Everything You Need To Know About Pendulums: Physics Help Room

Physics with Elliot
14 Sept 202114:41
EducationalLearning
32 Likes 10 Comments

TLDRIn this educational video, Elliot introduces the concept of pendulums, focusing on the simple pendulum to explore physical principles. He explains the setup, including the mass, length, and equilibrium position, then follows Newtonian mechanics to derive the equation of motion. Elliot simplifies the problem using the small angle approximation, leading to a sinusoidal motion pattern. The video covers natural frequency, period, and the independence of mass on oscillation rate, concluding with an interactive animation to deepen understanding.

Takeaways
  • πŸ“š The video is a physics tutorial focused on pendulums, aiming to teach physical principles through the study of simple pendulums.
  • πŸ” Elliot, the presenter, explains the setup of a simple pendulum, consisting of a mass 'm' attached to a rod of length 'l', pivoted at one end.
  • πŸ“ The video uses coordinates, specifically angle theta or arc length 's', to describe the pendulum's position and motion.
  • 🧩 Elliot introduces a three-step procedure in Newtonian mechanics to predict pendulum motion: drawing a free body diagram, applying Newton's second law, and solving the resulting equation.
  • πŸ“‰ The forces acting on the pendulum are identified as gravity and the tension in the rod, with only the component of gravity contributing to the pendulum's motion.
  • πŸ“ The video demonstrates the geometric relationship between the forces and the pendulum's motion, leading to the equation of motion for theta.
  • πŸ”„ The equation of motion for a pendulum is derived as ΞΈ'' = -(g/l)sin(ΞΈ), which governs the pendulum's oscillation.
  • πŸ“‰ For small angles, a simplification is made by approximating sin(ΞΈ) as ΞΈ, leading to a simpler harmonic motion equation.
  • πŸŒ€ The natural frequency of the pendulum, Ο‰, is introduced, which depends on gravity and the length of the pendulum, but not the mass.
  • πŸ” The general solution for the pendulum's motion, under the small angle approximation, is given as a combination of sine and cosine functions of Ο‰t.
  • ⏱ The period 'T' of the pendulum, the time for one complete oscillation, is derived and shown to be independent of the pendulum's mass and initial angle for small oscillations.
  • πŸ“š Elliot provides additional resources such as notes and problem sheets for further understanding and practice.
Q & A
  • What is the focus of the video on pendulums?

    -The video focuses on the simple pendulum, which consists of a ball of mass 'm' attached to a rod of length 'l' that is pivoted at its other end, allowing it to rotate freely.

  • What are the two coordinates that can be used to specify the position of a pendulum?

    -The two coordinates that can be used are the angle theta that the rod makes with the vertical, and the arc length coordinate 's' that is traced out along the circle by the particle.

  • Why is the rod in a simple pendulum considered to be massless?

    -The rod is considered massless because its mass is much lighter than the ball, allowing us to effectively treat it as having no mass for the purposes of the pendulum's motion analysis.

  • What is the equilibrium position of the pendulum?

    -The equilibrium position of the pendulum is when theta or 's' is equal to zero, which is the lowest point of its arc where the pendulum will sit at rest.

  • What is the three-step procedure in Newtonian mechanics for predicting the motion of the pendulum?

    -The three-step procedure is: 1) Draw the free body diagram showing all forces acting on the particle, 2) Write Newton's second law (F = ma) by summing all forces, and 3) Solve the equation to determine the trajectory of the pendulum over time.

  • What are the two forces acting on the particle in the simple pendulum?

    -The two forces are gravity (mg pulling straight down) and the tension 'T' in the rod pulling back toward the center of the circle.

  • Why does the tension in the rod not contribute to the total force in the tangent direction?

    -The tension in the rod does not contribute because it points radially inward toward the center of the circle, which is perpendicular to the tangent direction of the particle's motion.

  • What is the equation of motion for theta in a pendulum?

    -The equation of motion for theta is ΞΈ'' = -(g/l) * sin(ΞΈ), which is a differential equation that governs the motion of the pendulum.

  • What is the small angle approximation and when can it be applied?

    -The small angle approximation is an assumption that sine of theta is approximately equal to theta itself when theta is small (less than about half a radian or 30 degrees). It simplifies the equation of motion and can be applied when the pendulum does not deviate significantly from the equilibrium position.

  • What is the natural frequency of a pendulum and how is it determined?

    -The natural frequency, denoted by Ο‰, is a measure of how fast the pendulum oscillates. It is determined by the square root of the gravitational acceleration 'g' divided by the length of the pendulum 'l'.

  • How does the mass of the pendulum's bob affect the period of oscillation?

    -The mass of the bob does not affect the period of oscillation. The period depends only on the length of the pendulum and the gravitational acceleration, as shown by the formula T = 2Ο€βˆš(l/g).

  • What happens to the pendulum's motion when the small angle approximation breaks down?

    -When the small angle approximation breaks down (i.e., at larger angles), the motion is still periodic but is no longer sinusoidal. The pendulum may even swing all the way around the pivot if given a large enough initial kick.

Outlines
00:00
πŸ“š Introduction to Simple Pendulums

Elliot introduces the concept of simple pendulums, a fundamental system in physics for understanding various physical principles. He explains the basic setup of a simple pendulum, which consists of a mass m attached to a rod of length l that is pivoted at one end, allowing it to rotate freely. The focus is on predicting the pendulum's motion using coordinates, either the angle theta with the vertical or the arc length s. Elliot emphasizes the importance of the equilibrium position where the pendulum is at rest and introduces the three-step Newtonian mechanics procedure to analyze the pendulum's motion, starting with a free body diagram.

