Damped Oscillations:
The amplitude of oscillations of, for instance, a simple pendulum, slowly decreases to zero over time because of resistive force arising from surrounding air in this case. In other forms of s. h. m. it will occur from surrounding medium (like liquid or gas). Motion for such oscillations is not thus a perfect s. h. m. It is said to be damped by air resistance, i.e., there is stable loss of energy as energy is converted to other forms. Generally it will be internal energy through friction but energy may also be radiated away. For instance, a vibrating turning fork loses energy by sound radiation.
The behavior of the mechanical system depends on extent of damping. For instance, mass hanging from the coiled spring and immersed in the liquid when set to vibrate, goes through more damping than when it is in air. Know that undamped oscillations are said to be free. When vibrating system is greatly damped, no oscillations take place. System just slowly returns to its equilibrium position. Now, when time taken for displacement to be zero is extremely small, vibrating system is said to be significantly damped.
When damping forces are proportional to velocity, v, period remain constant as amplitude diminishes and oscillator is said to be isochronous. It will interest you to know that motion of some devices is decisively damped on reason to get the certain desired objective. For instance, shock absorbers on the car vitally damp suspension of vehicle and hence resist the setting up of vibration that could make control difficult or cause damage. In shock absorber the motion of suspension up or down is opposed by viscous forces when liquid passes through transfer tube from one side of piston to the other. Instruments like balances and electrical meters are vitally damped so that pointer moves quickly to the correct position without oscillating. Damping is frequently produced by electro-magnetic forces.
Forced Oscillation and Resonance:
Barton's Pendulums:
A number of paper coned pendulums of length varying from 1/4 m to 3/4 m, each loaded with the plastic curtain ring are suspended from same string as the driver pendulum that has heavy bob and a length of 1/2 m.
When driver pendulum is pulled well aside and then released, it oscillates in the plane perpendicular to plane of the diagram. After a short time, motion settles down and all the other pendulums oscillate with extremely almost same frequency as that of the driver although with different amplitudes. This is the example of forced oscillation. Out of the set of pendulums, one whose length equals that of driver pendulum has greatest amplitude of vibration. Therefore, its natural frequency of oscillation is same as the frequency of driving pendulum. This is the example of resonance and driving oscillator passes on its energy most easily to other system, i.e., proper cone pendulum of the same length. Therefore, when rings on paper cone pendulums are removed, their masses decrease and so damping increases. All amplitudes are then found to be reduced and that of resonance frequency being less pronounced.
Energy Considerations:
Whether or not a body is at or close to resonance, oscillator settles down in the steady state where energy supplied from driver per cycle is equal to energy dissipated per cycle. Sharpness of resonance, known as Q-factor is equal to:
= energy lost per cycle/energy at the start of the cycle
It is also provided by
Q = f0/Δf
Where Δf is the width of the resonance curve
When
x = xmax/√2
Xmax being maximum value of displacement x and where fo is the resonant frequency.
Phase:
At resonance, an oscillator lags behind the driver by 90o i.e. it is 90o out of phase with driver. When driver is at a much lower frequency than oscillator's natural frequency (fd < fN) oscillator is in step with driver. When driver frequency is much higher than natural frequency (fd > fN), driver and oscillator are 180o out of phase.
S. H. M. - A Mathematical Model:
S. h. m. is entirely an idealized situation which doesn't exist in nature or in practical world. Real oscillators like a motor cycle on its suspension, tall chimney swaying in wind, atoms or ions vibrating in the crystal etc only estimated to ideal kind of motion we call s.h.m. Simple harmonic motion is the mathematical model, helpful because it represents several real oscillations because of its simplicity. It doesn't have complications like damping, variable mass and stiffer (elastic modulus). Only condition it (s. h. m.) has to satisfy is that restoring force must be directed towards centre of motion and be proportional to displacement.
The more complex model might, for instance, take damping into consideration and therefore may be the better explanation of the particular oscillator. Such may perhaps not be extensively appropriate. Conversely, if the model is very simple, it may be of little use for dealing with actual systems. Therefore, a model should have just right degree of complexity. Mathematical s. h. m. has this and so is useful in practice.
