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Physics 101: Lecture 04 Exam I Kinematics + Dynamics Today’s lecture will cover Textbook Chapter 4 Physics 101: Lecture 4, Pg 1 What’s Most Difficult I’m a little slow dusting off the trig skills. Identifying all forces involved with free body diagrams. …I think I just need some more practice walking through the thought process required to solve the problems. I am having a hard time with vectors in this class… The most difficult problems right now are 2 dimension analysis problems where you don’t know 2 variables so you have to end up substituting in one variable for the other and manipulating equations. Everything :( I LOVE Free Body Diagrams. The lectures don’t seem to explain much, just random letters and numbers… Physics 101: Lecture 4, Pg 2 05 Review Kinematics : Description of Motion Position Displacement Velocity v = Dx / Dt » average » instantaneous Acceleration a = Dv / Dt » average » Instantaneous Physics 101: Lecture 4, Pg 3 07 Preflight 4.1 …most trouble with deciphering graphs… (A) (B) (C) •Which x vs t plot shows positive acceleration? 90% got this correct!!!! “The slope of the graph is getting increasingly positive; the velocity is increasing over time.” Physics 101: Lecture 4, Pg 4 08 Equations for Constant Acceleration (text, page 108) x (meters) 200 150 100 50 0 x = x0 + v0t + 1/2 at2 v = v0 + at v2 = v02 + 2a(x-x0) Dx = v0t + 1/2 0 5 10 t (seconds) 15 20 5 10 t (seconds) 15 20 5 10 t (seconds) 15 20 v (m/s) at2 Dv = at 20 15 10 v2 = v02 + 2a Dx Lets derive this… 5 0 0 2 a (m/s ) 2 1.5 1 0.5 0 0 Physics 101: Lecture 4, Pg 5 10 Equations for Constant Acceleration (text, page 108) x (meters) 200 150 100 50 0 x = x0 + v0t + 1/2 at2 v = v0 + at v2 = v02 + 2a(x-x0) Dx = v0t + 1/2 0 5 10 t (seconds) 15 20 5 10 t (seconds) 15 20 5 10 t (seconds) 15 20 v (m/s) at2 Dv = at 20 15 10 v2 = v02 + 2a Dx 5 0 0 2 a (m/s ) 2 1.5 1 0.5 0 0 Physics 101: Lecture 4, Pg 6 14 Kinematics Example A car is traveling 30 m/s and applies its breaks to stop after a distance of 150 m. How fast is the car going after it has traveled ½ the distance (75 meters) ? A) v < 15 m/s B) v = 15 m/s C) v > 15 m/s Physics 101: Lecture 4, Pg 9 18 Acceleration ACT An car accelerates uniformly from rest. If it travels a distance D in time t then how far will it travel in a time 2t ? A. D/4 B. D/2 C. D Demo… D. 2D Correct x=1/2 at2 E. 4D Follow up question: If the car has speed v at time t then what is the speed at time 2t ? A. v/4 B. v/2 C. v D. 2v Correct v=at E. 4v Physics 101: Lecture 4, Pg 10 24 Newton’s Second Law SF=ma Physics 101: Lecture 4, Pg 12 ACT A force F acting on a mass m1 results in an acceleration a1.The same force acting on a different mass m2 results in an acceleration a2 = 2a1. What is the mass m2? m1 F (A) 2m1 a1 m2 F (B) m1 (C) a2 = 2a1 1/2 m1 • F=ma • F= m1a1 = m2a2 = m2(2a1) • Therefore, m2 = m1/2 • Or in words…twice the acceleration means half the mass Physics 101: Lecture 4, Pg 13 29 Example: A tractor T (m=300Kg) is pulling a trailer M (m=400Kg). It starts from rest and pulls with constant force such that there is a positive acceleration of 1.5 m/s2. Calculate the horizontal force on the tractor due to the ground. X direction: Tractor SF = ma Fw – T = mtractora Fw = T+ mtractora X direction: Trailer SF = ma T = mtrailera y x FW = 1050 N N N Fw T T W W Combine: Fw = mtrailera + mtractora Fw = (mtrailer+mtractor ) a Physics 101: Lecture 4, Pg 14 35 Net Force ACT Compare Ftractor the net force on the tractor, with Ftrailer the net force on the trailer from the previous problem. SF = m a A) Ftractor > Ftrailor Ftractor = mtractor a B) Ftractor = Ftrailor 2) = (300 kg) (1.5 m/s C) Ftractor < Ftrailor = 450 N Ftrailer = mtrailer a = (400 kg) (1.5 m/s2) = 600 N Physics 101: Lecture 4, Pg 15 38 Pulley Example Two boxes are connected by a string over a frictionless pulley. Box 1 has mass 1.5 kg, box 2 has a mass of 2.5 kg. Box 2 starts from rest 0.8 meters above the table, how long does it take to hit the table. y •Compare the acceleration of boxes 1 and 2 A) |a1| > |a2| B) |a1| = |a2| x C) |a1| < |a2| 1) T - m1 g = m1 a1 2) T – m2 g = -m2 a1 1 T 2) T = m2 g -m2 a1 1) m2 g -m2 a1 - m1 g = m1 a1 a1 = (m2 – m1)g / (m1+m2) 1 T 2 2 m m24,gPg 16 1g 101: Lecture Physics 42 Pulley Example Two boxes are connected by a string over a frictionless pulley. Box 1 has mass 1.5 kg, box 2 has a mass of 2.5 kg. Box 2 starts from rest 0.8 meters above the table, how long does it take to hit the table. y •Compare the acceleration of boxes 1 and 2 A) |a1| > |a2| B) |a1| = |a2| a1 = (m2 – m1)g / (m1+m2) a = 2.45 m/s2 Dx = v0t + ½ a t2 Dx = ½ a t2 t = sqrt(2 Dx/a) t = 0.81 seconds x C) |a1| < |a2| 1 T 1 T 2 2 m m24,gPg 17 1g 101: Lecture Physics 46 Summary of Concepts • Constant Acceleration x = x0 + v0t + 1/2 at2 v = v0 + at v2 = v02 + 2a(x-x0) I feel that if there were suggested homework problems from the book, I would have a lot more practice with the concepts we’re learning. •F=ma – Draw Free Body Diagram – Write down equations – Solve •Ch 2 Problems: 1,5,7,11,13,17,29,49,69 •Ch 3 Problems: 5,13,33,47,57,65,67 Physics 101: Lecture 4, Pg 18