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Physics 221 Chapter 7

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Body building. How much work would you have to do to stretch a stiff spring 30 cm (k= 120 N/m) ... Body building. F is a variable force so integration must be ... – PowerPoint PPT presentation

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Title: Physics 221 Chapter 7


1
Physics 221Chapter 7
2
Problem 1 . . . Work for slackers!
  • WORK Force x Distance
  • W F . D
  • Units Nm J Newton meters Joules
  • Problem 1 You push a car with a force of 200 N
    over a distance of 3 m. How much work did you
    do?

3
Solution 1 . . . Work
  • W F.d
  • W 200x3
  • W 600 J

4
Problem 2 . . . Energy
  • Energy is the capacity to do work
  • Units Joules (J)
  • Kinetic Energy Energy due to motion
  • Problem 2 What is the kinetic energy of the car
    in Problem 1?

5
Solution 2 . . . Kinetic Energy
  • Kinetic Energy Work done (if no friction)
  • K.E. 600 J
  • Problem 3 Given that m 1000 kg, what is the
    speed of the car?

6
Solution 3 . . . Speed and K.E.
  • F ma
  • 200 1000 a
  • a 0.2 m/s2
  • Vf 2 Vi 2 2ad
  • Vf 2 0 2(0.2)(3)
  • Vf 2 1.2
  • Vf 1.1 m/s

7
Kinetic Energy Formula
  • K.E. 1/2 m v2
  • Problem 4 The K.E. of a car is 600 J and its
    mass is 1000 kg. What is its speed?

8
Solution 4 . . . more K.E.
  • K.E. 1/2 m v2
  • 600 1/2(1000)(v2)
  • v 1.1 m/s
  • Does this look familiar?
  • Moral of the story We can find the speed either
    by using Newtons Laws or Energy Principles.

9
Problem 5 . . . Lugging the Luggage
  • What is the speed when the distance is 3 m?

10
Solution 5 . . . Lugging the Luggage
  • What is the speed when the distance is 3 m?
  • F.d 1/2 m v2
  • (40 cos 600)(3) (1/2)(10)(v2)
  • v 3.5 m/s
  • Moral of the story
  • W (F)(d)(cos?)

11
Scalar Product (Dot Product)
  • A . B A B cos ?
  • i . i 1
  • i . j 0
  • W F . d

12
Problem 6 . . . work is a scalar !
  • F 3 i 2 j acts on an object and causes a
    displacement of 7 i
  • (a) How much work was done?
  • (b) What is the angle between F and d?

13
Solution 6 . . . work is a scalar !
  • (a) W F.d
  • W (3 i 2 j) . 7 i
  • W 21 0
  • W 21
  • (b) F 5 and d 7 and F.d 21
  • F.d F d cos ?
  • 21 (5)(7) cos ?
  • cos ? 3/5
  • ? 53 0

14
Stretching Springs
Hookes Law The amount of stretch is directly
proportional to the force applied. F k x
15
Example 6.6 . . . Springy Spring
The spring constant (k) of a spring is 20 N/m.
If you hang a 50 g mass, how much will it stretch?
16
Solution 6.6 . . . Springy Spring
F k x mg kx (50 /1000)(9.8) (20)(x) x 2.5
cm
17
Problem 8 . . . Body building
  • How much work would you have to do to stretch a
    stiff spring 30 cm (k 120 N/m)?

18
Solution 8 . . . Body building
  • W F . d
  • W (kx)(x)
  • W kx2
  • W (120)(0.3)2
  • W 10.8 J
  • ?

19
Correct Solution 8 . . . Body building
  • F is a variable force so integration must be
    performed.
  • W ?F . dx
  • W ? kx . dx
  • W 1/2 kx2
  • W (1/2)(120)(0.3)2
  • W 5 .4 J
  • ?

20
Problem 1 . . . Potential Energy
  • You lift a 2 kg book and put it on a shelf 3
    meters high.
  • A. How much work did you do?
  • B. Was the work lost?

21
Solution 1 . . . Hidden Energy (P.E.)
  • A.
  • W F.d
  • W mgh
  • W 2x10x3
  • W 60 J
  • B.
  • Work is stored as Potential Energy (hidden).

22
Problem 2 . . . In other words
  • In other words, if the 2 kg book fell down from
    the top of the bookshelf (3m), what would its
    K.E. be?

23
Solution 2 . . . In other words
  • The K.E. would be equal to the P.E.
  • K.E. 600 J.
  • In other words, energy was converted
    (transformed) from one form (P.E.) to another
    (K.E.)

24
Conservative Forces
  • If the work done against a force does not depend
    on the path taken then that force is called a
    conservative force. Examples are gravity and
    spring force. The total mechanical energy (P.E.
    K.E.) will remain constant in this case.
  • If the work done against a force depends on the
    path taken then that force is called a
    non-conservative force. Example is friction.
    The total mechanical energy (P.E. K.E.) will
    not remain constant in this case.
  • Vote Democrat . . . Just kidding!
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