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Today, we are going to explore the simple pendulum. Can anyone tell me what a pendulum is?
Is it that thing that swings back and forth like a clock?
Exactly! A simple pendulum consists of a mass, or bob, attached to a string that swings around a pivot point. It exhibits periodic motion, which means it repeats its motion over time. What do you think affects the time it takes for it to swing back and forth?
Maybe the weight of the bob?
Not quite. It's primarily affected by the length of the string. The longer the string, the longer the period. Letβs remember: Longer string = Longer period. This will help you when calculating the time period shortly.
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As the pendulum swings, what forces do you think are acting on it?
I think there's gravity pulling it down.
Correct! The tension in the string also plays a role. When displaced, the gravitational force can be split into two components. The tangential force tries to bring the bob back toward its equilibrium position, and the radial force provides centripetal acceleration. Can anyone express this in terms of a formula?
I think it relates to torque, like Ο = -L(mg sin ΞΈ)!
Excellent! This torque initiates the restoring force that leads to oscillation. Remember this key point: The restoring torque is directed toward the equilibrium position.
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When the bob is displaced from its mean position, how is the motion mathematically represented?
Does it follow SHM equations?
Correct! For small angles, we can approximate sin ΞΈ as ΞΈ. This makes the motion resemble simple harmonic motion with an angular frequency given by Ο = β(g/L). Can anyone tell me what limits the pendulum's motion from being SHM?
Is it the size of the angle? If it's too big, it won't be accurate?
Absolutely! For large angles, we canβt use that approximation anymore. But for small angles, it holds true. Good to remember: For SHM, keep ΞΈ small!
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Now, letβs derive the formula for the period of a simple pendulum. Can you remind me what the time period formula is?
It's T = 2Οβ(L/g)!
Correct! This formula shows how the period is related to the length and acceleration due to gravity. Why do we need to consider g in this equation?
Because g affects how fast the bob would fall due to gravity!
Exactly! So, a pendulum on the Moon would have a longer period compared to one on Earth due to the weaker gravitational pull. Keep this in mind: Period varies inversely with the square root of g.
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Finally, can anyone provide an example of where simple pendulums are used in real life?
Like in clocks?
Exactly! Pendulums are essential in traditional clocks for keeping time accurately. Understanding their motion helps us create precisely timed mechanical systems. Anyone else think of another example?
How about in amusement park rides?
Great example! Pendulum motions can be seen in rides that swing and oscillate. Remember: The physics of pendulums plays a vital role in various applications!
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The simple pendulum, consisting of a mass (bob) attached to a long string, swings back and forth in a periodic motion. For small angles, the motion can be approximated as simple harmonic motion with a specific relationship between its length and the period of oscillation. Various forces act on the pendulum bob, leading to restoring torque that enables its oscillations.
The simple pendulum consists of a bob of mass m attached to a massless inextensible string of length L. This pendulum swings around a fixed point, executing periodic motion. When the bob is displaced from its vertical equilibrium position by a small angle ΞΈ, gravitational forces lead to a restoring torque that brings it back to equilibrium.
\[ \tau = -L(mg \sin \theta) \]
\[ I \alpha = -mgL \sin \theta \]
Giving rise to an angular motion approximation, the motion becomes simple harmonic for small angles:
\[ \alpha \approx -\frac{mg}{I} \theta = -\frac{g}{L} \theta \]
The relationship between the pendulum length and the period is captured by the formula:
\[ T = 2\pi \sqrt{\frac{L}{g}} \]
Where T is the time period of the pendulum, L is the length, and g is the acceleration due to gravity.
In conclusion, a simple pendulum exhibits periodic motion closely related to simple harmonic motion (SHM) when the angle of displacement is small, enabling the derivation of its oscillation period based on length.
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It is said that Galileo measured the periods of a swinging chandelier in a church by his pulse beats. He observed that the motion of the chandelier was periodic. The system is a kind of pendulum. You can also make your own pendulum by tying a piece of stone to a long unstretchable thread, approximately 100 cm long. Suspend your pendulum from a suitable support so that it is free to oscillate. Displace the stone to one side by a small distance and release it.
A simple pendulum consists of a mass (the bob) attached to a string that swings back and forth. When an object, like a stone, is tied to a string and pulled to one side, it experiences gravitational forces and swings freely, creating periodic motion. This motion is observed in nature and has fascinated scientists historically, such as Galileo, who famously measured the time between swings using his pulse.
Imagine watching a swing in a park; when you push it to one side and let go, it moves back and forth in a smooth arc, similar to how the bob of a pendulum moves along a circular path.
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Consider simple pendulum β a small bob of mass m tied to an inextensible massless string of length L. The other end of the string is fixed to a rigid support. The bob oscillates in a plane about the vertical line through the support. Fig. 13.17(a) shows this system. Fig. 13.17(b) is a kind of βfree-bodyβ diagram of the simple pendulum showing the forces acting on the bob.
