PHYS 120 – Lecture 2 Announcements Reminder: Tutorials begin next week – on Tuesday, January 16th You will be working in groups of 3 (or maybe 4). Please fill out the “Tutorial Grouping Survey” in Canvas to help us place you into groups. This survey is due Friday January 12th at 11:59 PM. Note: The two free absences for tutorials are to be used when you’re sick or otherwise unable to attend. No need to contact your TA about your absence. iClicker Questions begin next week – on Monday, January 15th If you are not enrolled in the course yet and need access to Canvas, please send an email to: sjohnson@sfu.ca with your name, SFU email address and student number. PHYS 120 Today's Concepts: Dr. Bernd Stelzer a) Position, Velocity, Acceleration b) 1-D Kinematics, graphs and constant acceleration Pre-Lecture Thoughts Are there topics in this section that you still find confusing or that need further explanation? “I need help on the graphs, how to interpret the relationship between each of the three quantities.” “The idea behind solving question #2 was still a bit confusing, especially why it couldn’t be 2ft travelled between t=1s and 2s.” “Not so far. Although I haven't learned anti derivatives and integrals in Calculus II yet, but I will hopefully learn more about that before we require it in this course.” “I did not really find anything that confusing during this section of physics, I overall found it as a nice review to physics 12 since I did forget a lot of things.” 1D Position vs Time Graphs vavg = x t Displacement – change in position: Δx = x2 – x1 Time elapsed – change in time: Δt = t2 – t1 x Slope of the line drawn through the X2 two points X1 t1 t2 t Position vs Time Graphs vavg = x t Displacement Time elapsed Decrease the time interval x t2 t1 t Position vs Time Graphs Average Velocity vavg = x t Displacement Time elapsed Decrease the time interval x t1 t2 t 1D Position vs Time Graphs vavg = lim x t Decrease the time interval x t!0 dx v= dt Instantaneous velocity = time derivative of the position = the slope of the tangent line at time t t Slope = v t Differential Calculus Differentiation (taking a derivative) is a convenient method for calculating the constantly changing slope of a nonlinear curve. Consider a function where C and n are constants The first derivative of y with respect to x is: Example Discussion Question Which instantaneous velocity-vs-time graph goes with the position-vs-time graph on the left? x v v v v The v(t) vs. t graph is the slope of the x(t) vs. t graph. Slope begins with a constant positive value and later decreases to zero. PHYS120 10 Acceleration vs Time Graphs Slope = 0 Slope < 0 Slope > 0 Position a(t) is the slope of the v(t) vs. t graph a=0 a>0 a<0 PHYS120 11 Bridge Question: x(t), v(t), a(t) plots For the Position and Velocity curves shown on the left, which is the correct plot of acceleration vs. time? Position A negative slope positive slope B Position from Velocity vs Time Graph A velocity-vs-time graph can be made by finding the slope of the position-vs-time graph. slope v x v area A position-vs-time graph can be made by finding the area under the velocity-vs-time graph. – Let’s see how this works. PHYS120 13 Position from Velocity vs Time Graph x (m) v (m/s) Constant velocity 50 40 30 20 10 0 =vavg Δt = Δx Area = 30 m/s x 1 s = 30 m 0 1 2 3 4 t (s) 5 0 1 2 3 4 t (s) 5 180 150 120 90 60 30 0 Assuming x = 0 at t = 0 PHYS120 14 Position from Velocity vs Time Graph x (m) v (m/s) Constant velocity 50 40 30 20 10 0 Area = 30 m/s x 2 s = 60 m 0 1 2 3 4 t (s) 5 0 1 2 3 4 t (s) 5 180 150 120 90 60 30 0 PHYS120 15 Position from Velocity vs Time Graph x (m) v (m/s) Constant velocity 50 40 30 20 10 0 Area = 30 m/s x 3 s = 90 m 0 1 2 3 4 t (s) 5 0 1 2 3 4 t (s) 5 180 150 120 90 60 30 0 PHYS120 16 Position from Velocity vs Time Graph x (m) v (m/s) Constant velocity 50 40 30 20 10 0 Area = 30 m/s x 4 s = 120 m 0 1 2 3 4 t (s) 5 0 1 2 3 4 t (s) 5 180 150 120 90 60 30 0 PHYS120 17 Position from Velocity vs Time Graph v (m/s) Constant velocity 50 40 30 20 10 0 Area = 30 m/s x 5 s = 150 m x (m) 0 1 180 150 120 90 60 30 0 2 3 4 t (s) 5 3 4 t (s) 5 x = 30 t m =v 0 1 t 2 PHYS120 18 Position from Velocity vs Time Graph Linear increasing velocity v (m/s) 60 40 20 0 0 2 3 4 t (s) 5 1 Area = (10[m/s] ⇥ 1[s]) = 5m =vavg Δt = Δx 2 150 x (m) 1 100 50 0 0 1 2 3 4 PHYS120 t (s) 5 19 Constant Acceleration Linear increasing velocity v (m/s) 60 40 20 0 0 2 3 4 t (s) 5 1 Area = (20[m/s] ⇥ 2[s]) = 20m 2 150 x (m) 1 100 50 0 0 1 2 3 4 PHYS120 t (s) 5 20 Constant Acceleration Linear increasing velocity v (m/s) 60 40 20 0 0 2 3 4 t (s) 5 1 Area = (30[m/s] ⇥ 3[s]) = 45m 2 150 x (m) 1 100 50 0 0 1 2 3 4 PHYS120 t (s) 5 21 Constant Acceleration Linear increasing velocity v (m/s) 60 40 20 0 0 2 3 4 t (s) 5 1 Area = (40[m/s] ⇥ 4[s]) = 80m 2 150 x (m) 1 100 50 0 0 1 2 3 4 PHYS120 t (s) 5 22 Constant Acceleration Linear increasing velocity v (m/s) 60 40 20 0 0 2 3 4 t (s) 5 1 Area = (50[m/s] ⇥ 5[s]) = 125m 2 150 x (m) 1 100 50 0 0 1 2 3 4 PHYS120 t (s) 5 23 Constant Acceleration Linear increasing velocity v (m/s) 60 40 v=a t 20 0 0 1 2 3 4 2 3 4 t (s) 5 x (m) 150 1 x= a 2 100 50 t2 0 0 1 PHYS120 t (s) 5 24 Constant Acceleration Linear increasing velocity v (m/s) 60 40 20 0 0 1 2 3 4 3 4 t (s) 5 x (m) 150 100 slope increasing 50 0 0 1 2 PHYS120 t (s) 5 25 Position from Velocity vs Time Graph (vx is constant and >0) (vx is constant and <0) (vx varies with time) General v(t) vs. t curve. • The total displacement from t1 to t2 is the area under the curve for this interval. • This can be calculated by summing the areas of (infinitesimal) rectangles. (integral) N Δx = x f − xi = lim ∑ vx Δt = Δt→0 i=1 tf ∫ vx dt ti Don’t Panic! Discussion Question Which position-vs-time graph goes with the velocity-vs-time graph at the top? The particle’s position at t = 0 s is x0 = –10 m. Area > 0 Area < 0 dx/dt > 0 dx/dt < 0 Velocity from Acceleration vs Time Graph Constant acceleration a (m/s2) 15 10 5 Similarly, the area under a constant acceleration-vs-time graph gives a linear velocity-vs-time graph 0 0 1 2 3 4 t (s) 5 3 4 t (s) 5 v (m/s) 60 40 vf = vi + a t 20 0 0 1 2 PHYS120 28 Kinematic Equations In general: tf ti constant a(t) = a Throwing a ball vertically – free fall motion x vx > 0 vx < 0 Constant negative acceleration: ax= -9.81 m/s2 𝑣⃗ x=0 Slowing down as it rises: vx is positive and becoming smaller x(t),m Speeding up going down: vx is negative and becoming more negative PHYS120 30