Trigonometric and Hyperbolic Functions

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Transcript of Trigonometric and Hyperbolic Functions

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Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Trigonometric and Hyperbolic Functions

Bernd Schroder

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

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Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Introduction

1. For real numbers θ we have eiθ = cos(θ)+ isin(θ).2. Replacing θ with −θ we obtain e−iθ = cos(θ)− isin(θ).

(Remember that the cosine is even and the sine is odd.)

3. Adding the two and dividing by 2 gives cos(θ) =eiθ + e−iθ

2.

4. Subtracting the two and dividing by 2i gives sin(θ) =eiθ − e−iθ

2i.

5. The right sides above make sense for all complex numbers.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

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Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Introduction1. For real numbers θ we have eiθ = cos(θ)+ isin(θ).

2. Replacing θ with −θ we obtain e−iθ = cos(θ)− isin(θ).(Remember that the cosine is even and the sine is odd.)

3. Adding the two and dividing by 2 gives cos(θ) =eiθ + e−iθ

2.

4. Subtracting the two and dividing by 2i gives sin(θ) =eiθ − e−iθ

2i.

5. The right sides above make sense for all complex numbers.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Introduction1. For real numbers θ we have eiθ = cos(θ)+ isin(θ).2. Replacing θ with −θ we obtain e−iθ = cos(θ)− isin(θ).

(Remember that the cosine is even and the sine is odd.)

3. Adding the two and dividing by 2 gives cos(θ) =eiθ + e−iθ

2.

4. Subtracting the two and dividing by 2i gives sin(θ) =eiθ − e−iθ

2i.

5. The right sides above make sense for all complex numbers.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Introduction1. For real numbers θ we have eiθ = cos(θ)+ isin(θ).2. Replacing θ with −θ we obtain e−iθ = cos(θ)− isin(θ).

(Remember that the cosine is even and the sine is odd.)

3. Adding the two and dividing by 2 gives cos(θ) =eiθ + e−iθ

2.

4. Subtracting the two and dividing by 2i gives sin(θ) =eiθ − e−iθ

2i.

5. The right sides above make sense for all complex numbers.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Introduction1. For real numbers θ we have eiθ = cos(θ)+ isin(θ).2. Replacing θ with −θ we obtain e−iθ = cos(θ)− isin(θ).

(Remember that the cosine is even and the sine is odd.)

3. Adding the two and dividing by 2 gives cos(θ) =eiθ + e−iθ

2.

4. Subtracting the two and dividing by 2i gives sin(θ) =eiθ − e−iθ

2i.

5. The right sides above make sense for all complex numbers.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Introduction1. For real numbers θ we have eiθ = cos(θ)+ isin(θ).2. Replacing θ with −θ we obtain e−iθ = cos(θ)− isin(θ).

(Remember that the cosine is even and the sine is odd.)

3. Adding the two and dividing by 2 gives cos(θ) =eiθ + e−iθ

2.

4. Subtracting the two and dividing by 2i gives sin(θ) =eiθ − e−iθ

2i.

5. The right sides above make sense for all complex numbers.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Introduction1. For real numbers θ we have eiθ = cos(θ)+ isin(θ).2. Replacing θ with −θ we obtain e−iθ = cos(θ)− isin(θ).

(Remember that the cosine is even and the sine is odd.)

3. Adding the two and dividing by 2 gives cos(θ) =eiθ + e−iθ

2.

4. Subtracting the two and dividing by 2i gives sin(θ) =eiθ − e−iθ

2i.

5. The right sides above make sense for all complex numbers.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

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Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Definition.

For any complex number z we define

cos(z) =eiz + e−iz

2and

sin(z) =eiz− e−iz

2i.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Definition. For any complex number z we define

cos(z) =eiz + e−iz

2

and

sin(z) =eiz− e−iz

2i.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Definition. For any complex number z we define

cos(z) =eiz + e−iz

2and

sin(z) =eiz− e−iz

2i.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

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Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

This Time, All Common Identities Carry Over

1. sin(z1 + z2) = sin(z1)cos(z2)+ cos(z1)sin(z2)2. cos(z1 + z2) = cos(z1)cos(z2)− sin(z1)sin(z2)3. sin2(z)+ cos2(z) = 14. sin(z+2π) = sin(z)5. cos(z+2π) = cos(z)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

This Time, All Common Identities Carry Over1. sin(z1 + z2) = sin(z1)cos(z2)+ cos(z1)sin(z2)

2. cos(z1 + z2) = cos(z1)cos(z2)− sin(z1)sin(z2)3. sin2(z)+ cos2(z) = 14. sin(z+2π) = sin(z)5. cos(z+2π) = cos(z)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

This Time, All Common Identities Carry Over1. sin(z1 + z2) = sin(z1)cos(z2)+ cos(z1)sin(z2)2. cos(z1 + z2) = cos(z1)cos(z2)− sin(z1)sin(z2)

3. sin2(z)+ cos2(z) = 14. sin(z+2π) = sin(z)5. cos(z+2π) = cos(z)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

This Time, All Common Identities Carry Over1. sin(z1 + z2) = sin(z1)cos(z2)+ cos(z1)sin(z2)2. cos(z1 + z2) = cos(z1)cos(z2)− sin(z1)sin(z2)3. sin2(z)+ cos2(z) = 1

4. sin(z+2π) = sin(z)5. cos(z+2π) = cos(z)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

This Time, All Common Identities Carry Over1. sin(z1 + z2) = sin(z1)cos(z2)+ cos(z1)sin(z2)2. cos(z1 + z2) = cos(z1)cos(z2)− sin(z1)sin(z2)3. sin2(z)+ cos2(z) = 14. sin(z+2π) = sin(z)

5. cos(z+2π) = cos(z)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

This Time, All Common Identities Carry Over1. sin(z1 + z2) = sin(z1)cos(z2)+ cos(z1)sin(z2)2. cos(z1 + z2) = cos(z1)cos(z2)− sin(z1)sin(z2)3. sin2(z)+ cos2(z) = 14. sin(z+2π) = sin(z)5. cos(z+2π) = cos(z)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Some Proofs Actually Are Simpler Now

sin(z1)cos(z2)+ cos(z1)sin(z2)

=eiz1− e−iz1

2ieiz2 + e−iz2

2+

eiz1 + e−iz1

2eiz2− e−iz2

2i

=14i

(ei(z1+z2) + ei(z1−z2)− ei(−z1+z2)− e−i(z1+z2)

+ ei(z1+z2)− ei(z1−z2) + ei(−z1+z2)− e−i(z1+z2))

=14i

(2ei(z1+z2)−2e−i(z1+z2)

)=

ei(z1+z2)− e−i(z1+z2)

2i= sin(z1 + z2)

This is why many people like to work with the complex definition ofthe trigonometric functions.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Some Proofs Actually Are Simpler Now

sin(z1)cos(z2)+ cos(z1)sin(z2)

=eiz1− e−iz1

2ieiz2 + e−iz2

2+

eiz1 + e−iz1

2eiz2− e−iz2

2i

=14i

(ei(z1+z2) + ei(z1−z2)− ei(−z1+z2)− e−i(z1+z2)

