ME 012 Engineering Dynamics Lecture 2 Rectilinear Kinematics: Erratic Motion (Chapter 12, Section3) Thursday, Jan. 17, 2013 ME 012 Engineering Dynamics: Lecture 2 J. M. Meyers, Ph.D. (jmmeyers@uvm.edu) 12.3 Rectilinear Kinematics: Erratic Motion Today’s Objectives: Determine position, velocity, and acceleration of a particle using graphs. In-Class Activities: Applications s-t, v-t, a-t, v-s, and a-s diagrams Group Problem Solving ME 012 Engineering Dynamics: Lecture 2 J. M. Meyers, Ph.D. (jmmeyers@uvm.edu) 2 12.3 Rectilinear Kinematics: Erratic Motion Graphing provides a good way to handle complex motions that would be difficult to describe with formulas. Graphs also provide a visual description of motion and reinforce the calculus concepts of differentiation and integration as used in dynamics. The approach builds on the facts that slope and differentiation are linked and that integration can be thought of as finding the area under a curve. ME 012 Engineering Dynamics: Lecture 2 J. M. Meyers, Ph.D. (jmmeyers@uvm.edu) 3 12.3 Rectilinear Kinematics: Erratic Motion s-t GRAPH Plots of position vs. time can be used to find velocity vs. time curves. Finding the slope of the line tangent to the motion curve at any point is the velocity at that point (instantaneous velocity or v = ds/dt). s-t to v-t Therefore, the v-t graph can be constructed by finding the slope at various points along the s-t graph. ME 012 Engineering Dynamics: Lecture 2 J. M. Meyers, Ph.D. (jmmeyers@uvm.edu) 4 12.3 Rectilinear Kinematics: Erratic Motion v-t GRAPH Plots of velocity vs. time can be used to find acceleration vs. time curves. Finding the slope of the line tangent to the velocity curve at any point is the acceleration at that point (instantaneous acceleration or a = dv/dt). v-t to a-t Also, the distance moved (displacement) of the particle is the area under the v-t graph during time ∆t. Therefore, the a-t graph can be constructed by finding the slope at various points along the v-t graph. ME 012 Engineering Dynamics: Lecture 2 J. M. Meyers, Ph.D. (jmmeyers@uvm.edu) 5 12.3 Rectilinear Kinematics: Erratic Motion v-t GRAPH Given the v-t curve, we can also calculate the change in position (∆s) during a time period… this is the area under the v-t curve by the definition of an integral: v-t to s-t ∆ = d Area under v-t graph So we can construct an s-t graph from an v-t graph if we know the initial position of the particle. ME 012 Engineering Dynamics: Lecture 2 J. M. Meyers, Ph.D. (jmmeyers@uvm.edu) 6 12.3 Rectilinear Kinematics: Erratic Motion a-t GRAPH Given the a-t curve, the change in velocity (∆v) during a time period is the area under the a-t curve. a-t to v-t So we can construct a v-t graph from an a-t graph if we know the initial velocity of the particle. ME 012 Engineering Dynamics: Lecture 2 J. M. Meyers, Ph.D. (jmmeyers@uvm.edu) 7 12.3 Rectilinear Kinematics: Erratic Motion a-s GRAPH A more complex case is presented by the a-s graph. The area under the acceleration versus position curve represents the change in velocity (recall ∫ a ds = ∫ v dv ). 1 2 − = d a-s to v-s 1 2 − = d Area under a-s graph This equation can be solved for v1, allowing you to solve for the velocity at a point. By doing this repeatedly, you can create a plot of velocity versus distance. ME 012 Engineering Dynamics: Lecture 2 J. M. Meyers, Ph.D. (jmmeyers@uvm.edu) 8 12.3 Rectilinear Kinematics: Erratic Motion v-s GRAPH v-s to a-s Another more complex case is presented by the v-s graph. By reading the velocity v at a point on the curve and multiplying it by the slope of the curve (dv/ds) at this same point, we can obtain the acceleration at that point: a = v (dv/ds) Thus, we can obtain a plot of a vs. s from the vs curve. ME 012 Engineering Dynamics: Lecture 2 J. M. Meyers, Ph.D. (jmmeyers@uvm.edu) 9 12.3 Rectilinear Kinematics: Erratic Motion EXAMPLE 1 (in text) In many experiments, a velocity versus position (v-s) profile is obtained. If we have a v-s graph for the motorcycle, can we construct the a-s graph of the motion and determine the time needed for the motorcycle to reach the position s = 400 feet? ME 012 Engineering Dynamics: Lecture 2 J. M. Meyers, Ph.D. (jmmeyers@uvm.edu) 10 12.3 Rectilinear Kinematics: Erratic Motion EXAMPLE 1: Solution ME 012 Engineering Dynamics: Lecture 2 J. M. Meyers, Ph.D. (jmmeyers@uvm.edu) 11 12.3 Rectilinear Kinematics: Erratic Motion EXAMPLE 2 Given: v-t graph for a train moving between two stations Find: a-t graph and s-t graph over this time interval Think about your plan of attack for the problem! ME 012 Engineering Dynamics: Lecture 2 J. M. Meyers, Ph.D. (jmmeyers@uvm.edu) 12 12.3 Rectilinear Kinematics: Erratic Motion EXAMPLE 2: Solution ME 012 Engineering Dynamics: Lecture 2 J. M. Meyers, Ph.D. (jmmeyers@uvm.edu) 13 12.3 Rectilinear Kinematics: Erratic Motion EXAMPLE 3 Given: The v-t graph shown. The car starts from rest at s = 0 Find: 1) The a-t graph and determine the maximum acceleration during the 30 s interval. 2) Draw the s-t graph and determine the average speed and the distance travelled for the 30 s interval. Plan: Find slopes of the curves and draw the v-t graph. Find the area under the curve… that is the distance traveled. Finally, calculate equation for s-t diagram and find average speed (using basic definitions!). ME 012 Engineering Dynamics: Lecture 2 J. M. Meyers, Ph.D. (jmmeyers@uvm.edu) 14 12.3 Rectilinear Kinematics: Erratic Motion EXAMPLE 4: Solution (1/2) ME 012 Engineering Dynamics: Lecture 2 J. M. Meyers, Ph.D. (jmmeyers@uvm.edu) 15 12.3 Rectilinear Kinematics: Erratic Motion EXAMPLE 4: Solution (2/2) ME 012 Engineering Dynamics: Lecture 2 J. M. Meyers, Ph.D. (jmmeyers@uvm.edu) 16