Title | Linear and Angular Kinematics |
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Course | Biomechanics |
Institution | University of North Carolina at Charlotte |
Pages | 2 |
File Size | 127.9 KB |
File Type | |
Total Downloads | 113 |
Total Views | 190 |
Dr. Thomas...
Linear and Angular Kinematics Definitions Kinematics describes position, velocity, acceleration (disregards what causes motion Linear vs. Angular Motion Linear (meters): every part of the object experiences equivalent displacement If you (object) are walking in a straight line, every part of you will get from A to B (equivalent displacement) Angular: all parts of the object do not experience the same displacement Units: Degree Revolution Radian: ratio of circumference of a circle to its radius 1 revolution = 360deg 1 rev = 2pi radians = 6.28 radians Normal human movement encompasses linear and angular displacement Walking: you move linearly but your joints go through angular motion Throwing ball: arm moves angularly to project ball linearly Cycling Joint rotations create force on pedals Rotates gears wheels Results in linear motion of rider and bike Linear Motion Considerations Acceleration Defined as change in velocity WRT time Can have + or – value When direction of motion is described as something other than + or – + acceleration = speeding up - acceleration = speeding up If direction of motion is described as +/ Direction of motion dictates sign and negative acceleration may still be mean speeding up + = up, - = down May also have acceleration = 0 if moving at constant velocity Velocity tells you if you are moving or not, acceleration tells if speeding up or slowing down Average and Instantaneous Quantities Dictated by selection of time interval when analyzing motion Average is sometimes sufficient but may lose information depending on length of t Instantaneous important when considering projectile motion Velocity at release dictates how far an object will travel Angular Motion Angular Distance and Displacement Similar to linear motion Shoulder flexion Move from 00 to 900 Distance: 900 Displacement: 900 If we now return to 00 Distance: 1800 (90 + 90) Displacement: 00 Sign convention: clockwise motion is (-), counterclockwise motions are (+) Angular speed and Velocity Angular speed: angular distance/change in time Angular velocity: angular displacement/change in time
What are common angular velocities experienced during sports? Baseball pitching Elbow: 2320 0/s of extension Shoulder: 7240 0/s of IR Tennis serve Elbow: 1510 0/s of extension Shoulder: 2420 0/s of IR **Baseball faster than tennis, shoulder faster than elbow Angular Acceleration Change in angular velocity/change in time Relation Between Linear and Angular Motion Linear and Angular Displacement The greater the radius b/w a given point on a rotating body and its axis of rotation, the greater the linear distance covered by that point during an angular motion S: curvilinear distance R: radius of rotation Phi: angular displacement Curvilinear distance traveled by the point of interest is the product of the point’s radius of rotation and angular distance through which the rotating body moves Unit: radians Equation is only valid if Linear distance and radius of rotation are measured in the same units Angular distance must be expressed in radians Linear and Angular Velocity Consider baseball (or tennis, golf, etc) The greater R with which bat hits ball = greater linear velocity imparted on ball The greater radius of the bat, the greater the linear velocity at that point, the faster the ball leaves the bat, the farther that it can travel R = radius of rotation Omega = angular velocity Angular velocity is constant Linear and Angular Acceleration Acceleration of a body with angular motion has 2 components Tangential Radial Tangential Acceleration Ball will follow curved path while in pitcher’s hand (because moving around elbow’s fulcrum) Tangential component represents change in linear speed of ball (what is the linear speed of the ball at that one spot in the arc of motion) Goal is to maximize tangential velocity to throw far or fast Once ball is released, tangential acceleration = 0 b/c pitcher is no longer applying force Association b/w linear and angular Looks exactly like v= r x omega Take tangential acceleration, set it equal to the radius times the angular acceleration Radial Acceleration Rate of change in direction of a body in angular motion Always directed toward center of curvature (radius of rotation, center of circular motion) Ball follows curved path (until release) b/c hand restrains it Restraining force causes radial acceleration Upon release radial acceleration = 0 Ball follows path of tangent to curve at instant release Where release occurs dictates where ball ends up...