+ ei(z1+z2)− ei(z1−z2) + ei(−z1+z2)− e−i(z1+z2))

=14i

(2ei(z1+z2)−2e−i(z1+z2)

)=

ei(z1+z2)− e−i(z1+z2)

2i= sin(z1 + z2)

This is why many people like to work with the complex definition ofthe trigonometric functions.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Some Proofs Actually Are Simpler Now

sin(z1)cos(z2)+ cos(z1)sin(z2)

=eiz1− e−iz1

2ieiz2 + e−iz2

2+

eiz1 + e−iz1

2eiz2− e−iz2

2i

=14i

(ei(z1+z2) + ei(z1−z2)− ei(−z1+z2)− e−i(z1+z2)

+ ei(z1+z2)− ei(z1−z2) + ei(−z1+z2)− e−i(z1+z2))

=14i

(2ei(z1+z2)−2e−i(z1+z2)

)=

ei(z1+z2)− e−i(z1+z2)

2i= sin(z1 + z2)

This is why many people like to work with the complex definition ofthe trigonometric functions.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Some Proofs Actually Are Simpler Now

sin(z1)cos(z2)+ cos(z1)sin(z2)

=eiz1− e−iz1

2ieiz2 + e−iz2

2+

eiz1 + e−iz1

2eiz2− e−iz2

2i

=14i

(ei(z1+z2) + ei(z1−z2)− ei(−z1+z2)− e−i(z1+z2)

+ ei(z1+z2)− ei(z1−z2) + ei(−z1+z2)− e−i(z1+z2))

=14i

(2ei(z1+z2)−2e−i(z1+z2)

)=

ei(z1+z2)− e−i(z1+z2)

2i= sin(z1 + z2)

This is why many people like to work with the complex definition ofthe trigonometric functions.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Some Proofs Actually Are Simpler Now

sin(z1)cos(z2)+ cos(z1)sin(z2)

=eiz1− e−iz1

2ieiz2 + e−iz2

2+

eiz1 + e−iz1

2eiz2− e−iz2

2i

=14i

(ei(z1+z2) + ei(z1−z2)− ei(−z1+z2)− e−i(z1+z2)

+ ei(z1+z2)− ei(z1−z2) + ei(−z1+z2)− e−i(z1+z2))

=14i

(2ei(z1+z2)−2e−i(z1+z2)

)=

ei(z1+z2)− e−i(z1+z2)

2i= sin(z1 + z2)

This is why many people like to work with the complex definition ofthe trigonometric functions.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Some Proofs Actually Are Simpler Now

sin(z1)cos(z2)+ cos(z1)sin(z2)

=eiz1− e−iz1

2ieiz2 + e−iz2

2+

eiz1 + e−iz1

2eiz2− e−iz2

2i

=14i

(ei(z1+z2) + ei(z1−z2)− ei(−z1+z2)− e−i(z1+z2)

+ ei(z1+z2)− ei(z1−z2) + ei(−z1+z2)− e−i(z1+z2))

=14i

(2ei(z1+z2)−2e−i(z1+z2)

)

=ei(z1+z2)− e−i(z1+z2)

2i= sin(z1 + z2)

This is why many people like to work with the complex definition ofthe trigonometric functions.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Some Proofs Actually Are Simpler Now

sin(z1)cos(z2)+ cos(z1)sin(z2)

=eiz1− e−iz1

2ieiz2 + e−iz2

2+

eiz1 + e−iz1

2eiz2− e−iz2

2i

=14i

(ei(z1+z2) + ei(z1−z2)− ei(−z1+z2)− e−i(z1+z2)

+ ei(z1+z2)− ei(z1−z2) + ei(−z1+z2)− e−i(z1+z2))

=14i

(2ei(z1+z2)−2e−i(z1+z2)

)=

ei(z1+z2)− e−i(z1+z2)

2i

= sin(z1 + z2)

This is why many people like to work with the complex definition ofthe trigonometric functions.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Some Proofs Actually Are Simpler Now

sin(z1)cos(z2)+ cos(z1)sin(z2)

=eiz1− e−iz1

2ieiz2 + e−iz2

2+

eiz1 + e−iz1

2eiz2− e−iz2

2i

=14i

(ei(z1+z2) + ei(z1−z2)− ei(−z1+z2)− e−i(z1+z2)

+ ei(z1+z2)− ei(z1−z2) + ei(−z1+z2)− e−i(z1+z2))

=14i

(2ei(z1+z2)−2e−i(z1+z2)

)=

ei(z1+z2)− e−i(z1+z2)

2i= sin(z1 + z2)

This is why many people like to work with the complex definition ofthe trigonometric functions.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Some Proofs Actually Are Simpler Now

sin(z1)cos(z2)+ cos(z1)sin(z2)

=eiz1− e−iz1

2ieiz2 + e−iz2

2+

eiz1 + e−iz1

2eiz2− e−iz2

2i

=14i

(ei(z1+z2) + ei(z1−z2)− ei(−z1+z2)− e−i(z1+z2)

+ ei(z1+z2)− ei(z1−z2) + ei(−z1+z2)− e−i(z1+z2))

=14i

(2ei(z1+z2)−2e−i(z1+z2)

)=

ei(z1+z2)− e−i(z1+z2)

2i= sin(z1 + z2)

This is why many people like to work with the complex definition ofthe trigonometric functions.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Other Proofs Stay The Same

sin(z+2π) = sin(z)cos(2π)+ cos(z)sin(2π)= sin(z)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Other Proofs Stay The Same

sin(z+2π)

= sin(z)cos(2π)+ cos(z)sin(2π)= sin(z)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Other Proofs Stay The Same

sin(z+2π) = sin(z)cos(2π)+ cos(z)sin(2π)

= sin(z)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Other Proofs Stay The Same

sin(z+2π) = sin(z)cos(2π)+ cos(z)sin(2π)= sin(z)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

The Other Trigonometric Functions

1. tan(z) :=sin(z)cos(z)

2. cot(z) :=cos(z)sin(z)

3. sec(z) :=1

cos(z)

4. csc(z) :=1

sin(z)Note that secant and cosecant are not very common (around theworld).

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

The Other Trigonometric Functions1. tan(z) :=

sin(z)cos(z)

2. cot(z) :=cos(z)sin(z)

3. sec(z) :=1

cos(z)

4. csc(z) :=1

sin(z)Note that secant and cosecant are not very common (around theworld).

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

The Other Trigonometric Functions1. tan(z) :=

sin(z)cos(z)

2. cot(z) :=cos(z)sin(z)

3. sec(z) :=1

cos(z)

4. csc(z) :=1

sin(z)Note that secant and cosecant are not very common (around theworld).

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

The Other Trigonometric Functions1. tan(z) :=

sin(z)cos(z)

2. cot(z) :=cos(z)sin(z)

3. sec(z) :=1

cos(z)

4. csc(z) :=1

sin(z)Note that secant and cosecant are not very common (around theworld).

