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Eulers formula without calculus Steven Taschuk Intersections K W - - PowerPoint PPT Presentation

Eulers formula without calculus Steven Taschuk Intersections K W 2014 September 16 Eulers formula e iv = cos v + i sin v ( i 2 = 1) Leonhard Euler (17071783) Introductio in Analysin Infinitorum (1748), p. 104 CotesEuler


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SLIDE 1

Euler’s formula without calculus

Steven Taschuk

Intersections K ∩ W

2014 September 16

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SLIDE 2

Euler’s formula

eiv = cos v + i sin v (i2 = −1) Introductio in Analysin Infinitorum (1748), p. 104 Leonhard Euler (1707–1783)

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Cotes–Euler formula

eiv = cos v + i sin v (i2 = −1) “Logometria” (1714), p. 31 Roger Cotes (1682–1716)

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Cotes–Euler formula: a proof

For any real number x, ex = x0 0! + x1 1! + x2 2! + x3 3! + x4 4! + x5 5! + · · · Assume this holds for complex exponents too. Then eiv = (iv)0 0! + (iv)1 1! + (iv)2 2! + (iv)3 3! + (iv)4 4! + (iv)5 5! + · · · = v0 0! + iv1 1! − v2 2! − iv3 3! + v4 4! + iv5 5! − v6 6! − iv7 7! + · · · = cos v + i sin v

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Elementary definition of exponentiation

an =

n copies

  • a · a · · · a
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SLIDE 6

Elementary definition of exponentiation

an =

n copies

  • a · a · · · a

a0 = 1

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SLIDE 7

Elementary definition of exponentiation

an =

n copies

  • a · a · · · a

a0 = 1 a−n = 1 an

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SLIDE 8

Elementary definition of exponentiation

an =

n copies

  • a · a · · · a

a0 = 1 a−n = 1 an am/n =

n

√ am

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SLIDE 9

Elementary definition of exponentiation

an =

n copies

  • a · a · · · a

a0 = 1 a−n = 1 an am/n =

n

√ am ax = lim

m n →x am/n

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SLIDE 10

Reason for defining a0 and a−n as we do

a4 = a · a · a · a a3 = a · a · a ↑ ×a a2 = a · a ↓ ÷a a1 = a

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SLIDE 11

Reason for defining a0 and a−n as we do

a4 = a · a · a · a a3 = a · a · a ↑ ×a a2 = a · a ↓ ÷a a1 = a a0 = 1

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SLIDE 12

Reason for defining a0 and a−n as we do

a4 = a · a · a · a a3 = a · a · a ↑ ×a a2 = a · a ↓ ÷a a1 = a a0 = 1 a−1 = 1 a

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SLIDE 13

Reason for defining a0 and a−n as we do

a4 = a · a · a · a a3 = a · a · a ↑ ×a a2 = a · a ↓ ÷a a1 = a a0 = 1 a−1 = 1 a a−2 = 1 a2

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SLIDE 14

Reason for defining a0 and a−n as we do

a4 = a · a · a · a a3 = a · a · a ↑ ×a a2 = a · a ↓ ÷a a1 = a a0 = 1 a−1 = 1 a a−2 = 1 a2 i.e., we assume an+1 = an · a is also valid for negative exponents.

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Functional def’n of exponentiation (integer exponents)

Theorem

For every positive number a, there is exactly one function f : Z → R such that

◮ f (1) = a, and ◮ f (m + n) = f (m)f (n) for all m, n ∈ Z.

We write f (n) = an.

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Functional def’n of exponentiation (rational exponents)

Theorem

For every positive number a, there is exactly one function f : Q → R such that

◮ f (1) = a, and ◮ f (p + q) = f (p)f (q) for all p, q ∈ Q.

We write f (q) = aq.

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Functional def’n of exponentiation (real exponents)

Theorem

For every positive number a, there is exactly one function f : R → R such that

◮ f (1) = a, and ◮ f (u + v) = f (u)f (v) for all u, v ∈ R.

We write f (v) = av. FALSE (assuming the axiom of choice)

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SLIDE 18

Functional def’n of exponentiation (real exponents)

Theorem

For every positive number a, there is exactly one function f : R → R such that

◮ f (1) = a, and ◮ f (u + v) = f (u)f (v) for all u, v ∈ R, and ◮ f is continuous.

