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Physics 2211: Lecture 14 Todays Agenda WORK

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You will learn new (sometimes much easier) ways to solve problems ... Dyne-cm (erg) = 10-7 J. BTU = 1054 J. calorie = 4.184 J. foot-lb = 1.356 J. eV = 1.6x10-19 J ... – PowerPoint PPT presentation

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Title: Physics 2211: Lecture 14 Todays Agenda WORK


1
Physics 2211 Lecture 14Todays AgendaWORK
ENERGY
  • Work Energy
  • Discussion
  • Definition
  • Dot Product
  • Work of a constant force
  • Work/kinetic energy theorem

Work Energy are covered in Chapters 6 and 7 in
Tipler. (Read both chapters together.)
2
Work Energy
  • One of the most important concepts in physics
  • Alternative approach to mechanics
  • Many applications beyond mechanics
  • Thermodynamics (movement of heat)
  • Quantum mechanics...
  • Very useful tools
  • You will learn new (sometimes much easier) ways
    to solve problems

3
Forms of Energy
  • Kinetic Energy of motion.
  • A car on the highway has kinetic energy.
  • We have to remove this energy to stop it.
  • The breaks of a car get HOT!
  • This is an example of turning one form of energy
    into another (thermal energy).
  • Thermal, Potential, Nuclear (Emc2), etc.

4
Mass Energy (but not in Physics 2211)
  • Particle Physics

E 1010 eV
(a)
(b)
E mc2
M
( poof ! )
(c)
5
Energy Conservation
  • Energy cannot be destroyed or created.
  • Just changed from one form to another.
  • We say energy is conserved!
  • True for any isolated system.
  • i.e., when we put on the brakes, the kinetic
    energy of the car is turned into heat using
    friction in the brakes. The total energy of the
    car-breaks-road-atmosphere system is the same.
  • The energy of the car alone is not conserved...
  • It is reduced by the braking.
  • Doing work on an isolated system will change
    its energy...

6
Definition of Work
Ingredients Force ( ), displacement (
) Work, W, of a constant force acting through a
displacement is
?
Fr
displacement
Dot Product
7
Definition of Work
  • Only the component of along the displacement
    is doing work.
  • Example Train on a track.

?
F cos ?
8
Aside Dot Product (or Scalar Product)
Definition Some properties (a
is a scalar) ( is a vector) The
dot product of perpendicular vectors is 0 !!
ba
?
?
ab
9
Aside Examples of dot products
y
x
z
Suppose
Then
1x4 2x(-5) 3x6 12
1x1 2x2 3x3 14 4x4
(-5)x(-5) 6x6 77
10
Aside Properties of dot products
  • Magnitude
  • Pythagorean Theorem!!

ay
ax
11
Aside Properties of dot products
  • Components
  • Derivatives
  • Apply to velocity
  • So if v is constant
  • (like for Uniform Circular Motion)

12
Back to the definition of Work
Ingredients Force ( ), displacement (
) Work, W, of a constant force acting through a
displacement is
?
Fr
displacement
13
Lecture 14, Act 1Work Energy
  • A box is pulled up a rough (mk gt 0) incline by a
    rope-pulley-weight arrangement as shown below.
  • How many forces are doing work on the box?

(a) 2 (b) 3 (c) 4
14
Work 1-D Example (constant force)
  • A force F 10 N pushes a box across a
    frictionlessfloor for a distance ?x 5 m.

Work done by on box (since
is parallel to ) WF (10 N) x (5
m) 50 Joules (J)
15
Units
  • Force x Distance Work

Newton x ML / T2
Meter Joule L ML2 / T2
16
Work Kinetic Energy
  • A force F 10 N pushes a box across a
    frictionlessfloor for a distance ?x 5 m. The
    speed of the box is v1 before the push and v2
    after the push.

v1
v2
F
m
?x
17
Work Kinetic Energy
  • Since the force F is constant, acceleration a
    will be constant. We have shown that for
    constant a
  • v22 - v12 2a(x2-x1) 2a?x.
  • multiply by 1/2m 1/2mv22 - 1/2mv12 ma?x
  • But F ma 1/2mv22 - 1/2mv12 F?x

v1
v2
F
a
m
?x
18
Work Kinetic Energy
  • So we find that
  • 1/2mv22 - 1/2mv12 F?x WF
  • Define Kinetic Energy, K K 1/2mv2
  • K2 - K1 WF
  • WF ?K (Work / Kinetic Energy Theorem)

v1
v2
F
m
a
?x
19
Work / Kinetic Energy Theorem
  • Net (or Total) Work done on object
  • change in kinetic energy of object
  • Well prove this for a variable force later.

20
Lecture 14, Act 2Work Energy
  • Two blocks have masses m1 and m2, where m1 gt m2.
    They are sliding on a frictionless floor and have
    the same kinetic energy when they encounter a
    long rough stretch (i.e., mk gt 0) which slows
    them down to a stop.Which one will go farther
    before stopping?

(a) m1 (b) m2 (c) they will go the same
distance
m1
m2
21
Recap of todays lecture
  • Work Energy
  • Discussion
  • Definition
  • Dot Product
  • Work of a constant force
  • Work/kinetic energy theorem
  • Read Tipler 6.2 and 6.3
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