at the ground educated estimate of the element stiffnesses. floor is far from rigid and may range from The number of possibilities is too numerous Typical concrete core building configuration. very stiff to almost non-existent. A more real- for a prescriptive approach that will work for istic model is one in which the ground floor all buildings, which is perhaps why there is interface slip, and other unknowns, the stiffness restraint is modeled as a spring, producing little literature on the subject. Most building of the slab should be reduced for both shear results somewhere between Figures 1a and codes provide requirements for loading and (GAv) and flexural (EI) stiffness. Similar mod- 1b. Figure 1c shows this option. design of structural elements, but rarely provide eling guidelines ®and stiffness reductions should The complexity of an accurate model lies in detailed guidance on modeling procedures. A also be applied to basement wall elements. the fact that the spring in Figure 1c represents very good resource for an in depth discussion Soil stiffness should also be bracketed, typi- the cumulative stiffness of numerous elements of the backstay effect and recommendations for cally starting with recommendations provided in the building structure and supporting soil. A modeling is Modeling and Acceptance Criteria by the project geotechnical engineer. The sup- partial list of elements represented by the ground for Seismic Design and Analysis of Tall Buildings, porting stiffness under all elements should be floor spring would include: diaphragm to core PEER/ATC 72-1,Copyright which is available as a free taken at an upper and lower bound, and passive connection, diaphragm stiffness, diaphragm download from the PEER (Pacific Earthquake resistance provided against the perpendicular to basement wall connection, basement wall Engineering Institute) website. wall should also be bracketed if it is modeled. stiffness, foundation stiffness, and passive soil The backstay concept is more familiar to PEER/ATC 72-1 Table A-2 and Table A-3 resistance against the basement wall. engineers working in high seismic regions provide recommended upper and lower Ground floor diaphragms are often thick and has had less attention in other regions. bounds for bracketing the stiffness of the concrete plates with high relative stiffness. The concepts, however, are applicable for both above elements. PEER/ATC 72-1 also recom- However, this stiffness may be reduced by wind and seismic loading. mends that elements outside of the backstay cracking, bond slip, and discontinuities such influence (primarily tower elements) need not as large openings or slab elevation changes. Modeling be bracketed and should be modeled with In addition to the stiffness of the diaphragm the same assumptions used for their design. itself, the connections at each end must be A reasonablemagazine first step may be to assess whether Since these recommendations are intended for considered for their abilityS to transfer T the Rthe backstay U effect isC a consideration T forU the buildings R in highE seismic regions, it may be backstay shears. The same can be said for the building under investigation. A quick study of appropriate to adjust the recommendations basement walls which will have varying stiff- the parameters that create the backstay effect for wind controlled design to account for ness dependent on the same factors. may quickly rule out the need for a more in primarily elastic behavior. The overall stiffness of the diaphragm and depth analysis. The building system or con- Due to the complexity of capturing backstay basement wall system is also affected by the figuration may also determine the potential effects in the analysis, it may be desired to elimi- supporting foundation elements. Differences for backstay effects. nate the phenomenon in the actual building. in relative stiffness between core and perim- For buildings where backstay effects need This can be accomplished by isolating the LFRS eter wall soil support conditions may magnify to be considered, it will most likely be nec- from the foundation elements by providing lat- or lessen backstay effects. essary to consider multiple scenarios. Both eral joint at the backstay diaphragms. Typically The passive resistance provided by the soil on an overestimation and underestimation of this is done by providing a corbel or similar the basement wall face in the direction of force backstay effects can produce underestimates detail at the diaphragm to shear wall interface. of demand. For example, overestimating backstay restraint may underestimate the Conclusion overturning demand at the base of the main LFRS. The common approach is Ignoring the contribution of at- and below- to consider reasonable extremes for both grade structural elements in lateral models may The easiest to use software for calculating conditions and design each element for underestimate demands in key elements.
Recommended publications
  • The Experimental Determination of the Moment of Inertia of a Model Airplane Michael Koken [email protected]
    The University of Akron IdeaExchange@UAkron The Dr. Gary B. and Pamela S. Williams Honors Honors Research Projects College Fall 2017 The Experimental Determination of the Moment of Inertia of a Model Airplane Michael Koken [email protected] Please take a moment to share how this work helps you through this survey. Your feedback will be important as we plan further development of our repository. Follow this and additional works at: http://ideaexchange.uakron.edu/honors_research_projects Part of the Aerospace Engineering Commons, Aviation Commons, Civil and Environmental Engineering Commons, Mechanical Engineering Commons, and the Physics Commons Recommended Citation Koken, Michael, "The Experimental Determination of the Moment of Inertia of a Model Airplane" (2017). Honors Research Projects. 585. http://ideaexchange.uakron.edu/honors_research_projects/585 This Honors Research Project is brought to you for free and open access by The Dr. Gary B. and Pamela S. Williams Honors College at IdeaExchange@UAkron, the institutional repository of The nivU ersity of Akron in Akron, Ohio, USA. It has been accepted for inclusion in Honors Research Projects by an authorized administrator of IdeaExchange@UAkron. For more information, please contact [email protected], [email protected]. 2017 THE EXPERIMENTAL DETERMINATION OF A MODEL AIRPLANE KOKEN, MICHAEL THE UNIVERSITY OF AKRON Honors Project TABLE OF CONTENTS List of Tables ................................................................................................................................................