05:01
πŸ” Analyzing the Pendulum's Motion

In this section, Elliot delves into the specifics of analyzing the pendulum's motion using Newton's laws. He describes the forces acting on the pendulum, namely gravity and the tension in the rod, and how these forces contribute to the pendulum's motion. Elliot uses geometric reasoning to derive the tangential force acting on the pendulum, which is a component of gravity, and simplifies the equation of motion using the small angle approximation. This leads to a differential equation that governs the pendulum's motion, which can be solved to find the trajectory of the pendulum as a function of time, given certain initial conditions.

10:01
🌟 Simple Harmonic Motion and Periodicity

Elliot discusses the special case of simple harmonic motion for pendulums with small angles, where the motion can be approximated as sinusoidal. He defines the natural frequency of the pendulum, represented by omega, which depends on the length of the pendulum and the acceleration due to gravity, but not on the mass of the pendulum. Elliot explains that the period of the pendulum, the time for one complete oscillation, can be derived from the natural frequency and is independent of the initial angle for small oscillations. He also provides a problem for viewers to test their understanding and mentions additional resources, including notes and a problem sheet, available on his website.

πŸŽ₯ Visualizing and Understanding Pendulum Motion

In the final paragraph, Elliot provides a visual representation of the pendulum's motion over time through an animation, allowing viewers to adjust initial conditions and observe the resulting motion. He points out that for small initial angles, the motion is sinusoidal, but for larger angles or high initial speeds, the motion deviates from this pattern. Elliot encourages viewers to interact with the animation to build intuition about the physics involved and reiterates the availability of notes and a problem sheet for further learning. He concludes the video with a call to action for likes, subscriptions, and comments, inviting viewers to engage with the content and suggest future topics.

Mindmap
Keywords
πŸ’‘Pendulum
A pendulum is a weight suspended from a pivot so that it can swing freely. In the video, the pendulum serves as the central object of study, illustrating fundamental physical principles. The script discusses the simple pendulum, emphasizing its motion and the factors affecting it, such as the mass of the ball (m) and the length of the rod (l).
πŸ’‘Simple Pendulum
A simple pendulum is a specific type of pendulum with a small mass (m) attached to a rod (or string) of length (l) that is pivoted at the other end. The video focuses on this type to explore the motion of pendulums in a controlled manner, highlighting the importance of the angle theta and the arc length s in describing its motion.
πŸ’‘Equilibrium Position
The equilibrium position in the context of a pendulum is the point at which it would naturally rest without any external forces acting on it, typically the lowest point in its swing. The script mentions that when the angle theta or arc length s is equal to zero, the pendulum is at its equilibrium position.
πŸ’‘Newtonian Mechanics
Newtonian mechanics refers to the classical physics framework based on Isaac Newton's laws of motion. The video outlines a three-step procedure from Newtonian mechanics to predict the pendulum's motion: drawing a free body diagram, applying Newton's second law (F=ma), and solving the equation to find the trajectory.
πŸ’‘Free Body Diagram
A free body diagram is a tool used in physics to visualize all the forces acting on an object. In the script, it is used to depict the forces on the pendulum, such as gravity (mg) and the tension (T) in the rod, which are essential for deriving the pendulum's equation of motion.
πŸ’‘Tangent Component
The tangent component of a force is the part of the force that acts along the direction of motion. The script explains that only the tangential component of gravity (mg * sin(theta)) contributes to the pendulum's motion, as it is the only force component that points along the circle's path.
πŸ’‘Differential Equation
A differential equation is an equation that involves derivatives of a function. In the video, the equation of motion for the pendulum, theta double dot equals minus g over l times sine of theta, is a differential equation that describes how the pendulum's angle changes over time.
πŸ’‘Small Angle Approximation
The small angle approximation is a simplification used when the angle is sufficiently small, allowing the sine of the angle to be approximated as equal to the angle itself. The script uses this approximation to simplify the pendulum's equation of motion for cases where the pendulum does not deviate much from the equilibrium position.
πŸ’‘Natural Frequency
The natural frequency (denoted as capital omega in the script) is the rate at which an oscillating system, like a pendulum, vibrates. It is derived from the equation of motion and depends on the length of the pendulum and the acceleration due to gravity, but not on the mass of the pendulum.
πŸ’‘Period
The period of an oscillating system is the time it takes to complete one full cycle of motion. In the context of the pendulum, the script explains that the period (T) is the time for the pendulum to swing back to its starting position and is given by 2Ο€ times the square root of the length of the pendulum divided by the acceleration due to gravity.
Highlights

Introduction to pendulums and their importance in learning physical principles.

Focus on the simple pendulum with a mass m attached to a rod of length l.

Assumption of the rod being massless and the ball as a point particle for simplicity.

Setting up coordinates using angle theta or arc length s for pendulum motion analysis.

Equilibrium position of the pendulum at theta or s equal to zero.

Three-step Newtonian mechanics procedure for predicting pendulum motion.

Drawing the free body diagram to identify forces acting on the pendulum.

Force analysis considering gravity and tension in the rod.

Derivation of the equation of motion for the pendulum using Newton's second law.

Simplification of the equation using the small angle approximation for theta.

Solution of the simplified equation for pendulum motion under small angle conditions.

Introduction of the natural frequency omega and its dependence on g and l.

General solution for pendulum motion with initial conditions theta0 and theta0 dot.

Independence of the pendulum's period from its mass, demonstrating mass-independence.

Explanation of the pendulum's periodic motion and its relation to the natural frequency.

Discussion on the effect of initial angle on the period of the pendulum at larger amplitudes.

Animation demonstration of pendulum motion for different initial conditions.

Availability of notes, problem sheets, and additional resources for further understanding.

Conclusion and call to action for viewers to engage with the content and provide feedback.

Transcripts
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