Define kinetic energy and potential energy, along with the appropriate units in each system.
Describe the relationship between work and kinetic energy, and apply the WORK-ENERGY THEOREM.
Define and apply the concept of POWER, along with the appropriate units.
EnergyEnergyEnergyEnergy is anything that can be is anything that can be converted into work; i.e., anything converted into work; i.e., anything that can exert a force through a that can exert a force through a distancedistance.
Energy is the capability for doing Energy is the capability for doing work.work.
Potential Energy:Potential Energy: Ability to do work Ability to do work by virtue of position or conditionby virtue of position or condition.
A stretched bowA stretched bowA suspended weightA suspended weight
Gravitational Potential Gravitational Potential EnergyEnergy
What is the P.E. of a 50-kg person at a height of 480 m?
U = mgh = (50 kg)(9.8 m/s2)(480 m)
U = 235 kJU = 235 kJ
Kinetic Energy:Kinetic Energy: Ability to do work Ability to do work by virtue of motion. (Mass with by virtue of motion. (Mass with velocity)velocity)A speeding car A speeding car
or a space or a space rocketrocket
2 21 12 2 (1000 kg)(14.1 m/s)K mv
What is the kinetic energy of a 5-g What is the kinetic energy of a 5-g bullet traveling at 200 m/s?bullet traveling at 200 m/s?
What is the kinetic energy of a What is the kinetic energy of a 1000-kg car traveling at 14.1 m/s? 1000-kg car traveling at 14.1 m/s?
5 g5 g
200 200 m/sm/s
K = 100 JK = 100 J
K = 99.4 JK = 99.4 J
2 21 12 2 (0.005 kg)(200 m/s)K mv
A resultant force changes the velocity A resultant force changes the velocity of an object and does work on that of an object and does work on that
object.object.
m
vo
m
vfx
F F
( ) ;Work Fx ma x 2 2
0
2fv v
ax
2 21 102 2fWork mv mv
Work is Work is equal to the equal to the change inchange in ½mv½mv22
If we define If we define kinetic energykinetic energy as as ½mv½mv22 then we can state a very important then we can state a very important
physical principle:physical principle:
The Work-Energy Theorem:The Work-Energy Theorem: The work The work done by a resultant force is equal to done by a resultant force is equal to the change in kinetic energy that it the change in kinetic energy that it produces.produces.
2 21 102 2fWork mv mv
x
F = ?F = ?
80 80 m/sm/s
6 cm6 cmWork = ½Work = ½ mvmvff
2 2 - ½- ½ mvmvoo
22
0
F x = - F x = - ½½ mvmvoo22
FF (0.06 m) cos 180 (0.06 m) cos 18000 = - = - ½½ (0.02 kg)(80 (0.02 kg)(80 m/s)m/s)22
FF (0.06 m)(-1) = -64 J (0.06 m)(-1) = -64 J F = 1067 NF = 1067 N
Work to stop bullet = change in K.E. for Work to stop bullet = change in K.E. for bulletbullet
2525 mm fff = f = k.k.n = n = k k mgmg
Work =Work = F(F(cos cos ) ) xx
Work = - Work = - k k mg mg xx
0K =K = ½½ mvmvff
2 2 - ½- ½ mvmvoo22
-½-½ mvmvoo22 = - = -k k mgmg xx vvoo = = 22kkgxgx
vo = 2(0.7)(9.8 m/s2)(25 m) vo = 18.5 m/s
vo = 18.5 m/s
Work = K
K = Work
hh3030
00
nnff
mgmg
xx
Plan: Plan: We must calculate We must calculate both the resultant work both the resultant work and the net displacement and the net displacement xx. Then the velocity can . Then the velocity can be found from the fact be found from the fact that that Work = Work = K.K.
