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PHYS 1441 – Section 002 Lecture #9 Wednesday, Feb. 13, 2008 Dr. Jaehoon Yu • • Motion in Two Dimensions – Projectile Motion – Maximum ranges and heights Newton’s Laws of Motion – Force – Newton’s first law: Inertia & Mass – Newton’s second law Wednesday, Feb. 13, 2008 PHYS 1441-002, Spring 2008 Dr. Jaehoon Yu 1 Announcements • 1st term exam next Wednesday, Feb. 20 – – – – – Time: 1 – 2:20pm Place: SH103 Covers: Appendices, CH 1 – CH4.4 Style: mixture of multiple choices and essay problems Class on Monday, Feb. 18: Jason will be here to go over the any problems you would like to review • Colloquium today – UTA Physics faculty research topics – Good opportunity to learn what UTA Physics does – Possibly working with them if you are interested in… Wednesday, Feb. 13, 2008 PHYS 1441-002, Spring 2008 Dr. Jaehoon Yu 2 Reminder: Special Project • Show that a projectile motion’s trajectory is a parabola!! – 20 points – Due: Wednesday, Feb. 27 – You MUST show full details of computations to obtain any credit Wednesday, Feb. 13, 2008 PHYS 1441-002, Spring 2008 Dr. Jaehoon Yu 3 Wednesday, Feb. 13, 2008 PHYS 1441-002, Spring 2008 Dr. Jaehoon Yu 4 Projectile Motion • A 2-dim motion of an object under the gravitational acceleration with the following assumptions – Free fall acceleration, g, is constant over the range of the motion r r • g 9.8 j m s 2 • ax 0 m s 2 and a y 9.8m s 2 – Air resistance and other effects are negligible • A motion under constant acceleration!!!! Superposition of two motions – Horizontal motion with constant velocity ( no acceleration ) v xf vx 0 – Vertical motion under constant acceleration ( g ) v v a t v 9.8 Wednesday, Feb. 13, yf 2008 y0 t Spring 2008 y PHYS 1441-002, y0 Dr. Jaehoon Yu 5 Kinematic Equations in 2-Dim x-component y-component vx vxo axt v y v yo a y t x 1 2 vxo vx t 2 y 2 xo x vxot axt 1 2 Wednesday, Feb. 13, 2008 v yo vy t v v 2ay y v v 2a x x 2 x y 1 2 2 2 yo y vyot ayt PHYS 1441-002, Spring 2008 Dr. Jaehoon Yu 1 2 2 6 Show that a projectile motion is a parabola!!! x-component vxi vi cos v yi vi sin i y-component a axi a y j gj ax=0 x f vxi t vi cos i t t xf vi cos i In a projectile motion, the only acceleration is gravitational one whose direction is always toward the center of the earth (downward). 1 2 1 2 v sin t gt y f v yi t g t i i 2 2 Plug t into the above xf xf 1 y f vi sin i 2 g v cos i i vi cos i g y f x f tan i 2 2 2 v cos i i Wednesday, Feb. 13, 2008 PHYS 1441-002, Spring 2008 Dr. Jaehoon Yu 2 x f 2 What kind of parabola is this? 7 Projectile Motion Maximum height Wednesday, Feb. 13, 2008 The only acceleration in this PHYS 1441-002, Spring 2008 Dr. Jaehoon motion. It isYua constant!! 8 Example 6 The Height of a Kickoff A placekicker kicks a football at and angle of 40.0 degrees and the initial speed of the ball is 22 m/s. Ignoring air resistance, determine the maximum height that the ball attains. Wednesday, Feb. 13, 2008 PHYS 1441-002, Spring 2008 Dr. Jaehoon Yu 9 First, the initial velocity components v0 22 m s v0 y 40 v0 x vox vo cos 22m s cos 40 17 m s voy vo sin 22m s sin 40 14 m s Wednesday, Feb. 13, 2008 PHYS 1441-002, Spring 2008 Dr. Jaehoon Yu 10 Motion in y-direction is of the interest.. y ay vy voy ? -9.8 m/s2 0 m/s +14 m/s Wednesday, Feb. 13, 2008 PHYS 1441-002, Spring 2008 Dr. Jaehoon Yu t 11 Now the nitty, gritty calculations… y ay vy voy ? -9.80 m/s2 0 14 m/s t What happens at the maximum height? The ball’s velocity in y-direction becomes 0!! And the ball’s velocity in x-direction? Stays the same!! Why? Because there is no acceleration in xdirection!! Which kinematic formula would you like to use? v v 2ay y 2 y 2 oy y Wednesday, Feb. 13, 2008 Solve for y y 0 14 m s 2 9.8 m s 2 2 v y2 voy2 2a y 10 m PHYS 1441-002, Spring 2008 Dr. Jaehoon Yu 12 Example 7 The Time of Flight of a Kickoff What is the time of flight between kickoff and landing? Wednesday, Feb. 13, 2008 PHYS 1441-002, Spring 2008 Dr. Jaehoon Yu 13 What is y when it reached the max range? y ay 0m -9.80 m/s2 Wednesday, Feb. 13, 2008 vy PHYS 1441-002, Spring 2008 Dr. Jaehoon Yu voy t 14 m/s ? 14 Now solve the kinematic equations in y direction!! y ay 0 -9.80 m/s2 y voyt ayt 1 2 Two soultions 2 t 0 voy 12 a y t 0 Wednesday, Feb. 13, 2008 vy Since y=0 voy t 14 m/s ? 