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

The Other Trigonometric Functions1. tan(z) :=

sin(z)cos(z)

2. cot(z) :=cos(z)sin(z)

3. sec(z) :=1

cos(z)

4. csc(z) :=1

sin(z)

Note that secant and cosecant are not very common (around theworld).

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

The Other Trigonometric Functions1. tan(z) :=

sin(z)cos(z)

2. cot(z) :=cos(z)sin(z)

3. sec(z) :=1

cos(z)

4. csc(z) :=1

sin(z)Note that secant and cosecant are not very common (around theworld).

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

The Derivatives

1.ddz

sin(z)=ddz

eiz−e−iz

2i=

ieiz+ie−iz

2i=

eiz+e−iz

2=cos(z)

2.ddz

cos(z) =−sin(z)

3.ddz

tan(z) =1

cos2(z)

4.ddz

cot(z) =− 1sin2(z)

5.ddz

sec(z) = sec(z) tan(z)

6.ddz

csc(z) =−csc(z)cot(z)

Note that secant and cosecant are not very common (around theworld).

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

The Derivatives

1.ddz

sin(z)

=ddz

eiz−e−iz

2i=

ieiz+ie−iz

2i=

eiz+e−iz

2=cos(z)

2.ddz

cos(z) =−sin(z)

3.ddz

tan(z) =1

cos2(z)

4.ddz

cot(z) =− 1sin2(z)

5.ddz

sec(z) = sec(z) tan(z)

6.ddz

csc(z) =−csc(z)cot(z)

Note that secant and cosecant are not very common (around theworld).

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

The Derivatives

1.ddz

sin(z)=ddz

eiz−e−iz

2i

=ieiz+ie−iz

2i=

eiz+e−iz

2=cos(z)

2.ddz

cos(z) =−sin(z)

3.ddz

tan(z) =1

cos2(z)

4.ddz

cot(z) =− 1sin2(z)

5.ddz

sec(z) = sec(z) tan(z)

6.ddz

csc(z) =−csc(z)cot(z)

Note that secant and cosecant are not very common (around theworld).

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

The Derivatives

1.ddz

sin(z)=ddz

eiz−e−iz

2i=

ieiz+ie−iz

2i

=eiz+e−iz

2=cos(z)

2.ddz

cos(z) =−sin(z)

3.ddz

tan(z) =1

cos2(z)

4.ddz

cot(z) =− 1sin2(z)

5.ddz

sec(z) = sec(z) tan(z)

6.ddz

csc(z) =−csc(z)cot(z)

Note that secant and cosecant are not very common (around theworld).

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

The Derivatives

1.ddz

sin(z)=ddz

eiz−e−iz

2i=

ieiz+ie−iz

2i=

eiz+e−iz

2

=cos(z)

2.ddz

cos(z) =−sin(z)

3.ddz

tan(z) =1

cos2(z)

4.ddz

cot(z) =− 1sin2(z)

5.ddz

sec(z) = sec(z) tan(z)

6.ddz

csc(z) =−csc(z)cot(z)

Note that secant and cosecant are not very common (around theworld).

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

The Derivatives

1.ddz

sin(z)=ddz

eiz−e−iz

2i=

ieiz+ie−iz

2i=

eiz+e−iz

2=cos(z)

2.ddz

cos(z) =−sin(z)

3.ddz

tan(z) =1

cos2(z)

4.ddz

cot(z) =− 1sin2(z)

5.ddz

sec(z) = sec(z) tan(z)

6.ddz

csc(z) =−csc(z)cot(z)

Note that secant and cosecant are not very common (around theworld).

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

The Derivatives

1.ddz

sin(z)=ddz

eiz−e−iz

2i=

ieiz+ie−iz

2i=

eiz+e−iz

2=cos(z)

2.ddz

cos(z) =−sin(z)

3.ddz

tan(z) =1

cos2(z)

4.ddz

cot(z) =− 1sin2(z)

5.ddz

sec(z) = sec(z) tan(z)

6.ddz

csc(z) =−csc(z)cot(z)

Note that secant and cosecant are not very common (around theworld).

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

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Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

The Derivatives

1.ddz

sin(z)=ddz

eiz−e−iz

2i=

ieiz+ie−iz

2i=

eiz+e−iz

2=cos(z)

2.ddz

cos(z) =−sin(z)

3.ddz

tan(z) =1

cos2(z)

4.ddz

cot(z) =− 1sin2(z)

5.ddz

sec(z) = sec(z) tan(z)

6.ddz

csc(z) =−csc(z)cot(z)

Note that secant and cosecant are not very common (around theworld).

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

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Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

The Derivatives

1.ddz

sin(z)=ddz

eiz−e−iz

2i=

ieiz+ie−iz

2i=

eiz+e−iz

2=cos(z)

2.ddz

cos(z) =−sin(z)

3.ddz

tan(z) =1

cos2(z)

4.ddz

cot(z) =− 1sin2(z)

5.ddz

sec(z) = sec(z) tan(z)

6.ddz

csc(z) =−csc(z)cot(z)

Note that secant and cosecant are not very common (around theworld).

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

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Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

The Derivatives

1.ddz

sin(z)=ddz

eiz−e−iz

2i=

ieiz+ie−iz

2i=

eiz+e−iz

2=cos(z)

2.ddz

cos(z) =−sin(z)

3.ddz

tan(z) =1

cos2(z)

4.ddz

cot(z) =− 1sin2(z)

5.ddz

sec(z) = sec(z) tan(z)

6.ddz

csc(z) =−csc(z)cot(z)

Note that secant and cosecant are not very common (around theworld).

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

The Derivatives

1.ddz

sin(z)=ddz

eiz−e−iz

2i=

ieiz+ie−iz

2i=

eiz+e−iz

2=cos(z)

2.ddz

cos(z) =−sin(z)

3.ddz

tan(z) =1

cos2(z)

4.ddz

cot(z) =− 1sin2(z)

5.ddz

sec(z) = sec(z) tan(z)

6.ddz

csc(z) =−csc(z)cot(z)

Note that secant and cosecant are not very common (around theworld).

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

The Derivatives

1.ddz

sin(z)=ddz

eiz−e−iz

2i=

ieiz+ie−iz

2i=

eiz+e−iz

2=cos(z)

2.ddz

cos(z) =−sin(z)

3.ddz

tan(z) =1

cos2(z)

4.ddz

cot(z) =− 1sin2(z)

5.ddz

sec(z) = sec(z) tan(z)

6.ddz

csc(z) =−csc(z)cot(z)

Note that secant and cosecant are not very common (around theworld).

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

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Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Definition.

For any complex number z we define

cosh(z) =ez + e−z

2and

sinh(z) =ez− e−z

2.

Note.

sin(iz) =eiiz− e−iiz

2i=

e−z− ez

2i= ii

ez− e−z

2i= isinh(z)

cos(iz) = cosh(z)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

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Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Definition. For any complex number z we define

cosh(z) =ez + e−z

2

and

sinh(z) =ez− e−z

2.

Note.

sin(iz) =eiiz− e−iiz

2i=

e−z− ez

2i= ii

ez− e−z

2i= isinh(z)

cos(iz) = cosh(z)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Definition. For any complex number z we define

cosh(z) =ez + e−z

2and

sinh(z) =ez− e−z

2.

