Канал: Andrew Nicoll

Detecting Floods with Artificial Intelligence | International Conference of Undergraduate Research

Detecting Floods with Artificial Intelligence | International Conference of Undergraduate Research

The Wavelet Transform for Beginners

The Wavelet Transform for Beginners

Modular Arithmetic Around a Circle in Python

Modular Arithmetic Around a Circle in Python

Deriving the Electric Field of a Dipole

Deriving the Electric Field of a Dipole

Green's Theorem: Proof - Part 2

Green's Theorem: Proof - Part 2

Green's Theorem: Proof - Part 1

Green's Theorem: Proof - Part 1

(Levi-cevita symbol) Proving that the divergence of a curl and the curl of a gradient are zero

(Levi-cevita symbol) Proving that the divergence of a curl and the curl of a gradient are zero

Introduction to Dissipative forces - Power functions and damped pendulums

Introduction to Dissipative forces - Power functions and damped pendulums

Equations of motion of a pendulum attached to a mass on a spring

Equations of motion of a pendulum attached to a mass on a spring

Derivation of Gauss' Law from scratch using the inverse square law and the divergence theorem

Derivation of Gauss' Law from scratch using the inverse square law and the divergence theorem

The quantum harmonic oscillator (part 2) - Finding the wave functions of excited states

The quantum harmonic oscillator (part 2) - Finding the wave functions of excited states

The quantum harmonic oscillator: Solving the differential equation for the ground state

The quantum harmonic oscillator: Solving the differential equation for the ground state

The quantum harmonic oscillator (Part 1) - Finding the eigenstates, eigenvalues and wave fucntions

The quantum harmonic oscillator (Part 1) - Finding the eigenstates, eigenvalues and wave fucntions

Proving "the cancellation of dots" equation

Proving "the cancellation of dots" equation

Proof of Snell's law using Fermat's Principle and the Euler-Lagrange equation

Proof of Snell's law using Fermat's Principle and the Euler-Lagrange equation

Differential equations: The integrating factor

Differential equations: The integrating factor

Finding the volume of a cube using integration techniques

Finding the volume of a cube using integration techniques

Integrating parametric equations to find the area.

Integrating parametric equations to find the area.

Andrew Nicoll Live Stream

Andrew Nicoll Live Stream

Gauss' law for electric fields part 1 - The basics

Gauss' law for electric fields part 1 - The basics

Particles and potential steps: E-v(0) - Particle is reflected even though it has enough energy. - p

Particles and potential steps: E-v(0) - Particle is reflected even though it has enough energy. - p

Reflection and transmission coefficients

Reflection and transmission coefficients

Particles and potential steps: E-v(0) - part 2

Particles and potential steps: E-v(0) - part 2

particles and potential steps: E greater than V

particles and potential steps: E greater than V

Symmetric square well potentials

Symmetric square well potentials

Particle in an infinite square well (part 5)

Particle in an infinite square well (part 5)

Particle in an infinite square well (part 4)

Particle in an infinite square well (part 4)

Particle in an infinite square well (part 3) (cut short)

Particle in an infinite square well (part 3) (cut short)

Particle in an infinite square well (part 2)

Particle in an infinite square well (part 2)

Particle in an infinite square well (part 1)

Particle in an infinite square well (part 1)

Deriving the time-independent Schrödinger equation

Deriving the time-independent Schrödinger equation

Exercise VII (solution): Quantum Mechanics - Solving the time - dependent Schrödinger equation

Exercise VII (solution): Quantum Mechanics - Solving the time - dependent Schrödinger equation

Exercise VII: Quantum Mechanics - Solving the time-dependent Schrödinger equation

Exercise VII: Quantum Mechanics - Solving the time-dependent Schrödinger equation

Two books I recommend for people starting out in REAL physics.

Two books I recommend for people starting out in REAL physics.

Derivation of Lagrange's Equations - part 3

Derivation of Lagrange's Equations - part 3

Derivation of Lagrange's Equations - part 2

Derivation of Lagrange's Equations - part 2

Derivation of Lagrange's Equations - Part 1

Derivation of Lagrange's Equations - Part 1

Hamiltonian for the Lagrangian of a particle in circular motion

Hamiltonian for the Lagrangian of a particle in circular motion

Hamilton's Equations and the Harmonic Oscillator

Hamilton's Equations and the Harmonic Oscillator

Lagrangian of a particle in circular motion with changing radius (polar coordinates)

Lagrangian of a particle in circular motion with changing radius (polar coordinates)

Derivation of Hamilton's Equations

Derivation of Hamilton's Equations

Using a surface integral to derive the surface area of a torus (part 6) - Integration

Using a surface integral to derive the surface area of a torus (part 6) - Integration

Using a surface integral to derive the surface area of a torus (part 5) - Simplification

Using a surface integral to derive the surface area of a torus (part 5) - Simplification

Using a surface integral to derive the surface area of a torus (part 4) - The cross product

Using a surface integral to derive the surface area of a torus (part 4) - The cross product

Using a surface integral to derive the surface area of a torus (part 3) - Partial Derivatives

Using a surface integral to derive the surface area of a torus (part 3) - Partial Derivatives

Using a surface integral to derive the surface area of a torus (part 2) - Vector valued function

Using a surface integral to derive the surface area of a torus (part 2) - Vector valued function

Using a surface integral to derive the surface area of a torus (part 1) - The General Picture

Using a surface integral to derive the surface area of a torus (part 1) - The General Picture

Escape velocity in Earth's gravitational field (Proof)

Escape velocity in Earth's gravitational field (Proof)

Forming differential equations: Example 1 - Direct proportion type

Forming differential equations: Example 1 - Direct proportion type

Proof of Kepler's 3rd law of planetary motion (Easy derivation)

Proof of Kepler's 3rd law of planetary motion (Easy derivation)

Path independence for line integrals

Path independence for line integrals

Using a line integral to calculate work done.

