...Title: How different springs behave under the influence of same mass depending on the spring constant (k) and connection types (parallel or series)? Summary: This experiment will be carried out to investigate spring constants of different springs by measuring the length of springs under the influence of same mass and different masses, and observe how overall spring constant changes depending on connection types of springs by measuring amount of extension when springs are connected in series and parallel. Different springs with different constant, different masses, weighing machine and a measuring ruler will be used. Research: The course textbook and different textbooks (S.Beichner, Fizik1, Ankara: Palme Yayınevi, 2002.), some laboratory experiments, which retrieved from the Internet, some lectures and videos comprise sources for the theoretical analysis of the experiment. -Prof. Walter Lewin (1999), Hooke's Law, Simple Harmonic Oscillator (online) (http://ocw.mit.edu/courses/physics/8-01-physics-i-classical-mechanics-fall-1999/video-lectures/lecture-10), -Combination of springs (online) (http://engineeronadisk.com/V2/book_modelling/engineeronadisk-10.html) -Sal Khan (2008), Intro to springs and Hooke's Law (online) (http://www.youtube.com/watch?v=ZzwuHS9ldbY) -Forces and elasticity (online) (http://www.bbc.co.uk/schools/gcsebitesize/science/add_aqa/forces/forceselasticityrev2.shtml) -Deformation of materials (online) (http://qatemplates.everythingscience.co.z...
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...pulley system using the Atwood’s machine and using springs (2) in series and parallel to determine their spring constants and extensions when a mass is hanged from them. Newron’s second law states that the force on an object is directly proportional to the rate of change of momentum, which later gives the formula F =ma , m= mass and a is acceleration. Newton;s third law suggests that every action occurring on an object has an equal and opposite reaction when they occur in pairs, are acting in opposite directions and has same magnitude. In part one, we measure the acceleration of the mass pulley system using the photo gate. Data M1 = 151.25 g M2 =171.25 g Mean acceleration = 0.5992 m/s^2 Standard deviation 0.05463 Data Analysis Part 1 (Atwood’s Machine) – Formula and calculation of theoretical acceleration (ath) – A =(m1-m2)/(m1+m2) * g , ath= (0.17125-0.15125)/( 0.17125+0.15125)* 9.79 = 0.6083 m/s^2 % error = 0.05463/0.5592 *100 =9.76 % Formula and calculation of percent difference between ae and ath – % difference = (difference / A_th) *100 = (0.55992-0.6083) /0.6083 *100 =8.01% Part 2 (Springs in Series) – Hooke’s law equation – F = -Kx Calculation of spring constants, k1 and k2 using Hooke’s law equation – k1 = mg/ x = (2.75)/0.052 =52.9 k2 = mg/ x = (7.73)/ 0.058 = 90.9 Calculation of experimental keff for series combinations of springs – K eff = Fs / del(xs ) K = F/x =10.31...
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...in the springs once weight has been applied relating to Hooke’s Law. Key Results: When adding more force to the springs, the springs stretch further to the ground, then bounce further upward when released. The more force applied the more the restoring force will be. The restoring force is in the opposite direction from the displacement of the spring. The restoring force and the displacement depend on how hard or soft the spring is. The harder the spring the more difficult it is to stretch or bounce. The softer the spring the easier it is to stretch or bounce. The k of Spring 1 is 30 cm. When 50 grams were added the measurement dropped to about 35 cm when the spring stopped moving. When 100 grams were added the measurement dropped to 40 cm. When 250 grams were added the measurement dropped to 55 cm. The Effects of Mass: The larger the mass the longer the spring. To determine this effect I started by adding the smaller mass to the first spring and watched until it stopped its movement. I then proceeded with the same procedure with the medium mass, then finished with the larger mass. The Effects of Gravity: To determine the effects of gravity I first set the friction and softness back to the constant levels. When there was no gravity the springs were all at the constant level as if nothing were hanging on the springs at all. As the gravity increases the further the springs would stretch depending on the mass. When changed to the Moon the springs stretched...