Note.

sin(iz) =eiiz− e−iiz

2i=

e−z− ez

2i= ii

ez− e−z

2i= isinh(z)

cos(iz) = cosh(z)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Definition. For any complex number z we define

cosh(z) =ez + e−z

2and

sinh(z) =ez− e−z

2.

Note.

sin(iz) =eiiz− e−iiz

2i=

e−z− ez

2i= ii

ez− e−z

2i= isinh(z)

cos(iz) = cosh(z)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Definition. For any complex number z we define

cosh(z) =ez + e−z

2and

sinh(z) =ez− e−z

2.

Note.

sin(iz)

=eiiz− e−iiz

2i=

e−z− ez

2i= ii

ez− e−z

2i= isinh(z)

cos(iz) = cosh(z)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Definition. For any complex number z we define

cosh(z) =ez + e−z

2and

sinh(z) =ez− e−z

2.

Note.

sin(iz) =eiiz− e−iiz

2i

=e−z− ez

2i= ii

ez− e−z

2i= isinh(z)

cos(iz) = cosh(z)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Definition. For any complex number z we define

cosh(z) =ez + e−z

2and

sinh(z) =ez− e−z

2.

Note.

sin(iz) =eiiz− e−iiz

2i=

e−z− ez

2i

= iiez− e−z

2i= isinh(z)

cos(iz) = cosh(z)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Definition. For any complex number z we define

cosh(z) =ez + e−z

2and

sinh(z) =ez− e−z

2.

Note.

sin(iz) =eiiz− e−iiz

2i=

e−z− ez

2i= ii

ez− e−z

2i

= isinh(z)

cos(iz) = cosh(z)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Definition. For any complex number z we define

cosh(z) =ez + e−z

2and

sinh(z) =ez− e−z

2.

Note.

sin(iz) =eiiz− e−iiz

2i=

e−z− ez

2i= ii

ez− e−z

2i= isinh(z)

cos(iz) = cosh(z)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Definition. For any complex number z we define

cosh(z) =ez + e−z

2and

sinh(z) =ez− e−z

2.

Note.

sin(iz) =eiiz− e−iiz

2i=

e−z− ez

2i= ii

ez− e−z

2i= isinh(z)

cos(iz)

= cosh(z)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Definition. For any complex number z we define

cosh(z) =ez + e−z

2and

sinh(z) =ez− e−z

2.

Note.

sin(iz) =eiiz− e−iiz

2i=

e−z− ez

2i= ii

ez− e−z

2i= isinh(z)

cos(iz) = cosh(z)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Another Connection Between Sine and Hyperbolic Sine

|sin(z)|2

= sin(x+ iy)sin(x+ iy)=

(sin(x)cos(iy)+ sin(iy)cos(x)

)sin(x+ iy)

=(

sin(x)cosh(y)+ isinh(y)cos(x))×

×(

sin(x)cosh(y)− isinh(y)cos(x))

= sin2(x)cosh2(y)+ sinh2(y)cos2(x)+sinh2(y)sin2(x)− sinh2(y)sin2(x)

= sin2(x)(cosh2(y)− sinh2(y)

)+ sinh2(y)

(cos2(x)+ sin2(x)

)= sin2(x)+ sinh2(y)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

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Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Another Connection Between Sine and Hyperbolic Sine|sin(z)|2

= sin(x+ iy)sin(x+ iy)=

(sin(x)cos(iy)+ sin(iy)cos(x)

)sin(x+ iy)

=(

sin(x)cosh(y)+ isinh(y)cos(x))×

×(

sin(x)cosh(y)− isinh(y)cos(x))

= sin2(x)cosh2(y)+ sinh2(y)cos2(x)+sinh2(y)sin2(x)− sinh2(y)sin2(x)

= sin2(x)(cosh2(y)− sinh2(y)

)+ sinh2(y)

(cos2(x)+ sin2(x)

)= sin2(x)+ sinh2(y)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Another Connection Between Sine and Hyperbolic Sine|sin(z)|2

= sin(x+ iy)sin(x+ iy)

=(

sin(x)cos(iy)+ sin(iy)cos(x))sin(x+ iy)

=(

sin(x)cosh(y)+ isinh(y)cos(x))×

×(

sin(x)cosh(y)− isinh(y)cos(x))

= sin2(x)cosh2(y)+ sinh2(y)cos2(x)+sinh2(y)sin2(x)− sinh2(y)sin2(x)

= sin2(x)(cosh2(y)− sinh2(y)

)+ sinh2(y)

(cos2(x)+ sin2(x)

)= sin2(x)+ sinh2(y)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Another Connection Between Sine and Hyperbolic Sine|sin(z)|2

= sin(x+ iy)sin(x+ iy)=

(sin(x)cos(iy)+ sin(iy)cos(x)

)sin(x+ iy)

=(

sin(x)cosh(y)+ isinh(y)cos(x))×

×(

sin(x)cosh(y)− isinh(y)cos(x))

= sin2(x)cosh2(y)+ sinh2(y)cos2(x)+sinh2(y)sin2(x)− sinh2(y)sin2(x)

= sin2(x)(cosh2(y)− sinh2(y)

)+ sinh2(y)

(cos2(x)+ sin2(x)

)= sin2(x)+ sinh2(y)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Another Connection Between Sine and Hyperbolic Sine|sin(z)|2

= sin(x+ iy)sin(x+ iy)=

(sin(x)cos(iy)+ sin(iy)cos(x)

)sin(x+ iy)

=(

sin(x)cosh(y)+ isinh(y)cos(x))

××(

sin(x)cosh(y)− isinh(y)cos(x))

= sin2(x)cosh2(y)+ sinh2(y)cos2(x)+sinh2(y)sin2(x)− sinh2(y)sin2(x)

= sin2(x)(cosh2(y)− sinh2(y)

)+ sinh2(y)

(cos2(x)+ sin2(x)

)= sin2(x)+ sinh2(y)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Another Connection Between Sine and Hyperbolic Sine|sin(z)|2

= sin(x+ iy)sin(x+ iy)=

(sin(x)cos(iy)+ sin(iy)cos(x)

)sin(x+ iy)

=(

sin(x)cosh(y)+ isinh(y)cos(x))×

×(

sin(x)cosh(y)− isinh(y)cos(x))

= sin2(x)cosh2(y)+ sinh2(y)cos2(x)+sinh2(y)sin2(x)− sinh2(y)sin2(x)

= sin2(x)(cosh2(y)− sinh2(y)

)+ sinh2(y)

(cos2(x)+ sin2(x)

)= sin2(x)+ sinh2(y)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Another Connection Between Sine and Hyperbolic Sine|sin(z)|2

= sin(x+ iy)sin(x+ iy)=

(sin(x)cos(iy)+ sin(iy)cos(x)

)sin(x+ iy)

=(

sin(x)cosh(y)+ isinh(y)cos(x))×

×(

sin(x)cosh(y)− isinh(y)cos(x))

