V = 20 m/s magnitude of the velocity vector.

Slides:



Advertisements
Similar presentations
Circular Motion & Highway Curves
Advertisements

Physics 111: Mechanics Lecture 5
Circular Motion and Gravitation
Chapter 6: Circular Motion & Other Applications of Newton’s Laws
Uniform Circular Motion. Answer Me!!!!  Newton’s Laws state that an object in motion will stay at the same velocity until acted upon by an unbalanced.
Chapter 4- Forces and Motion
Circular Motion.
Copyright © 2008 Pearson Education, Inc., publishing as Pearson Addison-Wesley. Chapter 5: Uniform Circular Motion Chapter Goal: To learn how to solve.
Physics 2.2.
Chapter Opener. Caption: Newton’s laws are fundamental in physics
Example 1: A 3-kg rock swings in a circle of radius 5 m
Acceleration is equal to Δv/Δt. Velocity is a vector and there are two ways a vector can be changed: by changing magnitude or by changing direction.
Forces of Friction When an object is in motion on a surface or through a viscous medium, there will be a resistance to the motion This is due to the interactions.
Centripetal Force and Acceleration Unit 6, Presentation 1.
Dynamics of Uniform Circular Motion
Lecture 10 Employ Newton’s Laws in 2D problems with circular motion 1.
Chapter 5 Dynamics of Uniform Circular Motion. 5.1 Uniform Circular Motion DEFINITION OF UNIFORM CIRCULAR MOTION Uniform circular motion is the motion.
6-4 Connected Object The several objects tied together motion Separate these objects draw free body diagram: (1)Isolate the object (2)Draw the all external.
Circular Motion Part 2 By: Heather Britton. Circular Motion Part 2 According to Newton’s 2nd Law, an accelerating body must have a force acting on it.
Friction Ffriction = μFNormal.
Friction. Newton’s Second Law W = mg W = mg Gives us F = ma Gives us F = ma.
C H A P T E R 5 Dynamics of Uniform Circular Motion.
Uniform Circular Motion. What is uniform circular motion? Constant speed Circular path Must be an unbalanced force acting towards axis of rotation- think.
Uniform Circular Motion Physics 12. Uniform Circular Motion object is moving at a constant speed but changing directions acceleration occurs due to direction.
Uniform Circular Motion is the motion of an object traveling at a constant (uniform) speed on a circular path.
Cars travelling on a banked curve. For a level (flat) curved road all of the centripetal force, acting on vehicles, must be provided by friction.
Chapter 4 Laws of Motion and Forces Goals: Newtons Laws, Inertia and mass, Mass vs Weight, Free Body diagrams, Fg, Fn, Fy, Fx, Ff, coefficients of friction.
1. A car of mass 1000 kg is driving into a corner of radius 50m at a speed of 20 ms -1. The coefficient of friction between the road and the car’s tyres.
Ying Yi PhD Chapter 5 Dynamics of Uniform Circular Motion 1 PHYS HCC.
Chapter 6 Force and Motion II. Forces of Friction When an object is in motion on a surface or through a viscous medium, there will be a resistance to.
Frictional Force A force that opposes motion Acts parallel to the
Chapter 5: Dynamics of Uniform Circular Motion
C H A P T E R 6 Dynamics of Uniform Circular Motion
EQUATIONS OF MOTION: NORMAL AND TANGENTIAL COORDINATES (Section 13.5)
on an inclined surface. The surface makes 30⁰ angle with horizon.
Acceleration of a Single Body Sliding Down an Incline
Physics 2 – April 20, 2017 P3 Challenge – A kg block with an initial speed of 3.5 m/s is sliding on a level surface with a kinetic coefficient of.
Chapter 5 Applications of Newton’s Law
PHYS 1441 – Section 002 Lecture #11
Inclined Plane Problems
Uniform Circular Motion
Vertical Circular Motion
Physics 111: Mechanics Lecture 9
Circular Motion and Other Applications of Newton’s Laws
Ch. 6: Circular Motion & Other Applications of Newton’s Laws
Normal Force and Friction Force
Circular Motion © David Hoult 2009.
PHYS 1441 – Section 002 Lecture #11
Section 5.8: Friction.
AP Physics Section 4-8 Friction.
Roller Coaster Design Project
Recall: Uniform Circular Motion
Objectives Chapter 4 Section 4 Everyday Forces
Uniform Circular Motion
Chapter 4 Laws of Motion.
More Centripetal Force Problems
What causes UCM?.
Centripetal forces keep these children moving in a circular path.
Lecture 10 Employ Newton’s Laws in 2D problems with circular motion
Aim: How do we explain centripetal motion?
Motion on Inclined Planes
Horizontal Surface (no friction)
Circular Motion & Highway Curves
Pendulum A string is attached to mass m and swung in a horizontal circle of radius r. There is tension T in the string. The angle θ is measured from the.
Section 5.8: Friction.
Forces applied at an Angle & Inclined Planes
Coverage of the 1st Long test
Centripetal Force and Banked Curves Chapter 5 Lesson 2
Circular Motion.
EQUATIONS OF MOTION: NORMAL AND TANGENTIAL COORDINATES
Presentation transcript:

