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Learn and apply Newton's First, Second, and Third Laws of Motion in unidirectional and multidirectional scenarios. Understand the relationship between position, velocity, and acceleration.
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Analysis of Motion & Newton’s Laws
Class Objective • Learn and apply Newton’s First, Second, and Third Laws • Unidirectional • Multidirectional • Learn the relationship between position, velocity, and acceleration
-3 -2 -1 0 1 2 3 4 -3 -2 -1 0 1 2 3 4 Some Definitions (1D) Position - location on a straight line x Displacement - change in location on a straight line Dx = x2 - x1 = 4 - (-2) = 6 x
Some Definitions (1D) Average Velocity - rate of position change with time Instantaneous Velocity
Average and Instantaneous Velocity (1D) Position x2 x2 - x1 t2 - t1 Slope = = Average Velocity x1 t1t2 Time
Some Definitions (2D) Position -- a location usually described by a graphic on a map or by a coordinate system 4 3 2 (4, 3) 1 0 0 -3 -2 -1 -1 1 2 3 4 5 -2 -3 (-2, -3) -4
Some Definitions (2D) Displacement -- change in position, where 4 (4, 3) 3 2 1 0 0 -3 -2 -1 1 2 3 4 5 -1 -2 -3 (-2, -3) -4
Some Definitions (2D) Average velocity Instantaneous velocity Speed - the magnitude of instantaneous velocity (scalar)
Some Definitions (1D) Average Acceleration - rate of velocity change with time Instantaneous Acceleration
Average and Instantaneous Acceleration (1D) Velocity v2 v2 - v1 t2 - t1 Slope = = Average Acceleration v1 t1t2 Time
Some Definitions (2D) Average Acceleration Instantaneous Acceleration
Example One-dimensional motion Speed, miles per hour 20 10 0 0 1 2 3 Time, hours
20 10 0 0 1 2 3 Paired Exercise What is the distance traveled? What is the acceleration at 1.25 hours? Speed, miles per hour Time, hours
For constant acceleration... if acceleration is constant integrating both sides v0 is the original value at the beginning of the time interval (Definition)
Constant Acceleration (Definition) substituting the velocity equation from the previous page integrating both sides yields
Equations of Motion (Constant Acceleration) Velocity Position (in terms of x)
Multiple Directions Equations of motion can be written for each direction independently. Velocity Position
Distance, Velocity, and Acceleration • Suppose a dragster has constant acceleration. • If a dragster starts from rest and accelerates to 60 mph in 10 seconds. How far did it travel?
Plot Speed vs time What does the area under the line represent? 60 mph (1 mi/min) speed time 10 seconds (1/6 min)
Distances…. Area = distance? Sure: Right? So:
Your Turn: RAT 10.2
p = m v Momentum v m momentum
Newton’s 1st Law: “Every body persists in its state of rest or of uniform motion in a straight line unless it is compelled to change that state by forces impressed upon it.” “In the absence of a net force applied to an object, momentum stays constant.” Newton Holtzapple
Newton’s Second Law The time-rate-of-change of momentum is proportional to the net force on the object. If mass is constant...
Newton’s Third Law “To every action there is always opposed an equal reaction: or, the mutual actions of two bodies upon each other are always equal and directed in contrary parts.” Newton
Newton’s Third Law Other statements • Forces always exist by the interaction of two (or more) bodies • The force on one body is equal and opposite to the force on another body • It is impossible to have a single isolated force acting in one direction • The designation of an “action force” and a “reaction force” is arbitrary because there is mutual interaction between the bodies
Newton’s Third Law A Consequence The earth and the moon orbit about a common point about 1000 miles below the surface of the earth because the earth pulls on the moon and the moon pulls on the earth.
Example: Newton’s 3rd Law • Consider a rocket with constant exhaust gas velocity: • The mass changes (obviously) as the fuel is burned and the gas is ejected. Positive fuel ve v m
Example: Newton’s 3rd Law • The magnitude of the net force acting on the rocket can be determined by observing its acceleration where m is the instantaneous mass of the rocket and dv is the instantaneous change in rocket velocity.
Example: Newton’s 3rd Law • The magnitude of the net force acting on the ejected gas is where ve is the velocity of ejected gas and dm/dt is the rate mass is ejected from the rocket. (Note: The origin of this equation will become more clear when we do Accounting for Momentum.)
Example: Newton’s 3rd Law From Newton’s 3rd Law, these two forces must be opposite and equal to each other, so: or,
Example: 3rd Law Using calculus, this can be solved to yield: where m0 is the initial mass of rocket including fuel
Why Newton’s Laws? • Engineers use models to predict things such as motion, fluid flow, lift on an airplane wing, movement of neutrons in a nuclear reactor, deflection of beams or columns, etc. • Newton’s laws are widely used and a good first example of engineering models.
More on Models Question: If I toss a piece of chalk at a sleeping student, does its path follow a parabola? Answer: Not exactly, because air resistance affects the motion. Also, we should consider the effect of the spinning earth as it moves around the sun in an ellipse. However, for most practical work, a parabola is close enough.