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determination of acceleration due to gravity by compound pendulum

If you would like to change your settings or withdraw consent at any time, the link to do so is in our privacy policy accessible from our home page.. The angle \(\theta\) describes the position of the pendulum. A string is attached to the CM of the rod and the system is hung from the ceiling (Figure \(\PageIndex{4}\)). The relative uncertainty on our measured value of \(g\) is \(4.9\)% and the relative difference with the accepted value of \(9.8\text{m/s}^{2}\) is \(22\)%, well above our relative uncertainty. 1 Objectives: The main objective of this experiment is to determine the acceleration due to gravity, g by observing the time period of an oscillating compound pendulum. Find more Mechanics Practical Files on this Link https://alllabexperiments.com/phy_pract_files/mech/, Watch this Experiment on YouTube https://www.youtube.com/watch?v=RVDTgyj3wfw, Watch the most important viva questions on Bar Pendulum https://www.youtube.com/watch?v=7vUer4JwC5w&t=3s, Please support us by donating, Have a good day, Finally found the solution of all my problems,the best website for copying lab experiments.thanks for help, Your email address will not be published. Which is a negotiable amount of error but it needs to be justified properly. The minus sign shows that the restoring torque acts in the opposite direction to increasing angular displacement. Therefore, the period of the torsional pendulum can be found using, \[T = 2 \pi \sqrt{\frac{I}{\kappa}} \ldotp \label{15.22}\]. Formula: This Link provides the handwritten practical file of the above mentioned experiment (with readings) in the readable pdf format. Several companies have developed physical pendulums that are placed on the top of the skyscrapers. The LibreTexts libraries arePowered by NICE CXone Expertand are supported by the Department of Education Open Textbook Pilot Project, the UC Davis Office of the Provost, the UC Davis Library, the California State University Affordable Learning Solutions Program, and Merlot. The minus sign indicates the torque acts in the opposite direction of the angular displacement: \[\begin{split} \tau & = -L (mg \sin \theta); \\ I \alpha & = -L (mg \sin \theta); \\ I \frac{d^{2} \theta}{dt^{2}} & = -L (mg \sin \theta); \\ mL^{2} \frac{d^{2} \theta}{dt^{2}} & = -L (mg \sin \theta); \\ \frac{d^{2} \theta}{dt^{2}} & = - \frac{g}{L} \sin \theta \ldotp \end{split}\]. Thus you get the value of g in your lab setup. We expect that we can measure the time for \(20\) oscillations with an uncertainty of \(0.5\text{s}\). To Find the Value of Acceleration Due to Gravity (g), Radius of All of our measured values were systematically lower than expected, as our measured periods were all systematically higher than the \(2.0\text{s}\) that we expected from our prediction. 16.4 The Simple Pendulum - College Physics 2e | OpenStax 4 0 obj The formula then gives g = 9.8110.015 m/s2. The length of the pendulum has a large effect on the time for a complete swing. /Contents 4 0 R %PDF-1.5 A simple pendulum is defined to have a point mass, also known as the pendulum bob, which is suspended from a string of length L with negligible mass (Figure \(\PageIndex{1}\)). >> /F2 9 0 R Rather than measure the distance between the two knife edges, it is easier to adjust them to a predetermined distance. Theory The period of a pendulum (T) is related to the length of the string of the pendulum (L) by the equation: T = 2 (L/g) Equipment/apparatus diagram 1 The only things that affect the period of a simple pendulum are its length and the acceleration due to gravity. Kater's pendulum - Amrita Vishwa Vidyapeetham The Kater's pendulum used in the instructional laboratories is diagramed below and its adjustments are described in the Setting It Up section. In the experiment the acceleration due to gravity was measured using the rigid pendulum method. Use a stopwatch to record the time for 10 complete oscillations. We suspect that by using \(20\) oscillations, the pendulum slowed down due to friction, and this resulted in a deviation from simple harmonic motion. Objective The solution to this differential equation involves advanced calculus, and is beyond the scope of this text. What should be the length of the beam? In the experiment, the bar was pivoted at a distanice of Sem from the centre of gravity. We are asked to find the length of the physical pendulum with a known mass. If this experiment could be redone, measuring \(10\) oscillations of the pendulum, rather than \(20\) oscillations, could provide a more precise value of \(g\). [] or not rated [], Copyright 2023 The President and Fellows of Harvard College, Harvard Natural Sciences Lecture Demonstrations, Newton's Second Law, Gravity and Friction Forces, Simple Harmonic (and non-harmonic) Motion. Newtonian MechanicsFluid MechanicsOscillations and WavesElectricity and MagnetismLight and OpticsQuantum Physics and RelativityThermal PhysicsCondensed MatterAstronomy and AstrophysicsGeophysicsChemical Behavior of MatterMathematical Topics, Size: from small [S] (benchtop) to extra large [XL] (most of the hall)Setup Time: <10 min [t], 10-15 min [t+], >15 min [t++]/span>Rating: from good [] to wow! How to Calculate an Acceleration Due to Gravity Using the Pendulum !Yh_HxT302v$l[qmbVt f;{{vrz/de>YqIl>;>_a2>&%dbgFE(4mw. This page titled 27.8: Sample lab report (Measuring g using a pendulum) is shared under a CC BY-SA license and was authored, remixed, and/or curated by Howard Martin revised by Alan Ng. This correspond to a relative difference of \(22\)% with the accepted value (\(9.8\text{m/s}^{2}\)), and our result is not consistent with the accepted value. The acceleration of gravity decreases as the observation point is taken deeper beneath the surface of the Earth, but it's not the location of the compound pendulum that's responsible for the decrease. 