V = 20 m/s magnitude of the velocity vector. A car drives with speed of 20m/s on a banked track on a circular path, the surface of the road makes 15⁰ angle with horizon. Find the radius of the curve. Ignore the friction between the tires and the road. Break it down: V = 20 m/s magnitude of the velocity vector.   A car drives with speed of 20m/s The surface of the road is not horizontal. It makes an angle of θ with the horizon.   on a banked track on a circular path, the surface of the road makes 15⁰ angle with horizon. θ = 15⁰   r =?   Find the radius of the curve. Fs = 0 Fs = μS*FN  μS = 0 Although the car is moving, it should not be confused with kinetic friction. Kinetic friction opposes the movement of the car, but static friction keeps the car on the circular path. Static friction is toward the center of the circle.   Ignore the friction between the tires and the road. Physicsfix.com

Draw Free Body Diagram (FBD) for the car A car drives with speed of 20m/s on a banked track on a circular path, the surface of the road makes 15⁰ angle with horizon. Find the radius of the curve. Ignore the friction between the tires and the road. Solution: Draw a diagram Draw Free Body Diagram (FBD) for the car + Y FN FN Cos15⁰ 15⁰ r =? FN Sin15⁰ + X 15⁰ 15⁰ mg Notice that: FN is perpendicular to the curve surface “+X” axis is toward the center of the circular path (parallel to r). Weight (mg) is along “- Y” axis Physicsfix.com

Calculate Fnet along x and y axis A car drives with speed of 20m/s on a banked track on a circular path, the surface of the road makes 15⁰ angle with horizon. Find the radius of the curve. Ignore the friction between the tires and the road. Solution: Calculate Fnet along x and y axis FnetX = FnetY = This component of FN along x axis makes the centripetal acceleration. ∑Fx = FN sin 15⁰ ∑Fy = FN cos 15⁰ – mg This component of FN along + y axis supports the weight of the car. Note that the direction of +x axis is toward center of the horizontal path, and acceleration is along +x axis as well. Apply newton’s second law Again net force is equal to the centripetal force which is mv 2 / r. ∑FX = mv 2/r  F N sin 15⁰ = m v 2 /r (1) The car does not move along y axis, then ∑Fy = 0 ∑FY = 0  FN cos 15 – mg =  F N cos 15 = mg (2) Physicsfix.com

With the given speed and road slope, the radius of the circular path A car drives with speed of 20m/s on a banked track on a circular path, the surface of the road makes 15⁰ angle with horizon. Find the radius of the curve. Ignore the friction between the tires and the road. Solution: Divide equation (1) by equation (2) FN Sin15⁰/ FN Cos 15⁰ = [mV2/r]/mg  tg (15⁰) = V2/ (r * g) F N sin 15⁰ = m v 2 /r (1) F N cos 15 = mg (2) Solve this equation to find the radius (r) r = V 2 / [g * tg 15⁰] Now substitute V, tg 15⁰, and g to find the radius (r) V = 20 m/s θ = 15⁰  tg 15⁰ = 0.27 g = 9.8 m/s2 With the given speed and road slope, the radius of the circular path should be 151m that car can drive in order not rely on friction at all.  r = (20) 2 / [9.8 * (0.27)]  r = 151 m Physicsfix.com