chapter 7: conservation of energy - national maglabshill/teaching/2048 spring11/lecture12.pdf ·...

11
Chapter 7: Conservation of Energy Chapter 9: Center of Mass and Momentum Tuesday February 17 th Reading: up to page 113 in Ch. 7, then start of Ch. 9 Review: Potential Energy Review: Conservation of Energy Calculus method for determining work Example problems, iclicker and demos Chapter 9: center of mass (if time) Chapter 9: momentum and impulse (if time) Mini Exam III on Thursday Will cover LONCAPA #7-10 (Newton’s laws and energy cons.)

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Page 1: Chapter 7: Conservation of Energy - National MagLabshill/Teaching/2048 Spring11/Lecture12.pdf · Chapter 7: Conservation of Energy Chapter 9: Center of Mass and Momentum Tuesday February

Chapter 7: Conservation of Energy Chapter 9: Center of Mass and Momentum

Tuesday February 17th

Reading: up to page 113 in Ch. 7, then start of Ch. 9

• Review: Potential Energy • Review: Conservation of Energy • Calculus method for determining work • Example problems, iclicker and demos • Chapter 9: center of mass (if time) • Chapter 9: momentum and impulse (if time)

Mini Exam III on Thursday • Will cover LONCAPA #7-10 (Newton’s laws and energy cons.)

Page 2: Chapter 7: Conservation of Energy - National MagLabshill/Teaching/2048 Spring11/Lecture12.pdf · Chapter 7: Conservation of Energy Chapter 9: Center of Mass and Momentum Tuesday February

ΔU =U f −Ui

= −Wcons.

= −FgΔxΔUg = Mgh

= +Wn.c.

F

Mg

h

Work & Potential Energy One can define a ‘Potential Energy’, U, for ALL conservative forces as follows:

Page 3: Chapter 7: Conservation of Energy - National MagLabshill/Teaching/2048 Spring11/Lecture12.pdf · Chapter 7: Conservation of Energy Chapter 9: Center of Mass and Momentum Tuesday February

ΔU =U f −Ui

= −Wcons.

= −FgΔxΔUg = Mgh

= +Wn.c.

F

Mg

h

Work & Potential Energy One can define a ‘Potential Energy’, U, for ALL conservative forces as follows:

The Potential Energy change, ΔU, does not care how the height change was achieved.

Page 4: Chapter 7: Conservation of Energy - National MagLabshill/Teaching/2048 Spring11/Lecture12.pdf · Chapter 7: Conservation of Energy Chapter 9: Center of Mass and Momentum Tuesday February

Conservation of Energy

ΔK = K f − Ki =Wnet

=Wcons. +Wn.c.

Work-Kinetic Energy theorem

• We can now replace any work due to conservative forces by potential energy terms, i.e.,

ΔK = −ΔU +Wn.c.

ΔEmech = ΔK + ΔU =Wn.c.

Or

• Here, Emech is the total mechanical energy of a system, equal to the sum of the kinetic and potential energy of the system.

• If work is performed on the system by an external, non-conservative force, then Emech increases.

Page 5: Chapter 7: Conservation of Energy - National MagLabshill/Teaching/2048 Spring11/Lecture12.pdf · Chapter 7: Conservation of Energy Chapter 9: Center of Mass and Momentum Tuesday February

Conservation of Energy Alternatively:

ΔEmech = ΔK + ΔU =Wn.c.

⇒ K f − Ki( ) + U f −Ui( ) =Wn.c.

Or K f +U f = Ki +Ui( ) +Wn.c.

i.e. Emech, f = Emech,i +Wn.c.

Page 6: Chapter 7: Conservation of Energy - National MagLabshill/Teaching/2048 Spring11/Lecture12.pdf · Chapter 7: Conservation of Energy Chapter 9: Center of Mass and Momentum Tuesday February

Power • Power is defined as the "rate at which work is done." • If an amount of work W is done in a time interval Δt by a force, the average power due to the force during the time interval is defined as

Pavg =

WΔt

• Instantaneous power is defined as P = dW

dt• The SI unit for power is the Watt (W).

1 watt = 1 W = 1 J/s = 0.738 ft · lb/s 1 horsepower = 1 hp = 550 ft · lb/s = 746 W

1 kilowatt-hour = 1 kW · h = (103 W)(3600 s) = 3.60 MJ

Page 7: Chapter 7: Conservation of Energy - National MagLabshill/Teaching/2048 Spring11/Lecture12.pdf · Chapter 7: Conservation of Energy Chapter 9: Center of Mass and Momentum Tuesday February

More on Power • Power is defined as the "rate at which work is done." • If an amount of work W is done in a time interval Δt by a force, the average power due to the force during the time interval is defined as

P = dW

dt=!F. d !r

dt=!F.!v

• Alternative definition of instantaneous power: Pavg =

WΔt

Page 8: Chapter 7: Conservation of Energy - National MagLabshill/Teaching/2048 Spring11/Lecture12.pdf · Chapter 7: Conservation of Energy Chapter 9: Center of Mass and Momentum Tuesday February

General (calculus) method for calculating Work

ΔU = −Wc

= − Fc1Δx + Fc2Δx + ....FcjΔx + ...( )= − FcjΔx

j∑

ΔU = −Wc = − Fc (x)dx

xi

x f∫

Take the limit Δx → 0

Page 9: Chapter 7: Conservation of Energy - National MagLabshill/Teaching/2048 Spring11/Lecture12.pdf · Chapter 7: Conservation of Energy Chapter 9: Center of Mass and Momentum Tuesday February

Gravitational Potential Energy

ΔU = − (−mg)dyyi

y f∫ = mg dyyi

y f∫= mg y f − yi( ) = mgΔy = mgh

ΔU = −Wc = − Fc (x)dx

xi

x f∫Fg

-mg

yi yf

y

Constant Force

Fg = -mg

yi

yf

h

Page 10: Chapter 7: Conservation of Energy - National MagLabshill/Teaching/2048 Spring11/Lecture12.pdf · Chapter 7: Conservation of Energy Chapter 9: Center of Mass and Momentum Tuesday February

Gravitational Potential Energy

ΔU = + (+mg)dyyi

y f∫ = mg dyyi

y f∫= mg y f − yi( ) = mgΔy = mgh

Fg

-mg

yi yf

y

Constant Force

Fn.c. = mg

ΔU = +Wn.c. = + Fn.c.(x)dx

xi

x f∫

Page 11: Chapter 7: Conservation of Energy - National MagLabshill/Teaching/2048 Spring11/Lecture12.pdf · Chapter 7: Conservation of Energy Chapter 9: Center of Mass and Momentum Tuesday February

Elastic/Spring Potential Energy

ΔU = − (−kx)dxxi

x f∫ = k x dxxi

x f∫= 1

2 k x2⎡⎣ ⎤⎦xi

x f = 12 kx f

2 − 12 kxi

2

ΔU = −Wc = − Fc (x)dx

xi

x f∫F

xi xf

Fc = -kx Δx

Fc = -kx

U = − (−kx)dx0

x

∫ = k x dx0

x

∫= 1

2 k x2⎡⎣ ⎤⎦0

x= 1

2 kx2

0

x

-kxf