We write f (v) = av. TRUE

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Cotes–Euler formula: a proof

For any real number x, ex = x0 0! + x1 1! + x2 2! + x3 3! + x4 4! + x5 5! + · · · Assume this holds for complex exponents too. Then eiv = (iv)0 0! + (iv)1 1! + (iv)2 2! + (iv)3 3! + (iv)4 4! + (iv)5 5! + · · · = v0 0! + iv1 1! − v2 2! − iv3 3! + v4 4! + iv5 5! − v6 6! − iv7 7! + · · · = cos v + i sin v

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SLIDE 20

Cotes–Euler formula without calculus: part 0

eu+iv = eueiv

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Cotes–Euler formula without calculus: part 1

Let eiv = C(v) + iS(v); want to show C = cos, S = sin. ei(u+v) = eiu+iv = eiueiv C(u + v) + iS(u + v) = (C(u) + iS(u))(C(v) + iS(v)) = (C(u)C(v) − S(u)S(v)) + i(S(u)C(v) + C(u)S(v)) C(u + v) = C(u)C(v) − S(u)S(v) S(u + v) = S(u)C(v) + C(u)S(v)

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Cotes–Euler formula without calculus: part 2

Theorem

If C, S : R → R satisfy

◮ C(u + v) = C(u)C(v) − S(u)S(v) for all u, v ∈ R, and ◮ S(u + v) = S(u)C(v) + C(u)S(v) for all u, v ∈ R, and ◮ C and S are not both identically zero, and ◮ C and S are continuous,

then there exist b, λ ∈ R, b > 0, such that C(v) = bv cos(λv) and S(v) = bv sin(λv) .

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Characterization of sine and cosine: proof outline

  • 1. Isolate the exponential part.

(Let f (v) =

  • C(v)2 + S(v)2; show f (u + v) = f (u)f (v).

Replace C, S with C/f , S/f .)

  • 2. Prove identities, esp. C(2v) = 2C(v)2 − 1.
  • 3. Prove that C has a root (or is constant).

(If 0 ≤ C(v) ≤ 1 then 1 − C(2v) ≥ 2(1 − C(v)); so if C(v) = 1 then some C(2nv) < 0.)

  • 4. Let λ = π

2p, where p is the smallest positive root of C;

successively extend C(v) = cos(λv) from v = p to v of form p/2n to v of form mp/2n to v ∈ R

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SLIDE 24

Functional def’n of exponentiation (real exponents)

Theorem

For every positive number a, there is exactly one function f : R → R such that

◮ f (1) = a, and ◮ f (u + v) = f (u)f (v) for all u, v ∈ R, and ◮ f is continuous.

We write f (v) = av.

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SLIDE 25

Cotes–Euler formula without calculus: part 0

eu+iv = eueiv

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SLIDE 26

Cotes–Euler formula without calculus: part 1

Let eiv = C(v) + iS(v); want to show C = cos, S = sin. ei(u+v) = eiu+iv = eiueiv C(u + v) + iS(u + v) = (C(u) + iS(u))(C(v) + iS(v)) = (C(u)C(v) − S(u)S(v)) + i(S(u)C(v) + C(u)S(v)) C(u + v) = C(u)C(v) − S(u)S(v) S(u + v) = S(u)C(v) + C(u)S(v)

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Cotes–Euler formula without calculus: part 2

Theorem

If C, S : R → R satisfy

◮ C(u + v) = C(u)C(v) − S(u)S(v) for all u, v ∈ R, and ◮ S(u + v) = S(u)C(v) + C(u)S(v) for all u, v ∈ R, and ◮ C and S are not both identically zero, and ◮ C and S are continuous,

then there exist b, λ ∈ R, b > 0, such that C(v) = bv cos(λv) and S(v) = bv sin(λv) .

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(Almost) Cotes-Euler formula without calculus

eiv = bv(cos(λv) + i sin(λv))

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(Almost) Cotes-Euler formula without calculus

eiv = bv(cos(λv) + i sin(λv)) INSERT PICTURES HERE

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(Almost) Cotes-Euler formula without calculus

eiv = bv(cos(λv) + i sin(λv)) INSERT PICTURES HERE

◮ Getting b = 1:

◮ further assume ez = ez

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SLIDE 31

(Almost) Cotes-Euler formula without calculus

eiv = bv(cos(λv) + i sin(λv)) INSERT PICTURES HERE

◮ Getting b = 1:

◮ further assume ez = ez

◮ Getting λ = 1:

◮ further assume (ab)z = azbz ◮ . . . and normalize a logarithm