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3/29/13 1 Physics 132 Theme Music: Benny Goodman Swing, Swing, Swing Cartoon: Bill Watterson Calvin & Hobbes March 29, 2013 Physics 132 Prof. E. F. Redish

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Page 1: Swing, Swing, Swing - UMD Department of Physics - … Physics 132 1 Theme Music: Benny Goodman Swing, Swing, Swing Cartoon: Bill Watterson Calvin & Hobbes March 29, 2013 Physics 132

3/29/13 1 Physics 132

 Theme Music: Benny Goodman Swing, Swing, Swing  Cartoon: Bill Watterson

Calvin & Hobbes

March 29, 2013 Physics 132 Prof. E. F. Redish

Page 2: Swing, Swing, Swing - UMD Department of Physics - … Physics 132 1 Theme Music: Benny Goodman Swing, Swing, Swing Cartoon: Bill Watterson Calvin & Hobbes March 29, 2013 Physics 132

3/29/13 2 Physics 132

Mathematical structure  Express a = Fnet/m in terms of derivatives.

 Except for the constant, this is like having a functions that is its own second derivative.

  In calculus, we learn that sin(t) and cos(t)

work like this. How about: ?

d 2 fdt 2

= ! f

tx cos=

d 2xdt 2

= !" 02x

Page 3: Swing, Swing, Swing - UMD Department of Physics - … Physics 132 1 Theme Music: Benny Goodman Swing, Swing, Swing Cartoon: Bill Watterson Calvin & Hobbes March 29, 2013 Physics 132

3/29/13 3 Physics 132

  We can easily take the derivatives to show that our solution satisfies the N2 equations

  What do the various terms mean? –  A is the maximum displacement — the amplitude. –  What is ω0? If T is the period (how long it takes

to go through a full oscillation) then

TT

Ttt

!"!"

!"

22

0:20:

00

0

=#=

$$

Interpreting the Result

x(t) = Acos(! 0t)

Page 4: Swing, Swing, Swing - UMD Department of Physics - … Physics 132 1 Theme Music: Benny Goodman Swing, Swing, Swing Cartoon: Bill Watterson Calvin & Hobbes March 29, 2013 Physics 132

3/29/13 4 Physics 132

Graphs: sin(θ) vs cos(θ)   Which is which? How can you tell?   The two functions sin and cos are

derivatives of each other (slopes), but one has a minus sign. Which one? How can you tell?

θ

1 sin θ

cos θ

Page 5: Swing, Swing, Swing - UMD Department of Physics - … Physics 132 1 Theme Music: Benny Goodman Swing, Swing, Swing Cartoon: Bill Watterson Calvin & Hobbes March 29, 2013 Physics 132

3/29/13 5 Physics 132

Graphs: sin(θ) vs sin(ω0t)   For angles, θ = 0 and θ = 2π are the same

so you only get one cycle.   For time, t can go on forever

so the cycles repeat.

cos(θ) cos(ω0t)

What does changing ω0 do to this graph?

Page 6: Swing, Swing, Swing - UMD Department of Physics - … Physics 132 1 Theme Music: Benny Goodman Swing, Swing, Swing Cartoon: Bill Watterson Calvin & Hobbes March 29, 2013 Physics 132

3/29/13 6 Physics 132

Interpreting the Result  What about the starting point?

Using cos means you always start at a peak when t = 0. That might not always be true.

x

t

t 0

x(t) = Acos(!0t)

x(t) = Acos(!0(t " t0))

x(t) = Acos(!0(t " t0))= Acos(!0t "!0t0) = Acos(!0t "#)

Page 7: Swing, Swing, Swing - UMD Department of Physics - … Physics 132 1 Theme Music: Benny Goodman Swing, Swing, Swing Cartoon: Bill Watterson Calvin & Hobbes March 29, 2013 Physics 132

3/29/13 8 Physics 132

Summary with Equations: Mass on a spring FS!M

FE!Ma = 1

mFnet Fnet = !kx

a = !" 02x " 0

2 = km

x(t) = Acos(" 0t +#)

" 0 =2$T

Measured from where?

Interpret!

Page 8: Swing, Swing, Swing - UMD Department of Physics - … Physics 132 1 Theme Music: Benny Goodman Swing, Swing, Swing Cartoon: Bill Watterson Calvin & Hobbes March 29, 2013 Physics 132

3/29/13 9 Physics 132

Summary with Equations: Mass on a spring (Energy) FS!M

FE!M

E = 12 mv

2 +mgh + 12 k !l( )2

Ei = Ef

Measured from where?

Page 9: Swing, Swing, Swing - UMD Department of Physics - … Physics 132 1 Theme Music: Benny Goodman Swing, Swing, Swing Cartoon: Bill Watterson Calvin & Hobbes March 29, 2013 Physics 132

3/29/13 11 Physics 132

The Long Pendulum

Page 10: Swing, Swing, Swing - UMD Department of Physics - … Physics 132 1 Theme Music: Benny Goodman Swing, Swing, Swing Cartoon: Bill Watterson Calvin & Hobbes March 29, 2013 Physics 132

3/29/13 12 Physics 132

Pendulum motion energy E0 = 1

2 mv2 +mgh = 1

2 mv2 +mgL(1! cos" )

cos" #1! 12"

2

E0 # 12 mv

2 + 12 mgL[ ]" 2

" # sin" = xL

E0 # 12 mv

2 + 12 kx

2 k = mgL

Same as mass on a spring! Just with a different ω0

2 = k/m =g/L

What’s the period? Why doesn’t it depend on m?