= sin2(x)cosh2(y)+ sinh2(y)cos2(x)

+sinh2(y)sin2(x)− sinh2(y)sin2(x)= sin2(x)

(cosh2(y)− sinh2(y)

)+ sinh2(y)

(cos2(x)+ sin2(x)

)= sin2(x)+ sinh2(y)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Another Connection Between Sine and Hyperbolic Sine|sin(z)|2

= sin(x+ iy)sin(x+ iy)=

(sin(x)cos(iy)+ sin(iy)cos(x)

)sin(x+ iy)

=(

sin(x)cosh(y)+ isinh(y)cos(x))×

×(

sin(x)cosh(y)− isinh(y)cos(x))

= sin2(x)cosh2(y)+ sinh2(y)cos2(x)+sinh2(y)sin2(x)− sinh2(y)sin2(x)

= sin2(x)(cosh2(y)− sinh2(y)

)+ sinh2(y)

(cos2(x)+ sin2(x)

)= sin2(x)+ sinh2(y)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Another Connection Between Sine and Hyperbolic Sine|sin(z)|2

= sin(x+ iy)sin(x+ iy)=

(sin(x)cos(iy)+ sin(iy)cos(x)

)sin(x+ iy)

=(

sin(x)cosh(y)+ isinh(y)cos(x))×

×(

sin(x)cosh(y)− isinh(y)cos(x))

= sin2(x)cosh2(y)+ sinh2(y)cos2(x)+sinh2(y)sin2(x)− sinh2(y)sin2(x)

= sin2(x)(cosh2(y)− sinh2(y)

)+ sinh2(y)

(cos2(x)+ sin2(x)

)

= sin2(x)+ sinh2(y)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Another Connection Between Sine and Hyperbolic Sine|sin(z)|2

= sin(x+ iy)sin(x+ iy)=

(sin(x)cos(iy)+ sin(iy)cos(x)

)sin(x+ iy)

=(

sin(x)cosh(y)+ isinh(y)cos(x))×

×(

sin(x)cosh(y)− isinh(y)cos(x))

= sin2(x)cosh2(y)+ sinh2(y)cos2(x)+sinh2(y)sin2(x)− sinh2(y)sin2(x)

= sin2(x)(cosh2(y)− sinh2(y)

)+ sinh2(y)

(cos2(x)+ sin2(x)

)= sin2(x)+ sinh2(y)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

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Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Theorem.

The only zeros of the complex sine function are thenumbers nπ where n is an integer.

Proof. The only solutions of

0 =∣∣sin(z)

∣∣2 =∣∣sin(x+ iy)

∣∣2 = sin2(x)+ sinh2(y)

are y = 0 and x = nπ . So z = nπ where n is an integer are the zeros ofthe sine function.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

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Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Theorem. The only zeros of the complex sine function are thenumbers nπ where n is an integer.

Proof. The only solutions of

0 =∣∣sin(z)

∣∣2 =∣∣sin(x+ iy)

∣∣2 = sin2(x)+ sinh2(y)

are y = 0 and x = nπ . So z = nπ where n is an integer are the zeros ofthe sine function.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Theorem. The only zeros of the complex sine function are thenumbers nπ where n is an integer.

Proof.

The only solutions of

0 =∣∣sin(z)

∣∣2 =∣∣sin(x+ iy)

∣∣2 = sin2(x)+ sinh2(y)

are y = 0 and x = nπ . So z = nπ where n is an integer are the zeros ofthe sine function.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

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Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Theorem. The only zeros of the complex sine function are thenumbers nπ where n is an integer.

Proof. The only solutions of

0 =∣∣sin(z)

∣∣2

=∣∣sin(x+ iy)

∣∣2 = sin2(x)+ sinh2(y)

are y = 0 and x = nπ . So z = nπ where n is an integer are the zeros ofthe sine function.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Theorem. The only zeros of the complex sine function are thenumbers nπ where n is an integer.

Proof. The only solutions of

0 =∣∣sin(z)

∣∣2 =∣∣sin(x+ iy)

∣∣2

= sin2(x)+ sinh2(y)

are y = 0 and x = nπ . So z = nπ where n is an integer are the zeros ofthe sine function.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Theorem. The only zeros of the complex sine function are thenumbers nπ where n is an integer.

Proof. The only solutions of

0 =∣∣sin(z)

∣∣2 =∣∣sin(x+ iy)

∣∣2 = sin2(x)+ sinh2(y)

are y = 0 and x = nπ . So z = nπ where n is an integer are the zeros ofthe sine function.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Theorem. The only zeros of the complex sine function are thenumbers nπ where n is an integer.

Proof. The only solutions of

0 =∣∣sin(z)

∣∣2 =∣∣sin(x+ iy)

∣∣2 = sin2(x)+ sinh2(y)

are y = 0

and x = nπ . So z = nπ where n is an integer are the zeros ofthe sine function.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Theorem. The only zeros of the complex sine function are thenumbers nπ where n is an integer.

Proof. The only solutions of

0 =∣∣sin(z)

∣∣2 =∣∣sin(x+ iy)

∣∣2 = sin2(x)+ sinh2(y)

are y = 0 and x = nπ .

So z = nπ where n is an integer are the zeros ofthe sine function.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Theorem. The only zeros of the complex sine function are thenumbers nπ where n is an integer.

Proof. The only solutions of

0 =∣∣sin(z)

∣∣2 =∣∣sin(x+ iy)

∣∣2 = sin2(x)+ sinh2(y)

are y = 0 and x = nπ . So z = nπ where n is an integer are the zeros ofthe sine function.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Theorem. The only zeros of the complex sine function are thenumbers nπ where n is an integer.

Proof. The only solutions of

0 =∣∣sin(z)

∣∣2 =∣∣sin(x+ iy)

∣∣2 = sin2(x)+ sinh2(y)

are y = 0 and x = nπ . So z = nπ where n is an integer are the zeros ofthe sine function.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

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Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Identities for Hyperbolic Functions

1.ddz

sinh(z) = cosh(z)

2.ddz

cosh(z) = sinh(z)

3. sinh(z1 + z2) = sinh(z1)cosh(z2)+ cosh(z1)sinh(z2)4. cosh(z1 + z2) = cosh(z1)cosh(z2)+ sinh(z1)sinh(z2)5. cosh2(z)− sinh2(z) = 16. sinh(z+2πi) = sinh(z)7. cosh(z+2πi) = cosh(z)

... and more. And they can all be verified straight from the definition.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

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Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Identities for Hyperbolic Functions1.

ddz

sinh(z) = cosh(z)

2.ddz

cosh(z) = sinh(z)

3. sinh(z1 + z2) = sinh(z1)cosh(z2)+ cosh(z1)sinh(z2)4. cosh(z1 + z2) = cosh(z1)cosh(z2)+ sinh(z1)sinh(z2)5. cosh2(z)− sinh2(z) = 16. sinh(z+2πi) = sinh(z)7. cosh(z+2πi) = cosh(z)

... and more. And they can all be verified straight from the definition.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

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Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Identities for Hyperbolic Functions1.

