Storyline Chapter 2: Motion in One Dimension Physics for Scientists and Engineers, 10e Raymond A. Serway John W. Jewett, Jr. Position position x: location of particle with respect to chosen reference point Displacement Displacement x of particle: change in position in a given time interval x x f − xi Distance and Displacement Vector quantity requires specification of both direction and magnitude Scalar quantity has numerical value and no direction Position, Velocity, and Speed of a Particle Quick Quiz 2.1 Which of the following choices best describes what can be determined exactly from the table and figure for the entire 50-s interval? (a) The distance the car moved. (b) The displacement of the car. (c) Both (a) and (b). (d) Neither (a) nor (b). Quick Quiz 2.1 Which of the following choices best describes what can be determined exactly from the table and figure for the entire 50-s interval? (a) The distance the car moved. (b) The displacement of the car. (c) Both (a) and (b). (d) Neither (a) nor (b). Position, Velocity, and Speed of a Particle vx ,avg x t Average Velocity 52 m − 30 m Example: = 2.2 m/s 10 s − 0 Average Speed Average speed of particle (scalar quantity): total distance d traveled divided by elapsed time t vavg vavg d t 75 m = = +1.36 m/s 55.0 s 125 m average speed = = 2.27 m/s 55.0 s Example 2.1: Calculating the Average Velocity and Speed Find the displacement, average velocity, and average speed of the car in the figure between positions A and F. x = xF − xA = −53 m − 30 m = −83 m Example 2.1: Calculating the Average Velocity and Speed Average velocity: vx ,avg xF − xA = tF − tA −53 m − 30 m = 50 s − 0 s −83 m = = −1.7 m/s 50 s Example 2.1: Calculating the Average Velocity and Speed Average speed: vavg 127 m = = 2.54 m/s 50.0 s Instantaneous Velocity and Speed x dx vx lim = t → 0 t dt Quick Quiz 2.3 Members of the highway patrol are more interested in (a) your average speed or (b) your instantaneous speed as you drive. Quick Quiz 2.3 Members of the highway patrol are more interested in (a) your average speed or (b) your instantaneous speed as you drive. Example 2.3: Average and Instantaneous Velocity A particle moves along the x axis. Its position varies with time according to the expression x = −4t + 2t2, where x is in meters and t is in seconds. The position–time graph for this motion is shown in the figure. Because the position of the particle is given by a mathematical function, the motion of the particle is known at all times. Notice that the particle moves in the negative x direction for the first second of motion, is momentarily at rest at the moment t = 1 s, and moves in the positive x direction at times t > 1 s. Example 2.3: Average and Instantaneous Velocity (A) Determine the displacement of the particle in the time intervals t = 0 to t = 1 s and t = 1 s to t = 3 s. xA → B = x f − xi = xB − xA 2 2 = −4 (1) + 2 (1) − −4 ( 0 ) + 2 ( 0 ) = −2 m xB→ D = x f − xi = xD − xB 2 2 = −4 ( 3) + 2 ( 3) − −4 (1) + 2 (1) = +8 m Example 2.3: Average and Instantaneous Velocity (B) Calculate the average velocity during these two time intervals. vx ,avg ( A → B) vx ,avg ( B→ D ) xA → B −2 m = = = −2 m/s t 1s xB→ D 8 m = = = +4 m/s t 2s Example 2.3: Average and Instantaneous Velocity (C) Find the instantaneous velocity of the particle at t = 2.5 s. vx = 10 m − ( −4 m ) 3.8 s − 1.5 s = +6 m/s Analysis Model: Particle Under Constant