Using a line integral to calculate work done.

Proof that the divergence of a curl and the curl of a gradient are both equal to zero

Proof that the divergence of a curl and the curl of a gradient are both equal to zero

Exercise VI (solution) part 2: Classical Mechanics - Equation of motion for a disk

Exercise VI (solution) part 2: Classical Mechanics - Equation of motion for a disk

Exercise VI (Solution) part 1: Classical Mechanics - Equation of motion for a disk

Exercise VI (Solution) part 1: Classical Mechanics - Equation of motion for a disk

Exercise VI: Classical Mechanics - Equation of motion of a disk rolling down an inclined plane.

Exercise VI: Classical Mechanics - Equation of motion of a disk rolling down an inclined plane.

Integration by U-Substitution: 2 Examples - Trig and limits

Integration by U-Substitution: 2 Examples - Trig and limits

The Implicit Function Theorem

The Implicit Function Theorem

Classical Mechanics: An overview of the series and lectures

Classical Mechanics: An overview of the series and lectures

Integration by U - Substitution: 2 Examples: Root and exponential functions

Integration by U - Substitution: 2 Examples: Root and exponential functions

Exercise V (Solution): Classical Mechanics - Equations of motion of a pendulum

Exercise V (Solution): Classical Mechanics - Equations of motion of a pendulum

Exercise v: Classical Mechanics - Equations of motion of a pendulum

Exercise v: Classical Mechanics - Equations of motion of a pendulum

Integration by U - Substitution: 2 Examples

Integration by U - Substitution: 2 Examples

A level physics: Vectors - Part 2

A level physics: Vectors - Part 2

A level physics: Vectors - Part 1

A level physics: Vectors - Part 1

8 important Feynman diagrams to learn

8 important Feynman diagrams to learn

Exercise IV (solution): Special Relativity - Prove that E=pc

Exercise IV (solution): Special Relativity - Prove that E=pc

Exercise IV: Special Relativity - Prove that E=pc

Exercise IV: Special Relativity - Prove that E=pc

Differentiation: The Chain rule - Example 2 (Easy)

Differentiation: The Chain rule - Example 2 (Easy)

Differentiation: The chain rule - Example 1 (Hard)

Differentiation: The chain rule - Example 1 (Hard)

Proof - Force is equal to the negative derivative of potential energy

Proof - Force is equal to the negative derivative of potential energy

Integration: Integration by parts - Example 1 (The natural log)

Integration: Integration by parts - Example 1 (The natural log)

Exercise III (solution): classical mechanics - Conservation of energy

Exercise III (solution): classical mechanics - Conservation of energy

Problem 1 ( Overview):Quantum mechanics - Can you see why the phase factor can be ignored

Problem 1 ( Overview):Quantum mechanics - Can you see why the phase factor can be ignored

Binomial Expansion: Formula - part 1

Binomial Expansion: Formula - part 1

Exercise III: Classical mechanics - Conservation of energy ( single particle in 1 dimension)

Exercise III: Classical mechanics - Conservation of energy ( single particle in 1 dimension)

Exercise II (solution): Quantum mechanics - Eiganvalues of any hermitian operator are real numbers.

Exercise II (solution): Quantum mechanics - Eiganvalues of any hermitian operator are real numbers.

Exercise II: Quantum mechanics - Eieganvalues of an hermition operator are real numbers.

Exercise II: Quantum mechanics - Eieganvalues of an hermition operator are real numbers.

Problem 1: Quantum mechanics - Can you see why the phase factor can be ignored?

Problem 1: Quantum mechanics - Can you see why the phase factor can be ignored?

Exercise 1 (Solution): Classical mechanics - The Lagrangian and the Hamiltonian

Exercise 1 (Solution): Classical mechanics - The Lagrangian and the Hamiltonian

Exercise 1: Classical mechanics - The Lagrangian and the Hamiltonian

Exercise 1: Classical mechanics - The Lagrangian and the Hamiltonian

Differentiation: Using the definition of a derivative - Example 3 ( The natural log)

Differentiation: Using the definition of a derivative - Example 3 ( The natural log)

8 important limits to memorize

8 important limits to memorize

Types of derivative Notation

Types of derivative Notation

Differentiation: Using the definition of a derivative - Example 2

Differentiation: Using the definition of a derivative - Example 2

Differentiation: Using the definition of a derivative - Example 1

Differentiation: Using the definition of a derivative - Example 1

A level physics: Electromagnetic Waves

A level physics: Electromagnetic Waves

A level physics: Electromagnetic Induction part 2

A level physics: Electromagnetic Induction part 2

A level physics: Electromagnetic Induction part 1

A level physics: Electromagnetic Induction part 1

A level particle physics 3 of 5

A level particle physics 3 of 5

A level physics: Nuclear Energy

A level physics: Nuclear Energy

A level physics: Deformation of solids

A level physics: Deformation of solids

A level particle physics 1 of 5

A level particle physics 1 of 5

A level physics: Hooke's law and Young's modulus

A level physics: Hooke's law and Young's modulus

A level physics: Units, quantities and measurements

A level physics: Units, quantities and measurements

A level physics: Power and Energy

A level physics: Power and Energy

A level physics: Alternating Currents

A level physics: Alternating Currents

A level physics: Comparisons of electric and gravitational fields

A level physics: Comparisons of electric and gravitational fields

A level physics: Wave Particle Duality

A level physics: Wave Particle Duality

A level particle physics 2 of 5

A level particle physics 2 of 5