    [Show full text]
  • Rotational Motion (The Dynamics of a Rigid Body)
    University of Nebraska - Lincoln DigitalCommons@University of Nebraska - Lincoln Robert Katz Publications Research Papers in Physics and Astronomy 1-1958 Physics, Chapter 11: Rotational Motion (The Dynamics of a Rigid Body) Henry Semat City College of New York Robert Katz University of Nebraska-Lincoln, [email protected] Follow this and additional works at: https://digitalcommons.unl.edu/physicskatz Part of the Physics Commons Semat, Henry and Katz, Robert, "Physics, Chapter 11: Rotational Motion (The Dynamics of a Rigid Body)" (1958). Robert Katz Publications. 141. https://digitalcommons.unl.edu/physicskatz/141 This Article is brought to you for free and open access by the Research Papers in Physics and Astronomy at DigitalCommons@University of Nebraska - Lincoln. It has been accepted for inclusion in Robert Katz Publications by an authorized administrator of DigitalCommons@University of Nebraska - Lincoln. 11 Rotational Motion (The Dynamics of a Rigid Body) 11-1 Motion about a Fixed Axis The motion of the flywheel of an engine and of a pulley on its axle are examples of an important type of motion of a rigid body, that of the motion of rotation about a fixed axis. Consider the motion of a uniform disk rotat­ ing about a fixed axis passing through its center of gravity C perpendicular to the face of the disk, as shown in Figure 11-1. The motion of this disk may be de­ scribed in terms of the motions of each of its individual particles, but a better way to describe the motion is in terms of the angle through which the disk rotates.
    [Show full text]
  • Pierre Simon Laplace - Biography Paper
    Pierre Simon Laplace - Biography Paper MATH 4010 Melissa R. Moore University of Colorado- Denver April 1, 2008 2 Many people contributed to the scientific fields of mathematics, physics, chemistry and astronomy. According to Gillispie (1997), Pierre Simon Laplace was the most influential scientist in all history, (p.vii). Laplace helped form the modern scientific disciplines. His techniques are used diligently by engineers, mathematicians and physicists. His diverse collection of work ranged in all fields but began in mathematics. Laplace was born in Normandy in 1749. His father, Pierre, was a syndic of a parish and his mother, Marie-Anne, was from a family of farmers. Many accounts refer to Laplace as a peasant. While it was not exactly known the profession of his Uncle Louis, priest, mathematician or teacher, speculations implied he was an educated man. In 1756, Laplace enrolled at the Beaumont-en-Auge, a secondary school run the Benedictine order. He studied there until the age of sixteen. The nest step of education led to either the army or the church. His father intended him for ecclesiastical vocation, according to Gillispie (1997 p.3). In 1766, Laplace went to the University of Caen to begin preparation for a career in the church, according to Katz (1998 p.609). Cristophe Gadbled and Pierre Le Canu taught Laplace mathematics, which in turn showed him his talents. In 1768, Laplace left for Paris to pursue mathematics further. Le Canu gave Laplace a letter of recommendation to d’Alembert, according to Gillispie (1997 p.3). Allegedly d’Alembert gave Laplace a problem which he solved immediately.