Velocity Analysis model: represents common situation when solving physics problems Analysis Model: Particle Under Constant Velocity vx ,avg x x → vx = t t x = x f − xi → vx = x f − xi t x f = xi + vx t x f = xi + vx t ( for constant vx ) Analysis Model: Particle Under Constant Velocity x vx = t x f = xi + vx t ( for constant vx ) Analysis Model: Particle Under Constant Velocity x = xi + vi t Example 2.4: Modeling a Runner as a Particle A kinesiologist is studying the biomechanics of the human body. (Kinesiology is the study of the movement of the human body. Notice the connection to the word kinematics.) She determines the velocity of an experimental subject while he runs along a straight line at a constant rate. The kinesiologist starts the stopwatch at the moment the runner passes a given point and stops it after the runner has passed another point 20 m away. The time interval indicated on the stopwatch is 4.0 s. Example 2.4: Modeling a Runner as a Particle (A) What is the runner’s velocity? x x f − xi 20 m − 0 vx = = = = 5.0 m/s t t 4.0 s Example 2.4: Modeling a Runner as a Particle (B) If the runner continues his motion after the stopwatch is stopped, what is his position after 10 s have passed? x f = xi + vx t = 0 = 0 + ( 5.0 m/s )(10 s ) = 50 m/s Analysis Model: Particle Under Constant Speed d v= t d d 2 r 2 (10.0 m ) v= → t = = = = 12.6 s t v v 5.00 m/s Analysis Model: Particle Under Constant Velocity x constant velocity: vx = t position as a function of time: x f = xi + vx t Analysis Model: Particle Under Constant Speed d constant speed: v = t Analysis Model Approach to Problem-Solving • Conceptualize • Categorize • Analyze • Finalize Average Acceleration ax ,avg vx vxf − vxi = t t f − ti Instantaneous Acceleration vx dvx ax lim = t → 0 t dt Acceleration vs. Time Graph Acceleration dvx d dx d 2 x ax = = = 2 dt dt dt dt Conceptual Example 2.5: Graphical Relationships Between x, vx, and ax The position of an object moving along the x axis varies with time as in the figure. Graph the velocity versus time and the acceleration versus time for the object. Conceptual Example 2.5: Graphical Relationships Between x, vx, and ax Conceptual Example 2.5: Graphical Relationships Between x, vx, and ax Example 2.6: Average and Instantaneous Acceleration The velocity of a particle moving along the x axis varies according to the expression vx = 40 − 5t2, where vx is in meters per second and t is in seconds. Example 2.6: Average and Instantaneous Acceleration (A) Find the average acceleration in the time interval t = 0 to t = 2.0 s. vxA = 40 − 5tA 2 = 40 − 5 ( 0 ) = +40 m/s 2 vxB = 40 − 5tB 2 = 40 − 5 ( 2.0 ) = +20 m/s 2 ax ,avg = vxf − vxi t f − ti = = −10 m/s 2 vxB − vxA 20 m/s − 40 m/s = tB − t A 2.0 s − 0 s Example 2.6: Average and Instantaneous Acceleration (B) Determine the acceleration at t = 2.0 s. vxf = 40 − 5 ( t + t ) = 40 − 5t − 10t t − 5 ( t ) 2 2 vx = vxf − vxi = −10t t − 5 ( t ) 2 vx ax = lim = lim ( −10t − 5t ) = −10t t → 0 t t → 0 ax = ( −10 )( 2.0 ) m/s 2 = −20 m/s 2 2 Motion Diagrams Quick Quiz 2.6 Which one of the following statements is true? (a) If a car is traveling eastward, its acceleration must be eastward. (b) If a car is slowing down, its acceleration must be negative. (c) A particle with constant acceleration can never stop and stay stopped. Quick Quiz 2.6 Which one of the following statements is true? (a) If a car is