Welcome back to Physics 215 Lecture 2-2 Physics 215 – Fall 2016 02-2 Slide 1 • Last time: – Displacement, velocity, graphs • Today: – Constant acceleration, free fall Physics 215 – Fall 2016 02-2 Slide 2 2-2.1: An object moves with constant acceleration, starting from rest at t = 0 s. In the first four seconds, it travels 10 cm. What will be the displacement of the object in the following four seconds (i.e. between t = 4 s and t = 8 s)? A. B. C. D. 10 cm 20 cm 30 cm 40 cm Physics 215 – Fall 2016 02-2 Slide 3 Motion with constant acceleration: v = vi + at vav = (1/2) (vi + v) x = xi + vit + (1/2) a t2 v2 = vi2 + 2a (x - xi) *where xi, vi refer to time = 0 s ; x, v to time t Physics 215 – Fall 2016 02-2 Slide 4 Sample problem • A brick is dropped (zero initial speed) from the roof of a building. The brick strikes the ground in 2.50 s. Ignore air resistance, so the brick is in free fall. – How tall, in meters, is the building? – What is the magnitude of the brick s velocity just before it reaches the ground? – Sketch a(t), v(t), and y(t) for the motion of the brick. Physics 215 – Fall 2016 02-2 Slide 5 Sample problem • A student standing on the ground throws a ball straight up. The ball leaves the student’s hand with a speed of 15 m/s when the hand is 2.0 m above the ground. How long is the ball in the air before it hits the ground? – Assume that the student moves her hand out of the way. Physics 215 – Fall 2016 02-2 Slide 6 Sample problem • A cheetah spots a Thomson’s gazelle, its preferred prey, and leaps into action, quickly accelerating to its top speed of 30 m/s, the highest of any land animal. However, a cheetah can maintain this extreme speed for only 15 s before having to let up. The cheetah is 170 m from the gazelle as it reaches top speed, and the gazelle sees the cheetah at just this instant. With negligible reaction time, the gazelle heads directly away from the cheetah, accelerating at 4.6 m/s2 for 5.0 s, then running at constant speed. Does the gazelle escape? If so, by what distance is the gazelle in front when the cheetah gives up? Physics 215 – Fall 2016 02-2 Slide 7 Sample problem • A sprinter can accelerate with constant acceleration for 4.0 s before reaching top speed. He can run the 100 meter dash in 10.0 s. What is his speed as he crosses the finish line? Physics 215 – Fall 2016 02-2 Slide 8 Motion in more than 1 dimension • Have seen that 1D kinematics is written in terms of quantities with a magnitude and a sign • Examples of 1D vectors • To extend to d > 1, we need a more general definition of vector Physics 215 – Fall 2016 02-2 Slide 9 Vectors: basic properties • are used to denote quantities that have magnitude and direction • can be added and subtracted • can be multiplied or divided by a number • can be manipulated graphically (i.e., by drawing them out) or algebraically (by considering components) Physics 215 – Fall 2016 02-2 Slide 10 Vectors: examples and properties • Some vectors we will encounter: position, velocity, force • Vectors commonly denoted by boldface letters, or sometimes arrow on top • Magnitude of A is written |A|, or no boldface and no absolute value signs • Some quantities which are not vectors: temperature, pressure, volume …. Physics 215 – Fall 2016 02-2 Slide 11 Drawing a vector • A vector is represented graphically by a line with an arrow on one end. • Length of line gives the magnitude of the vector. • Orientation of line and sense of arrow give the direction of the vector. • Location of vector in space does not matter -- two vectors with the same magnitude and direction are equivalent, independent of their location Physics 215 – Fall 2016 02-2 Slide 12 Adding vectors To add vector B to vector A • Draw vector A • Draw vector B with its tail starting from the tip of A • The sum vector A+B is the vector drawn from the tail of vector A to the tip of vector B. Physics 215 – Fall 2016 02-2 Slide 13 Multiplying vectors by a number A • Direction of vector not affected (care with negative numbers – see below) • Magnitude (length) scaled, e.g. 1x A = – 1*A=A – 2*A is given by arrow of twice length, but same direction – 0*A = 0 null vector 2x 0x – -A = -1*A is arrow of same length, -1 x but reversed in direction Physics 215 – Fall 2016 02-2 A A A = = = Slide 14 Physics 215 – Fall 2016 02-2 Slide 15 2-2.2: Which of the vectors in the second row shows Physics 215 – Fall 2016 02-2 Slide 16 ? Slide 3-20 QuickCheck 3.1 2-2.2: Which of the vectors in the second row shows Physics 215 – Fall 2016 02-2 Slide 17 ? Slide 3-21 QuickCheck 3.2 2-2.3: Which of the vectors in the second row shows 2 - Physics 215 – Fall 2016 02-2 Slide 18 ? Slide 3-27 QuickCheck 3.2 Clicker 2-2.3: Which of the vectors in the second row shows 2 - Physics 215 – Fall 2016 02-2 Slide 19 ? Slide 3-28 Projection of a vector How much a vector acts along some arbitrary direction Component of a vector Projection onto one of the coordinate axes (x, y, z) Physics 215 – Fall 2016 02-2 Slide 20 Components A = Ax + Ay y A A = axi + ayj j x i = unit vector in x direction i j = unit vector in y direction Projection of A along coordinate axes ax, ay = components of vector A Physics 215 – Fall 2016 02-2 Slide 21 More on vector components y • Relate components to direction (2D): ax = |A|cosθ, ay = |A|sinθ A j θ i or Ay x Ax • Direction: tanθ = ay/ax • Magnitude: |A|2 = ax2 + ay2 Physics 215 – Fall 2016 02-2 Slide 22 2-2.4: A bird is flying along a straight line in a direction somewhere East of North. After the bird has flown a distance of 2.5 miles, it is 2 miles North of where it started. How far to the East is it from its starting point? A. B. C. D. 0 miles 0.5 miles 1.0 mile 1.5 miles Physics 215 – Fall 2016 02-2 Slide 23 Why are components useful? • Addition: just add components e.g. if C = A + B cx = ax + bx; cy = ay + by • Subtraction similar y B j A • Multiplying a vector by a number – just multiply components: if D = n*A x i dx = n*ax; dy = n*ay • Even more useful in 3 (or higher) dimensions Physics 215 – Fall 2016 02-2 Slide 24 Sample problem Sam leaves his house and follows the following three step path: He heads 50.0 m due east. Then he travels 20.0m at 480 north of east. He then travels 70.0m 620 north of west. Sketch the graph of Sam’s path in two-dimensions. What is Sam’s net displacement? What is the total distance that Sam travels? If Sam moves at constant speed and the trip takes 100s, what is Sam’s speed? What is the magnitude of Sam’s average velocity? Physics 215 – Fall 2016 02-2 Slide 25 2D Motion in components Note: component of position vector along x-direction is the x-coordinate! y Q yQ s – vector position → s = xQi + yQj j i x xQ Physics 215 – Fall 2016 02-2 Slide 26 Displacement in 2D Motion y Δs sI sF s – vector position Displacement Δs = sF - sI, also a vector! O x Physics 215 – Fall 2016 02-2 Slide 27
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