    [Show full text]
  • Magnetism, Angular Momentum, and Spin
    Chapter 19 Magnetism, Angular Momentum, and Spin P. J. Grandinetti Chem. 4300 P. J. Grandinetti Chapter 19: Magnetism, Angular Momentum, and Spin In 1820 Hans Christian Ørsted discovered that electric current produces a magnetic field that deflects compass needle from magnetic north, establishing first direct connection between fields of electricity and magnetism. P. J. Grandinetti Chapter 19: Magnetism, Angular Momentum, and Spin Biot-Savart Law Jean-Baptiste Biot and Félix Savart worked out that magnetic field, B⃗, produced at distance r away from section of wire of length dl carrying steady current I is 휇 I d⃗l × ⃗r dB⃗ = 0 Biot-Savart law 4휋 r3 Direction of magnetic field vector is given by “right-hand” rule: if you point thumb of your right hand along direction of current then your fingers will curl in direction of magnetic field. current P. J. Grandinetti Chapter 19: Magnetism, Angular Momentum, and Spin Microscopic Origins of Magnetism Shortly after Biot and Savart, Ampére suggested that magnetism in matter arises from a multitude of ring currents circulating at atomic and molecular scale. André-Marie Ampére 1775 - 1836 P. J. Grandinetti Chapter 19: Magnetism, Angular Momentum, and Spin Magnetic dipole moment from current loop Current flowing in flat loop of wire with area A will generate magnetic field magnetic which, at distance much larger than radius, r, appears identical to field dipole produced by point magnetic dipole with strength of radius 휇 = | ⃗휇| = I ⋅ A current Example What is magnetic dipole moment induced by e* in circular orbit of radius r with linear velocity v? * 휋 Solution: For e with linear velocity of v the time for one orbit is torbit = 2 r_v.
    [Show full text]
  • Finite Element Model Calibration of an Instrumented Thirteen-Story Steel Moment Frame Building in South San Fernando Valley, California
    Finite Element Model Calibration of An Instrumented Thirteen-story Steel Moment Frame Building in South San Fernando Valley, California By Erol Kalkan Disclamer The finite element model incuding its executable file are provided by the copyright holder "as is" and any express or implied warranties, including, but not limited to, the implied warranties of merchantability and fitness for a particular purpose are disclaimed. In no event shall the copyright owner be liable for any direct, indirect, incidental, special, exemplary, or consequential damages (including, but not limited to, procurement of substitute goods or services; loss of use, data, or profits; or business interruption) however caused and on any theory of liability, whether in contract, strict liability, or tort (including negligence or otherwise) arising in any way out of the use of this software, even if advised of the possibility of such damage. Acknowledgments Ground motions were recorded at a station owned and maintained by the California Geological Survey (CGS). Data can be downloaded from CESMD Virtual Data Center at: http://www.strongmotioncenter.org/cgi-bin/CESMD/StaEvent.pl?stacode=CE24567. Contents Introduction ..................................................................................................................................................... 1 OpenSEES Model ........................................................................................................................................... 3 Calibration of OpenSEES Model to Observed Response
    [Show full text]
  • Moment of Inertia
    MOMENT OF INERTIA The moment of inertia, also known as the mass moment of inertia, angular mass or rotational inertia, of a rigid body is a quantity that determines the torque needed for a desired angular acceleration about a rotational axis; similar to how mass determines the force needed for a desired acceleration. It depends on the body's mass distribution and the axis chosen, with larger moments requiring more torque to change the body's rotation rate. It is an extensive (additive) property: for a point mass the moment of inertia is simply the mass times the square of the perpendicular distance to the rotation axis. The moment of inertia of a rigid composite system is the sum of the moments of inertia of its component subsystems (all taken about the same axis). Its simplest definition is the second moment of mass with respect to distance from an axis. For bodies constrained to rotate in a plane, only their moment of inertia about an axis perpendicular to the plane, a scalar value, and matters. For bodies free to rotate in three dimensions, their moments can be described by a symmetric 3 × 3 matrix, with a set of mutually perpendicular principal axes for which this matrix is diagonal and torques around the axes act independently of each other. When a body is free to rotate around an axis, torque must be applied to change its angular momentum. The amount of torque needed to cause any given angular acceleration (the rate of change in angular velocity) is proportional to the moment of inertia of the body.