ddz

sinh(z) = cosh(z)

2.ddz

cosh(z) = sinh(z)

3. sinh(z1 + z2) = sinh(z1)cosh(z2)+ cosh(z1)sinh(z2)4. cosh(z1 + z2) = cosh(z1)cosh(z2)+ sinh(z1)sinh(z2)5. cosh2(z)− sinh2(z) = 16. sinh(z+2πi) = sinh(z)7. cosh(z+2πi) = cosh(z)

... and more. And they can all be verified straight from the definition.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

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Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Identities for Hyperbolic Functions1.

ddz

sinh(z) = cosh(z)

2.ddz

cosh(z) = sinh(z)

3. sinh(z1 + z2) = sinh(z1)cosh(z2)+ cosh(z1)sinh(z2)

4. cosh(z1 + z2) = cosh(z1)cosh(z2)+ sinh(z1)sinh(z2)5. cosh2(z)− sinh2(z) = 16. sinh(z+2πi) = sinh(z)7. cosh(z+2πi) = cosh(z)

... and more. And they can all be verified straight from the definition.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

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Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Identities for Hyperbolic Functions1.

ddz

sinh(z) = cosh(z)

2.ddz

cosh(z) = sinh(z)

3. sinh(z1 + z2) = sinh(z1)cosh(z2)+ cosh(z1)sinh(z2)4. cosh(z1 + z2) = cosh(z1)cosh(z2)+ sinh(z1)sinh(z2)

5. cosh2(z)− sinh2(z) = 16. sinh(z+2πi) = sinh(z)7. cosh(z+2πi) = cosh(z)

... and more. And they can all be verified straight from the definition.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Identities for Hyperbolic Functions1.

ddz

sinh(z) = cosh(z)

2.ddz

cosh(z) = sinh(z)

3. sinh(z1 + z2) = sinh(z1)cosh(z2)+ cosh(z1)sinh(z2)4. cosh(z1 + z2) = cosh(z1)cosh(z2)+ sinh(z1)sinh(z2)5. cosh2(z)− sinh2(z) = 1

6. sinh(z+2πi) = sinh(z)7. cosh(z+2πi) = cosh(z)

... and more. And they can all be verified straight from the definition.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Identities for Hyperbolic Functions1.

ddz

sinh(z) = cosh(z)

2.ddz

cosh(z) = sinh(z)

3. sinh(z1 + z2) = sinh(z1)cosh(z2)+ cosh(z1)sinh(z2)4. cosh(z1 + z2) = cosh(z1)cosh(z2)+ sinh(z1)sinh(z2)5. cosh2(z)− sinh2(z) = 16. sinh(z+2πi) = sinh(z)

7. cosh(z+2πi) = cosh(z)... and more. And they can all be verified straight from the definition.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Identities for Hyperbolic Functions1.

ddz

sinh(z) = cosh(z)

2.ddz

cosh(z) = sinh(z)

3. sinh(z1 + z2) = sinh(z1)cosh(z2)+ cosh(z1)sinh(z2)4. cosh(z1 + z2) = cosh(z1)cosh(z2)+ sinh(z1)sinh(z2)5. cosh2(z)− sinh2(z) = 16. sinh(z+2πi) = sinh(z)7. cosh(z+2πi) = cosh(z)

... and more. And they can all be verified straight from the definition.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Identities for Hyperbolic Functions1.

ddz

sinh(z) = cosh(z)

2.ddz

cosh(z) = sinh(z)

3. sinh(z1 + z2) = sinh(z1)cosh(z2)+ cosh(z1)sinh(z2)4. cosh(z1 + z2) = cosh(z1)cosh(z2)+ sinh(z1)sinh(z2)5. cosh2(z)− sinh2(z) = 16. sinh(z+2πi) = sinh(z)7. cosh(z+2πi) = cosh(z)

... and more.

And they can all be verified straight from the definition.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Identities for Hyperbolic Functions1.

ddz

sinh(z) = cosh(z)

2.ddz

cosh(z) = sinh(z)

3. sinh(z1 + z2) = sinh(z1)cosh(z2)+ cosh(z1)sinh(z2)4. cosh(z1 + z2) = cosh(z1)cosh(z2)+ sinh(z1)sinh(z2)5. cosh2(z)− sinh2(z) = 16. sinh(z+2πi) = sinh(z)7. cosh(z+2πi) = cosh(z)

... and more. And they can all be verified straight from the definition.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Theorem.

The only zeros of the complex hyperbolic sine function arethe numbers nπi, where n is an integer.

Proof. sinh(z) =−isin(iz) is equal to zero where sin(iz) is equal tozero. Hence the zeros of sinh(z) are at z = nπi, where n is an integer.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

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Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Theorem. The only zeros of the complex hyperbolic sine function arethe numbers nπi, where n is an integer.

Proof. sinh(z) =−isin(iz) is equal to zero where sin(iz) is equal tozero. Hence the zeros of sinh(z) are at z = nπi, where n is an integer.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

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Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Theorem. The only zeros of the complex hyperbolic sine function arethe numbers nπi, where n is an integer.

Proof.

sinh(z) =−isin(iz) is equal to zero where sin(iz) is equal tozero. Hence the zeros of sinh(z) are at z = nπi, where n is an integer.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Theorem. The only zeros of the complex hyperbolic sine function arethe numbers nπi, where n is an integer.

Proof. sinh(z) =−isin(iz)

is equal to zero where sin(iz) is equal tozero. Hence the zeros of sinh(z) are at z = nπi, where n is an integer.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Theorem. The only zeros of the complex hyperbolic sine function arethe numbers nπi, where n is an integer.

Proof. sinh(z) =−isin(iz) is equal to zero where sin(iz) is equal tozero.

Hence the zeros of sinh(z) are at z = nπi, where n is an integer.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Theorem. The only zeros of the complex hyperbolic sine function arethe numbers nπi, where n is an integer.

Proof. sinh(z) =−isin(iz) is equal to zero where sin(iz) is equal tozero. Hence the zeros of sinh(z) are at z = nπi, where n is an integer.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Theorem. The only zeros of the complex hyperbolic sine function arethe numbers nπi, where n is an integer.