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...laboratory in Physics I, student explored the motions of a mass on a spring. More specifically students looked at oscillations (periods) with various masses. Students set a spring into vertical oscillations with suspended masses and measured the period of oscillation. Using this method, students found a spring constant of 30.30N/m. Results should have verified that the period of oscillation depended on the effective mass of the spring and the period of oscillation. Students recorded basic information such as the position of the mass before the spring is charged, the path of the mass, the peak of the oscillation, as well as the force the mass and the spring exert on each other. Data studio and a force sensor, and a position sensor was used to get accurate measurements of these values. Goal The purpose of this laboratory is to characterize the oscillation of a simple spring-mass system. Theory If a spring is stretched or compressed a small distance from its equilibrium position, the spring will exert a force on the body given by Hooke's Law, where is known as the spring force. The constant, , known as the spring constant, and is the displacement from the equilibrium position. The spring constant is a clue of the spring's strength. A large value for indicates that the spring is strong or stiff. A low value for means the spring is weak or flexible. Springs with large values can balance larger forces than springs with low values. The negative sign in indicates that the...
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...Front Cover The Vibrating Spring - Experiment #02 Many objects in the real world have a frequency at which they vibrate. In modern engineering it is required to take this into consideration when designing them. There are many variables which could affect this frequency, therefore test are required to be conducted to see what these variables are and how they affect the vibrations the object undergoes. A vibration occurs when there is an oscillation about an equilibrium point. A good example for where oscillations occur is in a car’s suspension. The suspension takes a hit when a car goes over a bump or into a pothole. The springs in the suspension then oscillate and make the car “bounce” up and down. This is when the shock-absorbers kick in and damp the oscillations to make the car level again. The variables that could change the oscillations which the suspension undergoes could be the diameter of the springs or the number of coils. This would have been tested when the suspension was designed to make sure the car is safe and comfortable for the driver. The picture on the right shows a typical suspension that would be installed on a car. The coils can be clearly seen in the picture as well as the shock absorber in the centre which damps the oscillations. In the experiment which has been conducted here the vibrations of certain springs have been observed to see what variables affect the frequency at which they oscillate. The relationships between these variables and their...
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...Simple Harmonic Motion Aston University Engineering and Applied Science – Physics Lab Report 01/11/2014 Determination by simple harmonic motion of the acceleration due to gravity Introduction: A system undertaking simple harmonic motion (SHM) can be restrained very accurately. The period of the SHM depends both on the mass of the system and the strength of the force tending to restore the system to its equilibrium state). Oscillations are a common part of life, for instance the vibrations of a musical instrument which helps make sounds or the foundations of a car suspension which are assisted by oscillations. The main aims of this experiment was to determine if the oscillation of a mass which hung vertically from a spring; this oscillating system was used to measure the acceleration of earth due to gravity and to determine the accuracy of experimental results precisely. (http://www.pgccphy.net/1020/phy1020.pdf Theory: | | | Acceleration due to gravity The value of 9.8m/s/s acceleration is given to a free falling object, directing downwards towards Earth. Any object moving solely under the influence of gravity is known as acceleration of gravity and this vital quantity is denoted by Physicians as the symbol g. (http://www.physicsclassroom.com/class/1DKin/Lesson-5/Acceleration-of-Gravity) Simple harmonic motion This is everyplace where the acceleration is proportional and opposite to displacement to the continuous amplitude from the position...
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...earlier results. This shows that period of oscillations can be determined by length and gravitational acceleration, and doesn’t depend on mass. In our other activity, we measured the period of an oscillating mass connected to a spring. We had a hanging spring, and hung mass to the bottom of it, each time measuring the change in length of the spring from the time before. To find the spring constant, we used the masses added to calculate each of their elastic forces, by multiplying each by gravitational acceleration, then plotting them with their corresponding spring deformation, and the slope of that graph was the spring constant, k, which was 8.22 N/m. Using this value, we calculated the period of motion for the mass of 0.1 kg using a different given equation than the one before, obtaining a period of 0.69 seconds. To verify our results, we used the VideoCom to graph the spring as we placed 0.1 kg on it and then bounced it, then calculated a period from position, velocity, and acceleration vs time graphs by finding the distance between two peaks. With an average of these three periods of 0.86 seconds, we found our results were correct in calculating by hand the period of motion. This proved that if one knows the spring constant and mass of an...