traveling eastward, its acceleration must be eastward. (b) If a car is slowing down, its acceleration must be negative. (c) A particle with constant acceleration can never stop and stay stopped. Analysis Model: Particle Under Constant Acceleration ax = vxf − vxi t −0 vxf = vxi + ax t ( for constant ax ) vx ,avg = vxi + vxf 2 ( for constant ax ) Analysis Model: Particle Under Constant Acceleration vxi + vxf x vx ,avg = , vx ,avg = t 2 x = x f − xi , t = t f − ti = t − 0 = t 1 x f − xi = vx , avg t = ( vxi + vxf ) t 2 1 x f = xi + ( vxi + vxf ) t 2 ( for constant ax ) Analysis Model: Particle Under Constant Acceleration 1 vxf = vxi + ax t substitute into x f = xi + ( vxi + vxf ) t 2 1 x f = xi + vxi + ( vxi + ax t ) t 2 1 2 x f = xi + vxi t + ax t 2 ( for constant ax ) Analysis Model: Particle Under Constant Acceleration vxf = vxi + ax t → t = vxf − vxi ax 1 substitute into x f = xi + ( vxi + vxf ) t 2 vxf − vxi 1 x f = xi + ( vxi + vxf ) 2 ax vxf2 = vxi2 +2ax ( x f − xi ) = xi + vxf2 − vxi2 2ax ( for constant ax ) Analysis Model: Particle Under Constant Acceleration vxf = vxi + ax t 1 2 x f = xi + vx t + ax t 2 vxf = vxi = vx when ax = 0 x f = xi + vx t Kinematic Equations vxf = vxi + ax t vx ,avg = vxi + vxf 2 1 x f = xi + ( vxi + vxf ) t 2 1 2 x f = xi + vxi t + ax t 2 vxf 2 = vxi 2 + 2ax ( x f − xi ) ( 2.13) ( 2.14 ) ( 2.16 ) ( 2.15 ) ( 2.17 ) Constant acceleration only! Quick Quiz 2.7 In the figure, match each vx–t graph on the top with the ax–t graph on the bottom that best describes the motion. Quick Quiz 2.7 In the figure, match each vx–t graph on the top with the ax–t graph on the bottom that best describes the motion. (a)–(e), (b)–(d), (c)–(f) Analysis Model: Particle Under Constant Acceleration vxf = vxi + ax t vx ,avg = vxi + vxf 2 1 x f = xi + ( vxi + vxf ) t 2 1 2 x f = xi + vxi t + ax t 2 vxf 2 = vxi 2 + 2ax ( x f − xi ) Example 2.10: Not a Bad Throw for a Rookie! A stone thrown from the top of a building is given an initial velocity of 20.0 m/s straight upward. The stone is launched 50.0 m above the ground, and the stone just misses the edge of the roof on its way down as shown in the figure. Example 2.10: Not a Bad Throw for a Rookie! (A) Using tA = 0 as the time the stone leaves the thrower’s hand at position A, determine the time at which the stone reaches its maximum height. v yf = v yi + a y t t = v yf − v yi ay = v yB − v yA −g 0 − 20.0 m/s t = tB = = 2.04 s 2 −9.80 m/s Example 2.10: Not a Bad Throw for a Rookie! (B) Find the maximum height of the stone (above its initial position). ymax 1 2 = yB = y A + vxAt + a y t 2 yB = 0 + ( 20.0 m/s )( 2.04 s ) 1 2 2 + ( −9.8 m/s ) ( 2.04 s ) = 20.4 m 2 Example 2.10: Not a Bad Throw for a Rookie! (C) Determine the velocity of the stone when it returns to the height from which it was thrown. v yC 2 = v yA 2 + 2a y ( yC − yA ) v yC = ( 20.0 m/s ) + 2 ( −9.80 m/s 2 ) ( 0 − 0 ) 2 2 = 400 m /s 2 2 v yC = −20.0 m/s Example 2.10: Not a Bad Throw for a Rookie! (D) Find the velocity and position of the stone at t = 5.00 s. v yD = v yA + a y t = 20.0 m/s + ( −9.80 m/s 2 ) ( 5.00 s ) = −29.0 m/s 1 2 yD = yA + v yA t + a y t 2 1 2 2 = 0 + ( 20.0 m/s )( 5.00 s ) + ( −9.80 m/s ) ( 5.00 s ) 2 = −22.5 m Example 2.10: Not a Bad Throw for a Rookie! What if the throw were from 30.0 m above the ground instead of 50.0 m? Which answers in parts (A) to (D) would change? None of the answers would change.