Wednesday, Sept. 19, 2007 PHYS 1443-002, Fall 2007 Dr. Jaehoon Yu 1 PHYS 1443 – Section 002 Lecture #7 Wednesday, Sept. 19, 2007 Dr. Jaehoon Yu Motion.

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PHYS 1441 – Section 002 Lecture #7
PHYS 1443 – Section 003 Lecture #6
PHYS 1443 – Section 002 Lecture #8
PHYS 1443 – Section 002 Lecture #6
PHYS 1443 – Section 001 Lecture #4
PHYS 1443 – Section 003 Lecture #4
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PHYS 1441 – Section 002 Lecture #4
PHYS 1441 – Section 001 Lecture #6
PHYS 1443 – Section 004 Lecture #8
PHYS 1441 – Section 002 Lecture #9
PHYS 1443 – Section 001 Lecture #6
PHYS 1443 – Section 003 Lecture #3
PHYS 1443 – Section 003 Lecture #7
PHYS 1441 – Section 002 Lecture #8
PHYS 1441 – Section 002 Lecture #7
PHYS 1441 – Section 002 Lecture #8
PHYS 1441 – Section 002 Lecture #9
PHYS 1443 – Section 001 Lecture #6
PHYS 1441 – Section 002 Lecture #6
PHYS 1443 – Section 002 Lecture #7
PHYS 1441 – Section 501 Lecture #4
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Wednesday, Sept. 19, 2007 PHYS , Fall 2007 Dr. Jaehoon Yu 1 PHYS 1443 – Section 002 Lecture #7 Wednesday, Sept. 19, 2007 Dr. Jaehoon Yu Motion in Two Dimensions –Maximum ranges and heights Reference Frame and Relative Velocity Newton’s Laws of Motion –Force –Newton’s Law of Inertia & Mass –Newton’s second law of motion –Gravitational Force and Weight –Newton’s third law of motion

Wednesday, Sept. 19, 2007PHYS , Fall 2007 Dr. Jaehoon Yu 2 Announcements distribution list: 67 of you subscribed to the list so far –Will issue -3 extra credit points if not done by midnight Friday, Sept. 21

Wednesday, Sept. 19, 2007PHYS , Fall 2007 Dr. Jaehoon Yu 3

Wednesday, Sept. 19, 2007PHYS , Fall 2007 Dr. Jaehoon Yu 4 Announcements distribution list: 67 of you subscribed to the list so far –Will issue -3 extra credit points if not done by midnight Friday, Sept. 21 Homework site had massive failure about the time HW3 was due! –Many many of you communicated to me about the problem! Thanks! –Some of you submitted the homework despite the problems –But I extended the due till 7pm tonight! –Please submit ASAP. Let me know if you have any further problems! First term exam next Wednesday, Sept. 26 –1-2:20pm, SH103 –Covers Ch 1 to what we cover next Monday (~Ch4) There will be a quiz next Monday in the beginning of the class

Wednesday, Sept. 19, 2007PHYS , Fall 2007 Dr. Jaehoon Yu 5

Wednesday, Sept. 19, 2007PHYS , Fall 2007 Dr. Jaehoon Yu 6 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 At the maximum height the object’s vertical motion stops to turn around!! vivivivi  h What happens at the maximum height? Solve for tAtA

Wednesday, Sept. 19, 2007PHYS , Fall 2007 Dr. Jaehoon Yu 7 Horizontal Range and Max Height Since no acceleration is in x direction, it still flies even if v y =0. Range Height

Wednesday, Sept. 19, 2007PHYS , Fall 2007 Dr. Jaehoon Yu 8 Maximum Range and Height What are the conditions that give maximum height and range of a projectile motion? This formula tells us that the maximum height can be achieved when  i =90 o !!! This formula tells us that the maximum range can be achieved when 2  i =90 o, i.e.,  i =45 o !!!

Wednesday, Sept. 19, 2007PHYS , Fall 2007 Dr. Jaehoon Yu 9 Example for a Projectile Motion A stone was thrown upward from the top of a cliff at an angle of 37 o to horizontal with initial speed of 65.0m/s. If the height of the cliff is 125.0m, how long is it before the stone hits the ground? Since negative time does not exist. Becomes

Wednesday, Sept. 19, 2007PHYS , Fall 2007 Dr. Jaehoon Yu 10 Example cont’d What is the speed of the stone just before it hits the ground? What are the maximum height and the maximum range of the stone? Do these yourselves at home for fun!!!

Wednesday, Sept. 19, 2007PHYS , Fall 2007 Dr. Jaehoon Yu 11 Observations in Different Reference Frames Results of physical measurements in different reference frames could be different Observations of the same motion in a stationary frame would be different than the ones made in the frame moving together with the moving object. Consider that you are driving a car. To you, the objects in the car do not move while to the person outside the car they are moving in the same speed and direction as your car is. O Frame S r’ O’ Frame S’ The position vector r’ is still r’ in the moving frame S’no matter how much time has passed!! v0v0 The position vector r is no longer r in the stationary frame S when time t has passed. v0tv0t r How are these position vectors related to each other?

Wednesday, Sept. 19, 2007PHYS , Fall 2007 Dr. Jaehoon Yu 12 Relative Velocity and Acceleration The velocity and acceleration in two different frames of references can be denoted, using the formula in the previous slide: O Frame S r’ O’ Frame S’ v0v0 v0tv0t r Galilean transformation equation What does this tell you? The accelerations measured in two frames are the same when the frames move at a constant velocity with respect to each other!!! The earth’s gravitational acceleration is the same in a frame moving at a constant velocity wrt the earth.

Wednesday, Sept. 19, 2007PHYS , Fall 2007 Dr. Jaehoon Yu 13 Force We’ve been learning kinematics; describing motion without understanding what the cause of the motion is. Now we are going to learn dynamics!! Can someone tell me what FORCE is? FORCE is what causes an object to move. FORCEs are what cause any changes to the velocity of an object!! The above statement is not entirely correct. Why? Because when an object is moving with a constant velocity no force is exerted on the object!!! What does this statement mean? When there is force, there is change of velocity!! What happens if there are several forces being exerted on an object? Forces are vector quantities, so vector sum of all forces, the NET FORCE, determines the direction of the acceleration of the object. F1F1 F2F2 NET FORCE, F= F 1 +F 2 When the net force on an object is 0, it has constant velocity and is at its equilibrium!! What does force cause?It causes an acceleration.!!

Wednesday, Sept. 19, 2007PHYS , Fall 2007 Dr. Jaehoon Yu 14 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 Force? A calibrated spring whose length changes linearly with the force exerted. Forces are vector quantities, so addition of multiple forces must be done following the rules of vector additions.