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...scanning tunneling microscope is proposed as a method to measure forces as small as 10 N. As one application for this concept, we introduce a new type of microscope capable of investigating surfaces of insulators on an atomic scale. The atomic force microscope is a combination of the principles of the scanning tunneling microscope and the stylus profilometer. It incorporates a does not damage the surface. Our preliminary results in air demonstrate a lateral resoluprobe that 0 0 tion of 30 A and a vertical resolution less than 1 A. PACS numbers: 68.35.Gy %e are concerned in this paper with the measurement of ultrasmall forces on particles as small as single atoms. %e propose to do this by monitoring the elastic deformation of various types of springs with the scanning tunneling microscope (STM). ' It has been a common practice to use the displacement of springs as a measure of force, and previous methods have relied on electrostatic fields, magnetostatic fields, optical waves, and x rays. Jones~ has reviewed the devices that use variable capacitances and he reports that displacements of 10 4 A can be measured. SQUIDs3 are superconducting elements that measure the expulsion of magnetic fields in variable-inductance devices. They are used in gravity gradiometers to measure displacements of 10 6 A. Tabor and co-workers in their work with van der Waals forces have used optical interference methods to measure displacements of 1 A. With an x-ray interferometer...
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...Experimental design and procedure pg.4 Analysis result and conclusion pg.7 Reflection to other experiment pg.9 Introduction The purpose of this dynamic Lab is to measure the stiffness and resonant frequencies of a coupled oscillator on an air track. Four experiments will be taken in order to see the behaviour and performance of the rubbers connecting the trolleys. Calculate theoretical results by using background information. Comparisons of theoretical and experimental results will be done to see errors and find conclusions. Resonant frequencies are the frequencies that a system oscillates at greater amplitudes. This type of oscillations is what makes systems to vibrate many times. On the other hand, stiffness is a measurement of the ability a material have to extend without deformation. Low stiffness can result in failure of a system and high stiffness is required in the design of systems that deformation should be at its minimum. So both two factors are important in the performance of a system, in order to perform efficiently and without any failure. Theoretical calculations and background information A system working at resonant frequencies means that the amplitude of oscillations is high. This mainly is a disadvantage for a system. However these “disadvantages” can be used in...
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...the relationship between frequencies, wave length and wave velocity of a transverse wave on a string, as well as the relationship between the spring tension and the number of standing waves formed. Two different strings used in this experiment are white and black in colour; the µ1 value calculated for the white string is 2.73 x 10-3 ±0.00055kg/m with an uncertainty of ±8.2932 x 10-5 kg/m while the µ2 value calculated for the black string is 1.38 x 10-3 kg/m with an uncertainty of ±8.6492 x 10-5 kg/m. However, the actual linear mass density µ0 of the white spring calculated is 2.87x10-3kg/m; compared to the experimental linear mass density µ1, the difference in error was 4.88%, however, the mass of the black spring was too small to be weighted therefore the actual linear mass density µ0 was unable to be calculated, so cannot be compared to the experimental linear mass density µ2. Introduction: A wave can be described as a disturbance that carries energy and travels through a medium form one location to another. Waves can be classified into two types, transverse waves and longitudinal waves. This experiment was based on transverse wave and can be described by the position of the particles at a particular time as well as how the position changes with time. Transverse wave can also be considered as a wave that remains at constant position. Wave produced by a vibrator travels down a string and reflects back along the string on reaching the fixed end of string, and a wave...
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...To calculate the Time Constant we use T = RC To calculate the Time Constant we use T = RC Example of circuit used for testing capacitor charge and discharge. Example of circuit used for testing capacitor charge and discharge. Capacitors discharge exponentially, the rate of discharge is known as the time constant Capacitors discharge exponentially, the rate of discharge is known as the time constant We can also use similar equations to calculate the Voltage or Current at any point We can also use similar equations to calculate the Voltage or Current at any point When the equation is compared with y =mx+c m = 1/RC & C = ln Io When the equation is compared with y =mx+c m = 1/RC & C = ln Io To calculate the charge left on a capacitor at any point we use this equation. To calculate the charge left on a capacitor at any point we use this equation. Capacitor Discharge Capacitor Discharge When the switch is at A the capacitor charges exponentially up to a point where the capacitor cannot hold anymore electrons When the switch is at A the capacitor charges exponentially up to a point where the capacitor cannot hold anymore electrons When 2 Pendulums are suspended from the same piece of string when one pendulum is displaced it can transfer energy to the other pendulum causing it to swing When 2 Pendulums are suspended from the same piece of string when one pendulum is displaced it can transfer energy to the other pendulum...