In analyzing the forces at play, there are two main forces acting on the bob: tension (T) from the string, directed along the string, and gravitational force (mg), pointing downwards. This gravitational force can be broken into two components: one that acts along the string and another that acts perpendicular to it, which is responsible for changing the direction of the bob. Understanding these forces is crucial for determining how the bob will move.
Think of how when you swing a bucket of water in a circular path, the tension in your arm keeps the bucket moving in a circle while gravity tries to pull it down. Just like your arm provides the necessary force to keep the water from spilling out, the string in a pendulum holds the bob up while still letting it swing down.
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There are only two forces acting on the bob; the tension T along the string and the vertical force due to gravity (=mg). The force mg can be resolved into the component mg cosΞΈ along the string and mg sin ΞΈ perpendicular to it. Since the motion of the bob is along a circle of length L and centre at the support point, the bob has a radial acceleration (ΟΒ²L) and also a tangential acceleration; the latter arises since motion along the arc of the circle is not uniform.
When the bob swings away from its mean (vertical) position, gravity causes it to experience a tangential force (mg sin ΞΈ), which creates a restoring torque that pulls the bob back toward the center. This restoring force is what keeps the motion of the pendulum oscillating back and forth, and the relationship is similar to a spring bringing something back to its original shape after being stretched.
Imagine pulling back a rubber band and then releasing it; the band snaps back to its resting state. Similarly, when you pull the pendulum bob to the side, gravity acts like the rubber band, pulling it back toward the center.
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Now if ΞΈ is small, sin ΞΈ can be approximated by ΞΈ and Eq. (13.22) can then be written as, Ξ± = - (mg / L) I ΞΈ. This is mathematically identical to the equation for simple harmonic motion.
For small angles, we can simplify the mathematics by assuming that sin(ΞΈ) is approximately equal to ΞΈ (in radians). This allows us to express the angular motion of the pendulum in a way that mirrors simple harmonic motion equations, revealing that the pendulum's movement exhibits harmonic characteristics when the angles are small.
Think of your arm as you swing a small flashlight. At small angles, your arm's swinging path is nearly straight, similar to the pendulum's behavior. It allows us to predict its motion using simpler mathematics.
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Now since the string of the simple pendulum is massless, the moment of inertia I is simply mLΒ². Eq. (13.25) then gives the well-known formula for time period of a simple pendulum: T = 2Οβ(L/g).
The time period (T) of a simple pendulum is the time it takes to complete one full oscillation. It depends on the length of the string and acceleration due to gravity. Specifically, the longer the pendulum, the more time it takes to swing back and forth, which is represented in the formula derived from earlier equations.
Consider a child on a swing: a longer swing takes more time to go back and forth than a shorter swing, illustrating how pendulums behave similarly according to their lengths.
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What is the length of a simple pendulum, which ticks seconds? Answer: From Eq. (13.26), for g = 9.8 m/sΒ² and T = 2s, L = (gTΒ²)/(4ΟΒ²) = 1 m.
To find the length of a pendulum that ticks once per second, we can rearrange our previously derived formula. Substituting in the values for gravitational force and time (2 seconds for a full swing), we can calculate that the pendulum needs to be 1 meter long to achieve this ticking time. This direct relationship between length and period is crucial in timing mechanisms.
Just like the pendulum in a grandfather clock, adjusting its length determines how fast it ticks, connecting the mechanics of physics to the practical function of telling time.
Learn essential terms and foundational ideas that form the basis of the topic.
Key Concepts
Pendulum Dynamics: The pendulum swings about a fixed point, with the period related to its length and gravitational acceleration.
Forces at Work: The roles of tension and gravitational force are crucial for understanding the pendulum's motion.
Torque and SHM: The relationship between pendulum torque and simple harmonic motion is established for small angles.
See how the concepts apply in real-world scenarios to understand their practical implications.
A clock that uses a pendulum to keep time accurately.
Swing rides at amusement parks that demonstrate pendulum motion.
Use mnemonics, acronyms, or visual cues to help remember key information more easily.
Pendulum swings in time, like a clock keeping its rhyme. Longer the cord, longer the swing, each second's a beautiful ring.
Once upon a time in a village, there was a clock tower with a pendulum. The longer the pendulum, the slower the tick. It became the village's way to ensure everyone was on time!
Remember: T - Time = L - Length / G - Gravity for Pendulums.
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Review the Definitions for terms.
Term: Pendulum
Definition:
A weight suspended from a pivot so that it can swing back and forth.
Term: Restoring Torque
Definition:
The torque that acts to bring the pendulum bob back to its mean position.
Term: Angular Frequency (Ο)
Definition:
The rate of oscillation of the pendulum in radians per second.
Term: Time Period (T)
Definition:
The time taken for one complete cycle of motion.