Title: Physics 2211: Lecture 14 Todays Agenda WORK
1Physics 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.)
2Work 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
3Forms 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.
4Mass Energy (but not in Physics 2211)
E 1010 eV
(a)
(b)
E mc2
M
( poof ! )
(c)
5Energy 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...
6Definition of Work
Ingredients Force ( ), displacement (
) Work, W, of a constant force acting through a
displacement is
?
Fr
displacement
Dot Product
7Definition of Work
- Only the component of along the displacement
is doing work. - Example Train on a track.
?
F cos ?
8Aside 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
9Aside Examples of dot products
y
x
z
Suppose
Then
1x4 2x(-5) 3x6 12
1x1 2x2 3x3 14 4x4
(-5)x(-5) 6x6 77
10Aside Properties of dot products
- Magnitude
-
-
-
- Pythagorean Theorem!!
ay
ax
11Aside Properties of dot products
- Components
- Derivatives
- Apply to velocity
- So if v is constant
- (like for Uniform Circular Motion)
12Back to the definition of Work
Ingredients Force ( ), displacement (
) Work, W, of a constant force acting through a
displacement is
?
Fr
displacement
13Lecture 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
14Work 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)
15Units
Newton x ML / T2
Meter Joule L ML2 / T2
16Work 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
17Work 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
18Work 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
19Work / Kinetic Energy Theorem
- Net (or Total) Work done on object
-
- change in kinetic energy of object
- Well prove this for a variable force later.
20Lecture 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
21Recap 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