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Physics 1A, Section 7 October 8, 2007

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Physics 1A, Section 7. October 8, 2007. A modern look at historical laws of falling bodies. Oresme (14 th century): v  t s  t 2 (both correct). A modern look at historical laws of falling bodies. Galileo (17 th century):. - PowerPoint PPT Presentation

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Page 1: Physics 1A, Section 7

Physics 1A, Section 7

October 8, 2007

Page 2: Physics 1A, Section 7

• Oresme (14th century): v t

s t2

(both correct)

A modern look athistorical laws of falling bodies

Page 3: Physics 1A, Section 7

A modern look athistorical laws of falling bodies• Galileo (17th century):

time 1 2 3 4 5 …

s 1 3 5 7 9 …

Page 4: Physics 1A, Section 7

• Galileo (17th century):

time 1 2 3 4 5 …

s 1 3 5 7 9 …

s 1 4 9 16 25 …

A modern look athistorical laws of falling bodies

Page 5: Physics 1A, Section 7

• Galileo (17th century):

s t2 (correct)

time 1 2 3 4 5 …

s 1 3 5 7 9 …

s 1 4 9 16 25 …

A modern look athistorical laws of falling bodies

Page 6: Physics 1A, Section 7

• da Vinci (15th century):

time 1 2 3 4 5 …

s 1 2 3 4 5 …

A modern look athistorical laws of falling bodies

Page 7: Physics 1A, Section 7

• da Vinci (15th century):

time 1 2 3 4 5 …

s 1 2 3 4 5 …

s 1 3 6 10 15 …

A modern look athistorical laws of falling bodies

Page 8: Physics 1A, Section 7

• da Vinci (15th century):

s (t)(t + 1)/2 = t2/2 + t/2

time 1 2 3 4 5 …

s 1 2 3 4 5 …

s 1 3 6 10 15 …

A modern look athistorical laws of falling bodies

Page 9: Physics 1A, Section 7

• da Vinci (15th century):

s (t)(t + 1)/2 = t2/2 + t/2

v = ds/dt t + 1/2 (moving at the start)

time 1 2 3 4 5 …

s 1 2 3 4 5 …

s 1 3 6 10 15 …

A modern look athistorical laws of falling bodies

Page 10: Physics 1A, Section 7

• Albert of Saxony (14th century): v s

A modern look athistorical laws of falling bodies

Page 11: Physics 1A, Section 7

• Albert of Saxony (14th century): v s

ds/dt = s (ignored proportionality constant)

A modern look athistorical laws of falling bodies

Page 12: Physics 1A, Section 7

• Albert of Saxony (14th century): v s

ds/dt = s (ignored proportionality constant)

s = et (ignored another proportionality constant)

A modern look athistorical laws of falling bodies

Page 13: Physics 1A, Section 7

• Albert of Saxony (14th century): v s

ds/dt = s (ignored proportionality constant)

s = et (ignored another proportionality constant)

v = et

A modern look athistorical laws of falling bodies

Page 14: Physics 1A, Section 7

• Albert of Saxony (14th century): v s

ds/dt = s (ignored proportionality constant)

s = et (ignored another proportionality constant)

v = et

Takes an infinite time to start from infinitesimal velocity!

A modern look athistorical laws of falling bodies

Page 15: Physics 1A, Section 7

OM Chapter 1

Page 16: Physics 1A, Section 7

OM Chapter 1, part 2

Page 17: Physics 1A, Section 7

OM Chapter 2

Page 18: Physics 1A, Section 7

OM, Problem 2-72

Page 19: Physics 1A, Section 7

OM, Problem 2-72

• Answer: acceleration = 0.48 m/s2

time = 13.8 s

Page 20: Physics 1A, Section 7

Quiz Problem 35

Page 21: Physics 1A, Section 7

Quiz Problem 35

• Answer:a) a(t) = jt + a0

v(t) = jt2/2 + a0t + v0

x(t) = jt3/6 + a0t2/2 + v0t + x0

b)

c) A was ahead at t = 0.5 s.

d) J will win.0 0.5 1 1.5

time (s)

x

Car A

Car J

Page 22: Physics 1A, Section 7

OM, Problem 2-99

Page 23: Physics 1A, Section 7

OM, Problem 2-99

• Answer: a) n sqrt(2h/g)

b) 3h/4 above the ground

c) 2h/3 above the ground

(in the back of the book)

Page 24: Physics 1A, Section 7

Thursday, October 11:

• Quiz Problem 27

• TMU, Chapter 5, problem 40

• OM Chapter 3, problem 62

• OM Chapter 3, problem 63

• Optional to work on these in advance.