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...[pic] Internal Assessment Resource Physics Level 3 |This resource supports assessment against: | |Achievement Standard 91521 | |Carry out a practical investigation to test a physics theory relating two variables in a non-linear relationship | |Resource title: Baby bouncer | |4 credits | |This resource: | |Clarifies the requirements of the Standard | |Supports good assessment practice | |Should be subjected to the school’s usual assessment quality assurance process | |Should be modified to make the context relevant to students in their school environment and ensure that submitted | |evidence is authentic | |Date version published by Ministry of |December 2012 ...
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...sport of boxing. This fascination led me to explore what occurs to a human head upon impact from a boxer’s punch. It is known that a knockout occurs when blood circulation to the brain is compressed. This compression results from the sudden acceleration and deceleration of the head[1]. Therefore, the primary focus of this experiment explores the relative effort necessary to cause significant movement to a head about a neck. Figure 1 - Picture of modeled head and spine secured to a table ! To achieve this, a simplistic mechanical model of a human head, a socket, and a spine was built. A volleyball was used to simulate a head. A garage door spring with a diameter of 4.0 ± .05cm was used as a spine. Lastly, a small wooden block acted as a socket between the head and the spine. A small support board held the spring in place for the experiment and allowed it to be moved up or down to simulate different neck lengths. Wearing a standard 14oz boxing glove, I punched the model and recorded the subsequent motion utilizing a Fujiyama high speed camera at 240 frames per second (fps). This function of the camera...
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...Cesare Masin University of Padua, Italy Participants estimated the imagined elongation of a spring while they were imagining that a load was stretching the spring. This elongation turned out to be a multiplicative function of spring length and load weight—a cognitive law analogous to Hooke’s law of elasticity. Participants also estimated the total imagined elongation of springs joined either in series or in parallel. This total elongation was longer for serial than for parallel springs, and increased proportionally to the number of serial springs and inversely proportionally to the number of parallel springs. The results suggest that participants integrated load weight with imagined elasticity rather than with spring length. Intuitive physics refers to the cognitive laws of our tacit knowledge of the ordinary physical world (Anderson, 1983; Lipmann & Bogen, 1923; McCloskey, 1983; Shanon, 1976; Smith & Casati, 1994; Wilkening & Huber, 2002). In the following we report an investigation of the intuitive physics related to Hooke’s law of linear elasticity. We begin with a description of this law. HOOKE’S LAW Consider a close-coiled helical spring with length L and external diameter D, suspended from a fixed support. After an object with weight W is suspended from the lower end of the spring, Hooke’s law says that the spring elongation (increment in L) is E = k0 + k · W (1) with k0 a measurement error and k a parameter expressing the elasticity of * Acknowledgment: we would wish to...
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...Procedure: Note: The Force Probe is attached to a cart. 1. Zero the Force Probe. (With nothing attached to the Probe press "Start" on the control panel and observe the force. If it is not zero press the small button "TARE" on the side of the Sensor and confirm that the force measurement is now zero. If the Force Probe still registers a nonzero force contact your instructor.) 2. Measure the unstretched length of one rubber band and record here: Lo=________ 3. Place one end of the rubber band around the vertical rod on the stand. 4. Attach the Force Probe hook to the free end of the rubber band. See Figure 1A on the next page. [pic] Figure 1A 5. Click "Start" and pull the Force Probe horizontally to stretch the rubber band 10cm (10cm beyond the unstretched length). See Figure 1B below. [pic] Figure 1B 6. Select the statistics feature [pic] and determine the mean value of the force. Record the force in Newtons. _______N 7. Now stretch the rubber band 20cm. Record the force._________N 8. Now stretch the rubber band 30cm. Record the force._________N 1. Now stretch the rubber band 40cm. Record the force._________N 2. Record your measurements in Data Table 1. [pic] 9. Remove the Force Probe and zero it again. 10. Place a second...
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