    [Show full text]
  • Angular Momentum and Magnetic Moment
    Angular momentum and magnetic moment Introduction to Nuclear Science Simon Fraser University Spring 2011 NUCS 342 | January 12, 2011 NUCS 342 (Lecture 1) January 12, 2011 1 / 27 2 Conservation laws 3 Scalar and vector product 4 Rotational motion 5 Magnetic moment 6 Angular momentum in quantum mechanics 7 Spin Outline 1 Scalars and vectors NUCS 342 (Lecture 1) January 12, 2011 2 / 27 3 Scalar and vector product 4 Rotational motion 5 Magnetic moment 6 Angular momentum in quantum mechanics 7 Spin Outline 1 Scalars and vectors 2 Conservation laws NUCS 342 (Lecture 1) January 12, 2011 2 / 27 4 Rotational motion 5 Magnetic moment 6 Angular momentum in quantum mechanics 7 Spin Outline 1 Scalars and vectors 2 Conservation laws 3 Scalar and vector product NUCS 342 (Lecture 1) January 12, 2011 2 / 27 5 Magnetic moment 6 Angular momentum in quantum mechanics 7 Spin Outline 1 Scalars and vectors 2 Conservation laws 3 Scalar and vector product 4 Rotational motion NUCS 342 (Lecture 1) January 12, 2011 2 / 27 6 Angular momentum in quantum mechanics 7 Spin Outline 1 Scalars and vectors 2 Conservation laws 3 Scalar and vector product 4 Rotational motion 5 Magnetic moment NUCS 342 (Lecture 1) January 12, 2011 2 / 27 7 Spin Outline 1 Scalars and vectors 2 Conservation laws 3 Scalar and vector product 4 Rotational motion 5 Magnetic moment 6 Angular momentum in quantum mechanics NUCS 342 (Lecture 1) January 12, 2011 2 / 27 Outline 1 Scalars and vectors 2 Conservation laws 3 Scalar and vector product 4 Rotational motion 5 Magnetic moment 6 Angular momentum in quantum mechanics 7 Spin NUCS 342 (Lecture 1) January 12, 2011 2 / 27 Scalars and vectors Scalars Scalars are used to describe objects which are fully characterized by their magnitude (a number and a unit).
    [Show full text]
  • Rotation: Moment of Inertia and Torque
    Rotation: Moment of Inertia and Torque Every time we push a door open or tighten a bolt using a wrench, we apply a force that results in a rotational motion about a fixed axis. Through experience we learn that where the force is applied and how the force is applied is just as important as how much force is applied when we want to make something rotate. This tutorial discusses the dynamics of an object rotating about a fixed axis and introduces the concepts of torque and moment of inertia. These concepts allows us to get a better understanding of why pushing a door towards its hinges is not very a very effective way to make it open, why using a longer wrench makes it easier to loosen a tight bolt, etc. This module begins by looking at the kinetic energy of rotation and by defining a quantity known as the moment of inertia which is the rotational analog of mass. Then it proceeds to discuss the quantity called torque which is the rotational analog of force and is the physical quantity that is required to changed an object's state of rotational motion. Moment of Inertia Kinetic Energy of Rotation Consider a rigid object rotating about a fixed axis at a certain angular velocity. Since every particle in the object is moving, every particle has kinetic energy. To find the total kinetic energy related to the rotation of the body, the sum of the kinetic energy of every particle due to the rotational motion is taken. The total kinetic energy can be expressed as ..
    [Show full text]
  • Chapter 13: the Conditions of Rotary Motion
    Chapter 13 Conditions of Rotary Motion KINESIOLOGY Scientific Basis of Human Motion, 11 th edition Hamilton, Weimar & Luttgens Presentation Created by TK Koesterer, Ph.D., ATC Humboldt State University Revised by Hamilton & Weimar REVISED FOR FYS by J. Wunderlich, Ph.D. Agenda 1. Eccentric Force àTorque (“Moment”) 2. Lever 3. Force Couple 4. Conservation of Angular Momentum 5. Centripetal and Centrifugal Forces ROTARY FORCE (“Eccentric Force”) § Force not in line with object’s center of gravity § Rotary and translatory motion can occur Fig 13.2 Torque (“Moment”) T = F x d F Moment T = F x d Arm F d = 0.3 cos (90-45) Fig 13.3 T = F x d Moment Arm Torque changed by changing length of moment d arm W T = F x d d W Fig 13.4 Sum of Torques (“Moments”) T = F x d Fig 13.8 Sum of Torques (“Moments”) T = F x d § Sum of torques = 0 • A balanced seesaw • Linear motion if equal parallel forces overcome resistance • Rowers Force Couple T = F x d § Effect of equal parallel forces acting in opposite direction Fig 13.6 & 13.7 LEVER § “A rigid bar that can rotate about a fixed point when a force is applied to overcome a resistance” § Used to: – Balance forces – Favor force production – Favor speed and range of motion – Change direction of applied force External Levers § Small force to overcome large resistance § Crowbar § Large Range Of Motion to overcome small resistance § Hitting golf ball § Balance force (load) § Seesaw Anatomical Levers § Nearly every bone is a lever § The joint is fulcrum § Contracting muscles are force § Don’t necessarily resemble
    [Show full text]
  • Moment About an Axis.Pptx