Physical Pendulum:
It is not always that pendulum comprises of the massless string with the pointlike mass at the end of it. Sometimes a pendulum can comprise of the suspended swinging object of some form. We call this physical pendulum. Any object can be suspended from any point on object and serve as physical pendulum. This shows fact that s. h. m. is the general feature of motion about the stable equilibrium. You can even set up the physical pendulum, with measuring ruler in the room.
Therefore, the so-called physical pendulum is any real pendulum in which all mass is taken to be concentrated at the point. If a body with irregular shape pivoted about the horizontal frictionless axis O and displaced from vertical by an angle Θ. Distance from pivot to centre of gravity is h, the moment of inertia of pendulum about the axis through pivot is I and the mass of pendulum is m. Weight mg causes the restoring torque τ of value provided by
τ = - mgh sinΘ
When released, body oscillates about the equilibrium position. Note that, unlike s.h.m., motion of the physical pendulum is not simple harmonic as the torque τ is proportional not to Θ but to sin Θ. Though, if Θ is small, we can again estimate sin Θ by Θ so that motion becomes approximately harmonic.
Suppose this approximation then,
τ = (mgh)Θ
Effective torque constant is
K1 = -τ/Θ = mgh
Therefore, period of physical pendulum is
T = 2Π√I/K1 = 2Π√I/mgh
Tutorsglobe: A way to secure high grade in your curriculum (Online Tutoring)
Expand your confidence, grow study skills and improve your grades.
Since 2009, Tutorsglobe has proactively helped millions of students to get better grades in school, college or university and score well in competitive tests with live, one-on-one online tutoring.
Using an advanced developed tutoring system providing little or no wait time, the students are connected on-demand with a tutor at www.tutorsglobe.com. Students work one-on-one, in real-time with a tutor, communicating and studying using a virtual whiteboard technology. Scientific and mathematical notation, symbols, geometric figures, graphing and freehand drawing can be rendered quickly and easily in the advanced whiteboard.
Free to know our price and packages for online physics tutoring. Chat with us or submit request at [email protected]
a single transistor (BF 194) is employed. This stage contains local oscillator and mixer. The antenna coil is connected in the input section (Base) and IF transformer is connected in the output section (Collector).
Greek Art Assignment Help is the one stop destination - provides HD quality solutions with timely delivery at best prices.
www.tutorsglobe.com offers elements of the analysis model homework help, assignment help, case study, writing homework help, online tutoring assistance by computer science tutors.
Theory and lecture notes of single population variance all along with the key concepts of Testing a single population variance, Conditions for testing and Confidence Intervals. Tutorsglobe offers homework help, assignment help and tutor’s assistance on single population variance.
tutorsglobe.com balanced diet assignment help-homework help by online nutrition tutors
tutorsglobe.com melanin-functions assignment help-homework help by online skin tutors
online taks-teks exam preparation course and online taks-teks tutoring package offered by tutorsglobe are the most comprehensive and customized collection of study resources on the web, offering best collection of taks-teks practice papers, quizzes, taks-teks test papers, and guidance.
tutorsglobe.com monetary transmission assignment help-homework help by online monetary policy tutors
tutorsglobe.com fatty acids assignment help-homework help by online lipid metabolism tutors
Avail the most prominent Industrial Microbiology Assignment Help from top-rated experts and earn top grades at reasonable prices.
www.tutorsglobe.com offers free tutorial on determining price rigidity, answering questions based on price rigidity, oligopoly assignment help- homework help.
introduction to photochemistry tutorial all along with the key concepts of light-matter, absorption of light by atoms and molecules, photochemistry, basic laws of photochemistry, reaction pathways, applications of photochemistry, photochemistry induced by visible-ultraviolet light
Approach the trusted Computational Geometry Assignment Help tutors and get top-notch solutions with 24x7 support and secure high grades.
TutorsGlobe.com Elementary Units in Chemical Reactions Assignment Help-Homework Help by Online Access Chemistry Tutors
Theory and lecture notes of Least Squares Fitting-Noisy Data all along with the key concepts of functions and data, Traffic flow model, Linear least squares, Drag coefficients. Tutorsglobe offers homework help, assignment help and tutor’s assistance on Least Squares Fitting-Noisy Data.
1946599
Questions Asked
3689
Tutors
1492937
Questions Answered
Start Excelling in your courses, Ask an Expert and get answers for your homework and assignments!!