Proof. sinh(z) =−isin(iz) is equal to zero where sin(iz) is equal tozero. Hence the zeros of sinh(z) are at z = nπi, where n is an integer.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

More Hyperbolic Functions

1. tanh(z) :=sinh(z)cosh(z)

2. coth(z) :=cosh(z)sinh(z)

3. sech(z) :=1

cosh(z)

4. csch(z) :=1

sinh(z)Note that hyperbolic secant and cosecant are not very common(around the world) either.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

More Hyperbolic Functions1. tanh(z) :=

sinh(z)cosh(z)

2. coth(z) :=cosh(z)sinh(z)

3. sech(z) :=1

cosh(z)

4. csch(z) :=1

sinh(z)Note that hyperbolic secant and cosecant are not very common(around the world) either.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

More Hyperbolic Functions1. tanh(z) :=

sinh(z)cosh(z)

2. coth(z) :=cosh(z)sinh(z)

3. sech(z) :=1

cosh(z)

4. csch(z) :=1

sinh(z)Note that hyperbolic secant and cosecant are not very common(around the world) either.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

More Hyperbolic Functions1. tanh(z) :=

sinh(z)cosh(z)

2. coth(z) :=cosh(z)sinh(z)

3. sech(z) :=1

cosh(z)

4. csch(z) :=1

sinh(z)Note that hyperbolic secant and cosecant are not very common(around the world) either.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

More Hyperbolic Functions1. tanh(z) :=

sinh(z)cosh(z)

2. coth(z) :=cosh(z)sinh(z)

3. sech(z) :=1

cosh(z)

4. csch(z) :=1

sinh(z)

Note that hyperbolic secant and cosecant are not very common(around the world) either.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

More Hyperbolic Functions1. tanh(z) :=

sinh(z)cosh(z)

2. coth(z) :=cosh(z)sinh(z)

3. sech(z) :=1

cosh(z)

4. csch(z) :=1

sinh(z)Note that hyperbolic secant and cosecant are not very common(around the world) either.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Remaining Derivatives

1.ddz

tanh(z) =1

cosh2(z)

2.ddz

coth(z) =− 1sinh2(z)

3.ddz

sech(z) =−sech(z) tanh(z)

4.ddz

csch(z) =−csch(z)coth(z)

Note that hyperbolic secant and cosecant are not very common(around the world) either.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

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Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Remaining Derivatives1.

ddz

tanh(z) =1

cosh2(z)

2.ddz

coth(z) =− 1sinh2(z)

3.ddz

sech(z) =−sech(z) tanh(z)

4.ddz

csch(z) =−csch(z)coth(z)

Note that hyperbolic secant and cosecant are not very common(around the world) either.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Remaining Derivatives1.

ddz

tanh(z) =1

cosh2(z)

2.ddz

coth(z) =− 1sinh2(z)

3.ddz

sech(z) =−sech(z) tanh(z)

4.ddz

csch(z) =−csch(z)coth(z)

Note that hyperbolic secant and cosecant are not very common(around the world) either.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Remaining Derivatives1.

ddz

tanh(z) =1

cosh2(z)

2.ddz

coth(z) =− 1sinh2(z)

3.ddz

sech(z) =−sech(z) tanh(z)

4.ddz

csch(z) =−csch(z)coth(z)

Note that hyperbolic secant and cosecant are not very common(around the world) either.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Remaining Derivatives1.

ddz

tanh(z) =1

cosh2(z)

2.ddz

coth(z) =− 1sinh2(z)

3.ddz

sech(z) =−sech(z) tanh(z)

4.ddz

csch(z) =−csch(z)coth(z)

Note that hyperbolic secant and cosecant are not very common(around the world) either.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Remaining Derivatives1.

ddz

tanh(z) =1

cosh2(z)

2.ddz

coth(z) =− 1sinh2(z)

3.ddz

sech(z) =−sech(z) tanh(z)

4.ddz

csch(z) =−csch(z)coth(z)

Note that hyperbolic secant and cosecant are not very common(around the world) either.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

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Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Theorem.

For all complex numbers z we have

arccos(z) =−i log(

z+ i(1− z2) 1

2

)where the right side is a multivalued function.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Theorem. For all complex numbers z we have

arccos(z) =−i log(

z+ i(1− z2) 1

2

)

where the right side is a multivalued function.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Theorem. For all complex numbers z we have

arccos(z) =−i log(

z+ i(1− z2) 1

2

)where the right side is a multivalued function.

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Proof.

w = arccos(z)cos(w) = z

eiw + e−iw

2= z

eiw−2z+ e−iw = 0(eiw)2−2zeiw +1 = 0

eiw =2z±√

4z2−42

= z±√

z2−1

w =1i

log(

z±√

z2−1)

= −i log(

z± i√

1− z2)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

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Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Proof.

w = arccos(z)

cos(w) = zeiw + e−iw

2= z

eiw−2z+ e−iw = 0(eiw)2−2zeiw +1 = 0

eiw =2z±√

4z2−42

= z±√

z2−1

w =1i

log(

z±√

z2−1)

= −i log(

z± i√

1− z2)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Proof.

w = arccos(z)cos(w) = z

eiw + e−iw

2= z

eiw−2z+ e−iw = 0(eiw)2−2zeiw +1 = 0

eiw =2z±√

4z2−42

= z±√

z2−1

w =1i

log(

z±√

z2−1)

= −i log(

z± i√

1− z2)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Proof.

w = arccos(z)cos(w) = z

eiw + e−iw

2= z

eiw−2z+ e−iw = 0(eiw)2−2zeiw +1 = 0

eiw =2z±√

4z2−42

= z±√

z2−1

w =1i

log(

z±√

z2−1)

= −i log(

z± i√

1− z2)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Proof.

w = arccos(z)cos(w) = z

eiw + e−iw

2= z

eiw−2z+ e−iw = 0

(eiw)2−2zeiw +1 = 0

eiw =2z±√

4z2−42

= z±√

z2−1

w =1i

log(

z±√

z2−1)

= −i log(

z± i√

1− z2)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Proof.

w = arccos(z)cos(w) = z

eiw + e−iw

2= z

eiw−2z+ e−iw = 0(eiw)2−2zeiw +1 = 0

eiw =2z±√

4z2−42

= z±√

z2−1

w =1i

log(

z±√

z2−1)

= −i log(

z± i√

1− z2)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Proof.

w = arccos(z)cos(w) = z

eiw + e−iw

2= z

eiw−2z+ e−iw = 0(eiw)2−2zeiw +1 = 0

eiw =2z±√

4z2−42

= z±√

z2−1

w =1i

log(

z±√

z2−1)

= −i log(

z± i√

1− z2)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Proof.

w = arccos(z)cos(w) = z

eiw + e−iw

2= z

eiw−2z+ e−iw = 0(eiw)2−2zeiw +1 = 0

eiw =2z±√

4z2−42

= z±√

z2−1

w =1i

log(

z±√

z2−1)

= −i log(

z± i√

1− z2)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Proof.

w = arccos(z)cos(w) = z

eiw + e−iw

2= z

eiw−2z+ e−iw = 0(eiw)2−2zeiw +1 = 0

eiw =2z±√

4z2−42

= z±√

z2−1

w =1i

log(

z±√

z2−1)

= −i log(

z± i√

1− z2)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Proof.

w = arccos(z)cos(w) = z

eiw + e−iw

2= z

eiw−2z+ e−iw = 0(eiw)2−2zeiw +1 = 0

eiw =2z±√

4z2−42

= z±√

z2−1

w =1i

log(

z±√

z2−1)

= −i log(

z± i√

1− z2)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Proof.

w = arccos(z)cos(w) = z

eiw + e−iw

2= z

eiw−2z+ e−iw = 0(eiw)2−2zeiw +1 = 0

eiw =2z±√

4z2−42

= z±√

z2−1

w =1i

log(

z±√

z2−1)

= −i log(

z± i√

1− z2)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Similarly We Can Derive ...

