CHAPTER 2 2.4 Continuity Applications to Physics and Engineering Work: W = lim n->   i=1 n f (x i * )  x =  a b f (x) dx Moments and centers of mass:

Slides:



Advertisements
Similar presentations
Work Colin Murphy, Kevin Su, and Vaishnavi Rao. Work (J if force is in N, ft-lb if force is in lb) Work = Force * distance Force (N)= mass * acceleration.
Advertisements

Chapter 7: Work (Ewen et al. 2005) Objectives: Define power and solve power problems Define power and solve power problems.
Applications of Integration
Integrating Force to find Work. Work, measured in either joules(Newton-meters) or foot- pounds, is the product of the force necessary to move and object.
PHYSICS 50: Lecture 11.1 RICHARD CRAIG.
Rotational Dynamics Chapter 9.
7.5 Applications to Physics and Engineering. Review: Hooke’s Law: A spring has a natural length of 1 m. A force of 24 N stretches the spring to 1.8 m.
APPLICATIONS OF INTEGRATION Work APPLICATIONS OF INTEGRATION In this section, we will learn about: Applying integration to calculate the amount.
FURTHER APPLICATIONS OF INTEGRATION
Applications of Integration
Chapter 8 – Further Applications of Integration
Section 6.4 Another Application of Integration. Definition: Work Work generally refers to the amount of effort required to perform a task.
Lecture 6 – Physics Applications Mass 1 1D object: 3D object: If density varies along the length of the 1-D object (wires, rods), then use integrals to.
6.4 Arc Length. Length of a Curve in the Plane If y=f(x) s a continuous first derivative on [a,b], the length of the curve from a to b is.
Applications of the Definite Integral
Work = Force * Distance Work = 5 * 6 = 30 Foot Pounds.
APPLICATIONS OF INTEGRATION 6. A= Area between f and g Summary In general If.
Copyright © Cengage Learning. All rights reserved. 5 Applications of Integration.
Greg Kelly, Hanford High School, Richland, WashingtonPhoto by Vickie Kelly, 2004 Section 6.7 Work and Pumping Liquids Hoover Dam Nevada & Arizona.
Section 8.5 Applications to Physics
A Balancing Act. When is an object in Equilibrium? When its state of motion is not changing What are the conditions for Equilibrium? 1) the net force.
Chapter 2.2 Notes Work in Fluids. When work is done, we measure the force that moves a certain distance. In a fluid system, it is easier to measure the.
Centroids and Centers of Gravity
Applications of Integration In this chapter we explore some of the applications of the definite integral by using it for 1.Computing the area between curves.
The Area Between Two Curves Lesson 6.1. When f(x) < 0 Consider taking the definite integral for the function shown below. The integral gives a ___________.
Law of Universal Gravitation. Universal Gravitation gravity is a force of attraction between any two masses gravity is a UNIVERSAL force –universal meaning.
Final JEOPARDY ROUND 1: JEOPARDY Subby Hubby Part-y Highly Improper DanceDance Revolution Potpourri
September 27, 2007 Welcome to the cavernous pit of math!
Work.
Chapter 6: Concurrent and Parallel Forces (Ewen et al. 2005) Objectives: Use the center of gravity to solve parallel force problems. Use the center of.
Section 6.6 Work. All graphics are attributed to:  Calculus,10/E by Howard Anton, Irl Bivens, and Stephen Davis Copyright © 2009 by John Wiley & Sons,
Copyright © Cengage Learning. All rights reserved. 8 Further Applications of Integration.
7.5 - Work. When the force acting on an object is constant, work can be described without calculus But constant force is very limiting. Take a simple.
Section 6.4 Work. In physics the word “work” is used to describe the work a force has done on an object to move it some distance. Work done = Force ·
Work Lesson 7.5. Work Definition The product of  The force exerted on an object  The distance the object is moved by the force When a force of 50 lbs.
7.5 part 1 Work and Pumping Liquids Greg Kelly, Hanford High School, Richland, Washington.
Calculating Work. Work = force x distance W=f x d Unit of Measurement for Work is Joules Unit of Measurement for Force is Newtons Unit of Measurement.
Chapter 10 Lecture 18: Rotation of a Rigid Object about a Fixed Axis: II.
20) 108° 21) 80° 22) 70° 23) 123° 24) 38° 25) 167° 26) 10° 27) 154° 28) 105 = 2x – 11; x = 58 29) 6x x = 180; x = 23.
7.5 Work and Pumping Liquids and Fluid Pressure. Review: Hooke’s Law: A spring has a natural length of 1 m. A force of 24 N stretches the spring to 1.8.
Chapter 6 – Applications of Integration
Copyright © Cengage Learning. All rights reserved.
Lecture 1 – Volumes Area – the entire 2-D region was sliced into strips Before width(x) was introduced, only dealing with length f(x) a b Volume – same.
Work and Fluid Pressure
Work (variable distance)
Objective: Computing work.
7 Applications of Integration
Find the work done in pushing a car a distance of 14 m while exerting a constant force of 800 N. Select the correct answer. W = 10,700 J W = 11,200 J.
**Uniform Circular Motion
True or False: If a force of 6 lbs is required to hold a spring stretched 5 inches beyond its natural length, then 60 lb-in. of work is done in stretching.
If {image} find the Riemann sum with n = 5 correct to 3 decimal places, taking the sample points to be midpoints
8.3 – Applications to Physics and Engineering
Section Work Work is a measure of the cumulative effect of a force in moving an object from one position to another. Pushing a box full of books.
Non-constant Forces Up until this time, we have mainly dealt with forces that are constant. These produce a uniform, constant acceleration. Kinematic.
Work Lesson 7.5.
Use the Midpoint Rule with n = 10 to approximate the integral
Quick Review & Centers of Mass
Work and Pumping Liquids
All the clockwise ……………. on the right hand side are
Applications of Integration
Numerical methods for engineers includes units
Numerical methods for engineers includes units
Math – Work.
Copyright © Cengage Learning. All rights reserved.
Work and Fluid Pressure
7.1 Work Force (N) W = F x d Work (joules) Distance (m)
Symbolic Integral Notation
Work.
Presentation transcript:

CHAPTER Continuity Applications to Physics and Engineering Work: W = lim n->   i=1 n f (x i * )  x =  a b f (x) dx Moments and centers of mass: 1. M y = lim n->   i=1 n  x i f (x i )  x =   a b x f (x) dx 2. M x = lim n->   i=1 n  (1/2) [ f (x i )] 2  x =   a b (1/2) ) [ f (x)] 2 dx x = (1/A)  a b x f (x) dx y = (1/A)  a b (1/2)[ f (x)] 2 dx

Example: When a particle is located at a distance x meters from the origin, a force of cos (  x /3) newtons act on it. How much work is done in moving the particle from x = 1 to x = 2? Interpret your answer by considering the work done from x = 1 to x = 1.5 and from x = 1.5 to x = 2. Example: Show how to approximate the required work by Riemann sum. Then express the work as an integral and evaluate it. A uniform cable hanging over the edge of a tall building is 40ft. long and weighs 60 lb. How much work is required to pull 10ft. of the cable to the top?

Example: A circular swimming pool has a diameter of 24ft, the sides are 5ft high, and the dept of the water is 4ft. How much work is required to pump all of the water out over the size? (use the fact that water weighs 62.5 lb/ft 3.) Example: x = The masses m i are located at the points P i. Find the moments M x and M y and the center of mass of the system. m 1 = 3, m 2 = 3, m 3 = 8, m 4 = 6; P 1 =(0,0), P 2 =(1,8), P 3 =(3,-4), P 4 =(-6,-5).