Resultant work = (Resultant force down Resultant work = (Resultant force down the plane) the plane) xx (the (the displacement down the displacement down the plane)plane)
h
300
nf
mg
x
From trig, we know that the Sin From trig, we know that the Sin 303000 = = h/x h/x and:and:
0
20 m40 m
sin 30x 0sin 30
h
x
hx
303000
WWyy = = (4 kg)(9.8 m/s(4 kg)(9.8 m/s22)(cos 30)(cos 3000) = 33.9 N
hh
303000
nnff
mgmg
x = x = 4040
mm
Draw free-body diagram to find the resultant Draw free-body diagram to find the resultant force:force:
nnff
mgmg303000
x
y
mgmg cos 30 cos 3000 mgmg sin 30 sin 3000
WWxx = = (4 kg)(9.8 m/s(4 kg)(9.8 m/s22)(sin 30)(sin 3000) = 19.6 N
nnff
mgmg303000
x
y
33.9 N33.9 N19.6 N19.6 N
Resultant force down Resultant force down plane: plane: 19.6 N - 19.6 N - ffRecall that Recall that ffkk = = k k
nnFFyy = 0 or = 0 or nn = 33.9 = 33.9 NN
Resultant Force = 19.6 N – kn ; and k = 0.2Resultant Force = 19.6 N – (0.2)(33.9 N) = 12.8 N
Resultant Force Down Plane = 12.8 N
(Work)(Work)RR = = FFRRxx
FFRR
303000
xxNet Work = (12.8 N)(40 m)Net Work = 512 J
Finally, we are able to apply the work-energy theorem to find the final velocity:
2 21 102 2fWork mv mv
0
hh3030
00
nnff
mgmg
xx Resultant Work = Resultant Work = 512 J512 JWork done on block Work done on block
equals the change in K. equals the change in K. E. of block.E. of block.
½½ mvmvff2 2 - ½- ½ mvmvoo
22 = = WorkWork
0 ½½ mvmvff
22 = = 512 J512 J
½½(4 kg)(4 kg)vvff22 = 512 = 512
JJ vf = 16 m/svf = 16 m/s
Power is defined as the rate at which work is done: (P = dW/dt )
10 kg
20 mh
m
mg
t
4 s
F
Power of 1 W is work done at rate of 1 J/s
Power of 1 W is work done at rate of 1 J/s
Work F rPower
time t
Work F rPower
time t
2(10kg)(9.8m/s )(20m)
4 s
mgrP
t
490J/s or 490 watts (W)P 490J/s or 490 watts (W)P
1 W = 1 J/s and 1 kW = 1000 W
One watt (W) is work done at the rate of one joule per second.
One ft lb/s is an older (USCS) unit of power.One horsepower is work done at the rate of 550 ft lb/s. ( 1 hp = 550 ft lb/s )
Power Consumed: P = 2220 W
Power Consumed: P = 2220 W
What power is consumed in lifting a 70-kg robber 1.6 m in
0.50 s?Fh mghP
t t
2(70 kg)(9.8 m/s )(1.6 m)
0.50 sP
Recognize that work is equal Recognize that work is equal to the change in kinetic to the change in kinetic energy:energy: Work
Pt
2 21 102 2fWork mv mv
2 21 12 2 (100 kg)(30 m/s)
4 sfmv
Pt
m = 100 kg
Power Consumed: P = 1.22 kW
Power Consumed: P = 1.22 kW
Recall that average or constant velocity is distance covered per unit
of time v = x/t.
P = = Fx
t
F x
tIf power varies with time, then calculus is needed to integrate over time. (Optional)
Since P = dW/dt: ( )Work P t dt ( )Work P t dt
P FvP Fv
Work = 132,000 ft lb
Work = 132,000 ft lb
550ft lb/s4hp 2200ft lb/s
1hp
(2200ft lb/s)(60s)Work
; Work
P Work Ptt
The Work-Energy Theorem:The Work-Energy Theorem: The work The work done by a resultant force is equal to the done by a resultant force is equal to the change in kinetic energy that it produces.change in kinetic energy that it produces.
The Work-Energy Theorem:The Work-Energy Theorem: The work The work done by a resultant force is equal to the done by a resultant force is equal to the change in kinetic energy that it produces.change in kinetic energy that it produces.
Potential Energy:Potential Energy: Ability to do Ability to do work by virtue of position or work by virtue of position or conditioncondition.
U mgh
Kinetic Energy:Kinetic Energy: Ability to do work Ability to do work by virtue of motion. (Mass with by virtue of motion. (Mass with velocity)velocity)
212K mv
Work = ½ mvf2 - ½
mvo2
Work = ½ mvf2 - ½
mvo2
Power is defined as the rate at which work is done: (P = dW/dt )
WorkP
t
Work F rPower
time t
Work F rPower
time t
Power of 1 W is work done at rate of 1 J/s
Power of 1 W is work done at rate of 1 J/s
P= F v