1. arcsin(z) =−i log(

iz+(1− z2) 1

2

)2. arctan(z) =

i2

log(

i+ zi− z

)3. arsinh(z) = log

(z+(1+ z2) 1

2

)4. arcosh(z) = log

(z+(z2−1

) 12

)5. artanh(z) =

12

log(

1+ z1− z

)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Similarly We Can Derive ...1. arcsin(z) =−i log

(iz+

(1− z2) 1

2

)

2. arctan(z) =i2

log(

i+ zi− z

)3. arsinh(z) = log

(z+(1+ z2) 1

2

)4. arcosh(z) = log

(z+(z2−1

) 12

)5. artanh(z) =

12

log(

1+ z1− z

)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Similarly We Can Derive ...1. arcsin(z) =−i log

(iz+

(1− z2) 1

2

)2. arctan(z) =

i2

log(

i+ zi− z

)

3. arsinh(z) = log(

z+(1+ z2) 1

2

)4. arcosh(z) = log

(z+(z2−1

) 12

)5. artanh(z) =

12

log(

1+ z1− z

)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Similarly We Can Derive ...1. arcsin(z) =−i log

(iz+

(1− z2) 1

2

)2. arctan(z) =

i2

log(

i+ zi− z

)3. arsinh(z) = log

(z+(1+ z2) 1

2

)

4. arcosh(z) = log(

z+(z2−1

) 12

)5. artanh(z) =

12

log(

1+ z1− z

)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Similarly We Can Derive ...1. arcsin(z) =−i log

(iz+

(1− z2) 1

2

)2. arctan(z) =

i2

log(

i+ zi− z

)3. arsinh(z) = log

(z+(1+ z2) 1

2

)4. arcosh(z) = log

(z+(z2−1

) 12

)

5. artanh(z) =12

log(

1+ z1− z

)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Similarly We Can Derive ...1. arcsin(z) =−i log

(iz+

(1− z2) 1

2

)2. arctan(z) =

i2

log(

i+ zi− z

)3. arsinh(z) = log

(z+(1+ z2) 1

2

)4. arcosh(z) = log

(z+(z2−1

) 12

)5. artanh(z) =

12

log(

1+ z1− z

)

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

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Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Theorem.

ddz

arcsin(z) =1

(1− z2)12

where the right side is

multivalued again.

Proof.ddz

arcsin(z) =ddz

(−i log

(iz+

(1− z2) 1

2

))= −i

1

iz+(1− z2)12

(i+

12

1

(1− z2)12(−2z)

)

=−i

iz+(1− z2)12

i(1− z2

) 12 − z

(1− z2)12

=

1

(1− z2)12

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

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Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Theorem.ddz

arcsin(z) =1

(1− z2)12

where the right side is

multivalued again.

Proof.ddz

arcsin(z) =ddz

(−i log

(iz+

(1− z2) 1

2

))= −i

1

iz+(1− z2)12

(i+

12

1

(1− z2)12(−2z)

)

=−i

iz+(1− z2)12

i(1− z2

) 12 − z

(1− z2)12

=

1

(1− z2)12

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

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Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Theorem.ddz

arcsin(z) =1

(1− z2)12

where the right side is

multivalued again.

Proof.ddz

arcsin(z) =ddz

(−i log

(iz+

(1− z2) 1

2

))= −i

1

iz+(1− z2)12

(i+

12

1

(1− z2)12(−2z)

)

=−i

iz+(1− z2)12

i(1− z2

) 12 − z

(1− z2)12

=

1

(1− z2)12

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Theorem.ddz

arcsin(z) =1

(1− z2)12

where the right side is

multivalued again.

Proof.

ddz

arcsin(z) =ddz

(−i log

(iz+

(1− z2) 1

2

))= −i

1

iz+(1− z2)12

(i+

12

1

(1− z2)12(−2z)

)

=−i

iz+(1− z2)12

i(1− z2

) 12 − z

(1− z2)12

=

1

(1− z2)12

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Theorem.ddz

arcsin(z) =1

(1− z2)12

where the right side is

multivalued again.

Proof.ddz

arcsin(z)

=ddz

(−i log

(iz+

(1− z2) 1

2

))= −i

1

iz+(1− z2)12

(i+

12

1

(1− z2)12(−2z)

)

=−i

iz+(1− z2)12

i(1− z2

) 12 − z

(1− z2)12

=

1

(1− z2)12

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Theorem.ddz

arcsin(z) =1

(1− z2)12

where the right side is

multivalued again.

Proof.ddz

arcsin(z) =ddz

(−i log

(iz+

(1− z2) 1

2

))

= −i1

iz+(1− z2)12

(i+

12

1

(1− z2)12(−2z)

)

=−i

iz+(1− z2)12

i(1− z2

) 12 − z

(1− z2)12

=

1

(1− z2)12

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Theorem.ddz

arcsin(z) =1

(1− z2)12

where the right side is

multivalued again.

Proof.ddz

arcsin(z) =ddz

(−i log

(iz+

(1− z2) 1

2

))= −i

1

iz+(1− z2)12

(i+

12

1

(1− z2)12(−2z)

)

=−i

iz+(1− z2)12

i(1− z2

) 12 − z

(1− z2)12

=

1

(1− z2)12

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Theorem.ddz

arcsin(z) =1

(1− z2)12

where the right side is

multivalued again.

Proof.ddz

arcsin(z) =ddz

(−i log

(iz+

(1− z2) 1

2

))= −i

1

iz+(1− z2)12

(i+

12

1

(1− z2)12(−2z)

)

=−i

iz+(1− z2)12

i(1− z2

) 12 − z

(1− z2)12

=1

(1− z2)12

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Theorem.ddz

arcsin(z) =1

(1− z2)12

where the right side is

multivalued again.

Proof.ddz

arcsin(z) =ddz

(−i log

(iz+

(1− z2) 1

2

))= −i

1

iz+(1− z2)12

(i+

12

1

(1− z2)12(−2z)

)

=−i

iz+(1− z2)12

i(1− z2

) 12 − z

(1− z2)12

=

1

(1− z2)12

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Theorem.ddz

arcsin(z) =1

(1− z2)12

where the right side is

multivalued again.

Proof.ddz

arcsin(z) =ddz

(−i log

(iz+

(1− z2) 1

2

))= −i

1

iz+(1− z2)12

(i+

12

1

(1− z2)12(−2z)

)

=−i

iz+(1− z2)12

i(1− z2

) 12 − z

(1− z2)12

=

1

(1− z2)12

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Similarly ...

1.ddz

arccos(z) =− 1

(1− z2)12

2.ddz

arctan(z) =1

1+ z2

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Similarly ...1.

ddz

arccos(z) =− 1

(1− z2)12

2.ddz

arctan(z) =1

1+ z2

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions

logo1

Trigonometric Functions Hyperbolic Functions Inverse Trigonometric and Hyperbolic Functions

Similarly ...1.

ddz

arccos(z) =− 1

(1− z2)12

2.ddz

arctan(z) =1

1+ z2

Bernd Schroder Louisiana Tech University, College of Engineering and Science

Trigonometric and Hyperbolic Functions