    Moment of a force along an axis Couples “If you find yourself in a hole, stop digging.” –Will Rogers Objectives ¢ Understand the vector formulation for finding the component of a moment along an axis ¢ Understand the idea of a couple and the moment it produces 2 Moments Along an Axis, Couples Monday, September 24, 2012 1 Tools ¢ Basic Trigonometry ¢ Pythagorean Theorem ¢ Algebra ¢ Visualization ¢ Position Vectors ¢ Unit Vectors ¢ Reviews ¢ Cross Products ¢ Dot Products 3 Moments Along an Axis, Couples Monday, September 24, 2012 Review ¢ A moment is the tendency of a force to cause rotation about a point or an axis 4 Moments Along an Axis, Couples Monday, September 24, 2012 2 Moment about an Axis ¢ There are times that we are interested in the moment of a force that produces some component of rotation about (or along) a specific axis ¢ We can use all the we have learned up to this point to solve this type of problem 5 Moments Along an Axis, Couples Monday, September 24, 2012 Moment about an Axis ¢ First select any point on the axis of interest and find the moment of the force about that point ¢ Using the dot product and multiplication of the scalar times the unit vector of the axis, the component of the moment about the axis can be calculated 6 Moments Along an Axis, Couples Monday, September 24, 2012 3 Moment about an Axis ¢ If we have an axis a-a we can find the component of a moment along that axis by M = u u M a−a a−a ( a−a ) where M is the moment about any point on a-a 7 Moments Along an Axis, Couples Monday, September 24, 2012
    [Show full text]
  • Magnetic Dipoles Magnetic Field of Current Loop I
    PHY2061 Enriched Physics 2 Lecture Notes Magnetic Dipoles Magnetic Dipoles Disclaimer: These lecture notes are not meant to replace the course textbook. The content may be incomplete. Some topics may be unclear. These notes are only meant to be a study aid and a supplement to your own notes. Please report any inaccuracies to the professor. Magnetic Field of Current Loop z B θ R y I r x For distances R r (the loop radius), the calculation of the magnetic field does not depend on the shape of the current loop. It only depends on the current and the area (as well as R and θ): ⎧ μ cosθ B = 2 μ 0 ⎪ r 4π R3 B ==⎨ where μ iA is the magnetic dipole moment of the loop μ sinθ ⎪ B = μ 0 ⎩⎪ θ 4π R3 Here i is the current in the loop, A is the loop area, R is the radial distance from the center of the loop, and θ is the polar angle from the Z-axis. The field is equivalent to that from a tiny bar magnet (a magnetic dipole). We define the magnetic dipole moment to be a vector pointing out of the plane of the current loop and with a magnitude equal to the product of the current and loop area: μ K K μ ≡ iA i The area vector, and thus the direction of the magnetic dipole moment, is given by a right-hand rule using the direction of the currents. D. Acosta Page 1 10/24/2006 PHY2061 Enriched Physics 2 Lecture Notes Magnetic Dipoles Interaction of Magnetic Dipoles in External Fields Torque By the FLB=×i ext force law, we know that a current loop (and thus a magnetic dipole) feels a torque when placed in an external magnetic field: τ =×μ Bext The direction of the torque is to line up the dipole moment with the magnetic field: F μ θ Bext i F Potential Energy Since the magnetic dipole wants to line up with the magnetic field, it must have higher potential energy when it is aligned opposite to the magnetic field direction and lower potential energy when it is aligned with the field.
    [Show full text]
  • Lecture 18: Planar Kinetics of a Rigid Body
    ME 230 Kinematics and Dynamics Wei-Chih Wang Department of Mechanical Engineering University of Washington Planar kinetics of a rigid body: Force and acceleration Chapter 17 Chapter objectives • Introduce the methods used to determine the mass moment of inertia of a body • To develop the planar kinetic equations of motion for a symmetric rigid body • To discuss applications of these equations to bodies undergoing translation, rotation about fixed axis, and general plane motion W. Wang 2 Lecture 18 • Planar kinetics of a rigid body: Force and acceleration Equations of Motion: Rotation about a Fixed Axis Equations of Motion: General Plane Motion - 17.4-17.5 W. Wang 3 Material covered • Planar kinetics of a rigid body : Force and acceleration Equations of motion 1) Rotation about a fixed axis 2) General plane motion …Next lecture…Start Chapter 18 W. Wang 4 Today’s Objectives Students should be able to: 1. Analyze the planar kinetics of a rigid body undergoing rotational motion 2. Analyze the planar kinetics of a rigid body undergoing general plane motion W. Wang 5 Applications (17.4) The crank on the oil-pump rig undergoes rotation about a fixed axis, caused by the driving torque M from a motor. As the crank turns, a dynamic reaction is produced at the pin. This reaction is a function of angular velocity, angular acceleration, and the orientation of the crank. If the motor exerts a constant torque M on Pin at the center of rotation. the crank, does the crank turn at a constant angular velocity? Is this desirable for such a machine? W.
    [Show full text]