2 0 obj In this experiment the value of g, acceleration due gravity by means of compound pendulum is obtained and it is 988.384 cm per sec 2 with an error of 0.752%. PDF Acceleration due to gravity 'g' by Bar Pendulum - Home Page of Dr The solution is, \[\theta (t) = \Theta \cos (\omega t + \phi),\], where \(\Theta\) is the maximum angular displacement. /Parent 2 0 R Anupam M (NIT graduate) is the founder-blogger of this site. This experiment uses a uniform metallic bar with holes/slots cut down the middle at regular intervals. The bar was displaced by a small angle from its equilibrium position and released freely. 15.5: Pendulums - Physics LibreTexts 1 Pre-lab: A student should read the lab manual and have a clear idea about the objective, time frame, and outcomes of the lab. ], ICSE, CBSE class 9 physics problems from Simple Pendulum chapter with solution, How to Determine g in laboratory | Value of acceleration due to gravity -, Simple Harmonic Motion of a Simple Pendulum, velocity of the pendulum bob at the equilibrium position, Transfers between kinetic & potential energy in a simple pendulum, Numerical problem worksheet based on the time period of pendulum, Acceleration, velocity, and displacement of projectile at different points of its trajectory, Satellite & Circular Motion & understanding of Geostationary Satellite. We also found that our measurement of \(g\) had a much larger uncertainty (as determined from the spread in values that we obtained), compared to the \(1\)% relative uncertainty that we predicted. /F6 21 0 R /F7 24 0 R You can download the paper by clicking the button above. Two knife-edge pivot points and two adjustable masses are positioned on the rod so that the period of swing is the same from either edge. Using the small angle approximation gives an approximate solution for small angles, \[\frac{d^{2} \theta}{dt^{2}} = - \frac{g}{L} \theta \ldotp \label{15.17}\], Because this equation has the same form as the equation for SHM, the solution is easy to find. The bar can be hung from any one of these holes allowing us to change the location of the pivot. The restoring torque is supplied by the shearing of the string or wire. 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"zz:_Back_Matter" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()" }, [ "article:topic", "Pendulums", "authorname:openstax", "simple pendulum", "physical pendulum", "torsional pendulum", "license:ccby", "showtoc:no", "program:openstax", "licenseversion:40", "source@https://openstax.org/details/books/university-physics-volume-1" ], https://phys.libretexts.org/@app/auth/3/login?returnto=https%3A%2F%2Fphys.libretexts.org%2FBookshelves%2FUniversity_Physics%2FBook%253A_University_Physics_(OpenStax)%2FBook%253A_University_Physics_I_-_Mechanics_Sound_Oscillations_and_Waves_(OpenStax)%2F15%253A_Oscillations%2F15.05%253A_Pendulums, \( \newcommand{\vecs}[1]{\overset { \scriptstyle \rightharpoonup} {\mathbf{#1}}}\) \( \newcommand{\vecd}[1]{\overset{-\!-\!\rightharpoonup}{\vphantom{a}\smash{#1}}} \)\(\newcommand{\id}{\mathrm{id}}\) \( \newcommand{\Span}{\mathrm{span}}\) \( \newcommand{\kernel}{\mathrm{null}\,}\) \( \newcommand{\range}{\mathrm{range}\,}\) \( \newcommand{\RealPart}{\mathrm{Re}}\) \( \newcommand{\ImaginaryPart}{\mathrm{Im}}\) \( \newcommand{\Argument}{\mathrm{Arg}}\) \( \newcommand{\norm}[1]{\| #1 \|}\) \( \newcommand{\inner}[2]{\langle #1, #2 \rangle}\) \( \newcommand{\Span}{\mathrm{span}}\) \(\newcommand{\id}{\mathrm{id}}\) \( \newcommand{\Span}{\mathrm{span}}\) \( \newcommand{\kernel}{\mathrm{null}\,}\) \( \newcommand{\range}{\mathrm{range}\,}\) \( \newcommand{\RealPart}{\mathrm{Re}}\) \( \newcommand{\ImaginaryPart}{\mathrm{Im}}\) \( \newcommand{\Argument}{\mathrm{Arg}}\) \( \newcommand{\norm}[1]{\| #1 \|}\) \( \newcommand{\inner}[2]{\langle #1, #2 \rangle}\) \( \newcommand{\Span}{\mathrm{span}}\)\(\newcommand{\AA}{\unicode[.8,0]{x212B}}\), Example \(\PageIndex{1}\): Measuring Acceleration due to Gravity by the Period of a Pendulum, Example \(\PageIndex{2}\): Reducing the Swaying of a Skyscraper, Example \(\PageIndex{3}\): Measuring the Torsion Constant of a String, 15.4: Comparing Simple Harmonic Motion and Circular Motion, source@https://openstax.org/details/books/university-physics-volume-1, State the forces that act on a simple pendulum, Determine the angular frequency, frequency, and period of a simple pendulum in terms of the length of the pendulum and the acceleration due to gravity, Define the period for a physical pendulum, Define the period for a torsional pendulum, Square T = 2\(\pi \sqrt{\frac{L}{g}}\) and solve for g: $$g = 4 \pi^{2} \frac{L}{T^{2}} ldotp$$, Substitute known values into the new equation: $$g = 4 \pi^{2} \frac{0.75000\; m}{(1.7357\; s)^{2}} \ldotp$$, Calculate to find g: $$g = 9.8281\; m/s^{2} \ldotp$$, Use the parallel axis theorem to find the moment of inertia about the point of rotation: $$I = I_{CM} + \frac{L^{2}}{4} M = \frac{1}{12} ML^{2} + \frac{1}{4} ML^{2} = \frac{1}{3} ML^{2} \ldotp$$, The period of a physical pendulum has a period of T = 2\(\pi \sqrt{\frac{I}{mgL}}\).

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determination of acceleration due to gravity by compound pendulum