0 voyt ayt t voy 12 a y t 1 2 2 or Solve for t voy 2voy 2 14 2.9 s t 9.8 1 a y ay 2 PHYS 1441-002, Spring 2008 Dr. Jaehoon Yu 15 Ex. 8 The Range of a Kickoff Calculate the range R of the projectile. 2 1 v t a t x ox 2 x vox t 17 m s 2.9 s 49 m Wednesday, Feb. 13, 2008 PHYS 1441-002, Spring 2008 Dr. Jaehoon Yu 16 Projectile Motion Wednesday, Feb. 13, 2008 The only acceleration in this PHYS 1441-002, Spring 2008 Dr. Jaehoon motion. It isYua constant!! 17 Horizontal Range and Max Height • Based on what we have learned in the previous lecture, one can analyze a projectile motion in more detail – Maximum height an object can reach – Maximum range What happens at the maximum height? At the maximum height the object’s vertical motion stops to turn around!! v yf v0 y a y t v0 sin 0 gt A 0 Solve for tA Wednesday, Feb. 13, 2008 v0 sin 0 tA g PHYS 1441-002, Spring 2008 Dr. Jaehoon Yu Time to reach to the maximum height!! 18 Horizontal Range and Max Height Since no acceleration is in x direction, it still flies even if vy=0. v0 sin 0 R v0 xt v0 x 2t A 2v0 cos 0 g v0 2 sin 20 Range R y f h v0 y t Height g 1 v0 sin 0 2 g t v0 sin 0 g 2 1 2 v0 sin 0 g g v0 2 sin 2 0 yf h 2g Wednesday, Feb. 13, 2008 PHYS 1441-002, Spring 2008 Dr. Jaehoon Yu 19 2 Maximum Range and Height • What are the conditions that give maximum height and range of a projectile motion? v0 sin 0 h 2g 2 2 v02 sin 20 R g Wednesday, Feb. 13, 2008 This formula tells us that the maximum height can be achieved when i=90o!!! This formula tells us that the maximum range can be achieved when 2i=90o, i.e., i=45o!!! PHYS 1441-002, Spring 2008 Dr. Jaehoon Yu 20 Force We’ve been learning kinematics; describing motion without understanding what the cause of the motion is. Now we are going to learn dynamics!! FORCE is what causes an object to move. Can someone tell me The above statement is not entirely correct. Why? what FORCE is? Because when an object is moving with a constant velocity no force is exerted on the object!!! FORCEs are what cause any changes to the velocity of an object!! What does this statement mean? What happens if there are several forces being exerted on an object? F1 F2 Wednesday, Feb. 13, 2008 NET FORCE, F= F1+F2 When there is force, there is change of velocity!! What does force cause? It causes an acceleration.!! Forces are vector quantities, so vector sum of all forces, the NET FORCE, determines the direction of the acceleration of the object. When the net force on an object is 0, it has constant velocity and is at its equilibrium!! PHYS 1441-002, Spring 2008 Dr. Jaehoon Yu 21 More Force There are various classes of forces Contact Forces: Forces exerted by physical contact of objects Examples of Contact Forces: Baseball hit by a bat, Car collisions Field Forces: Forces exerted without physical contact of objects Examples of Field Forces: Gravitational Force, Electro-magnetic force What are possible ways to measure strength of the force? A calibrated spring whose length changes linearly with the force exerted . Forces are vector quantities, so the addition of multiple forces must be done following the rules of vector additions. Wednesday, Feb. 13, 2008 PHYS 1441-002, Spring 2008 Dr. Jaehoon Yu 22 Newton’s First Law and Inertial Frames Aristotle (384-322BC): A natural state of a body is rest. Thus force is required to move an object. To move faster, ones needs larger forces. Galileo’s statement on natural states of matter: Any velocity once imparted to a moving body will be rigidly maintained as long as the external causes of retardation are removed!! Galileo’s statement is formulated by Newton into the 1st law of motion (Law of Inertia): In the absence of external forces, an object at rest remains at rest and an object in motion continues in motion with a constant velocity. What does this statement tell us? • • • When no force is exerted on an object, the acceleration of the object is 0. Any isolated object, the object that do not interact with its surroundings, is either at rest or moving at a constant velocity. Objects would like to keep its current state of motion, as long as there are no forces that interfere with the motion. This tendency is called the Inertia. A frame of reference that is moving at a constant velocity is called the Inertial Frame Is a frame of reference with an acceleration an Inertial Frame? Wednesday, Feb. 13, 2008 PHYS 1441-002, Spring 2008 Dr. Jaehoon Yu NO! 23