|
|
| Line 1: |
Line 1: |
| [[File:Mausefalle 300px.jpg|thumb|300px|A [[mousetrap]] powered by a helical torsion spring]]
| | This is what I would say the days of low-level linkbuilding were search engine marketing numbered. Try to negotiate the fees. The popular and well rated SEO company stands out from the crowd. And Sheffield United retake the lead against Aston Villa thanks to Ryan Flynn.<br><br>my blog ... [http://yellowpages.ny1.com/biz/orlando-seo-gaba-marketing-inc/orlando/fl/32801/65952817 online reputation mangement] |
| | |
| A '''torsion spring''' is a [[spring (device)|spring]] that works by [[Torsion (mechanics)|torsion]] or twisting; that is, a flexible [[Elasticity (physics)|elastic]] object that stores [[mechanical energy]] when it is twisted. When it is twisted, it exerts a force (actually [[torque]]) in the opposite direction, proportional to the amount (angle) it is twisted. There are two types. A '''torsion bar''' is a straight bar of metal or rubber that is subjected to twisting ([[shear stress]]) about its axis by torque applied at its ends. A more delicate form used in sensitive instruments, called a '''torsion fiber''' consists of a [[fiber]] of silk, glass, or [[Fused quartz|quartz]] under tension, that is twisted about its axis. The other type, a '''helical torsion spring''', is a metal rod or wire in the shape of a [[helix]] (coil) that is subjected to twisting about the axis of the coil by sideways forces ([[bending moment]]s) applied to its ends, twisting the coil tighter. This terminology can be confusing because in a helical torsion spring the forces acting on the wire are actually bending stresses, not [[Deformation (mechanics)|torsional]] (shear) stresses.<ref>{{Citation
| |
| |last=Shigley
| |
| |first=Joseph E.
| |
| |coauthors=Mischke, Charles R.; Budynas, Richard G.
| |
| |title=Mechanical Engineering Design
| |
| |publisher=McGraw Hill
| |
| |location=New York
| |
| |year=2003
| |
| |page=542|url=http://books.google.com/?id=j8xscqTxWUgC&pg=PA542
| |
| |isbn=0-07-292193-5}}</ref>
| |
| <ref>{{Citation
| |
| | last = Bandari
| |
| | first = V. B.
| |
| | authorlink =
| |
| | coauthors =
| |
| | title = Design of Machine Elements
| |
| | publisher = Tata McGraw-Hill
| |
| | year = 2007
| |
| | location =
| |
| | page = 429
| |
| | url = http://books.google.com/?id=f5Eit2FZe_cC&pg=PA429
| |
| | doi =
| |
| | isbn = 0-07-061141-6}}</ref>
| |
| | |
| ==Torsion coefficient==
| |
| As long as they are not twisted beyond their [[elastic limit]], torsion springs obey an angular form of [[Hooke's law]]:
| |
| | |
| :<math> \tau = -\kappa\theta\,</math>
| |
| | |
| where <math>\tau\,</math> is the torque exerted by the spring in [[newton (unit)|newton]]-meters, and <math>\theta\,</math> is the angle of twist from its equilibrium position in [[radian]]s. <math>\kappa\,</math> is a constant with units of newton-meters / radian, variously called the spring's '''torsion coefficient''', '''torsion elastic modulus''', '''rate''', or just '''spring constant''', equal to the change in torque required to twist the spring through an angle of 1 radian. It is analogous to the spring constant of a linear spring. The negative sign indicates that the direction of the torque is opposite to the direction of twist.
| |
| | |
| The energy ''U'', in [[joule]]s, stored in a torsion spring is:
| |
| | |
| :<math> U = \frac{1}{2}\kappa\theta^2</math>
| |
| | |
| ==Uses==
| |
| Some familiar examples of uses are the strong helical torsion springs that operate [[clothespin]]s and traditional springloaded-bar type [[mousetrap]]s. Other uses are in the large coiled torsion springs used to counterbalance the weight of [[garage door]]s, and a similar system is used to assist in opening the [[decklid|trunk (boot) cover]] on some [[sedan (car)|sedan]]s. Small coiled torsion springs are often used to operate pop-up doors found on small consumer goods like [[digital camera]]s and [[compact disc]] players. Other more specific uses:
| |
| | |
| *A ''[[torsion bar suspension]]'' is a thick steel torsion bar spring attached to the body of a vehicle at one end and to a lever arm which attaches to the axle of the wheel at the other. It absorbs road shocks as the wheel goes over bumps and rough road surfaces, cushioning the ride for the passengers. Torsion bar suspensions are used in many modern cars and trucks, as well as military vehicles.
| |
| | |
| *The ''[[sway bar]]'' used in many [[Suspension (vehicle)|vehicle suspension]] systems also uses the torsion spring principle.
| |
| | |
| *The ''torsion pendulum'' used in [[torsion pendulum clock]]s is a wheel-shaped weight suspended from its center by a wire torsion spring. The weight rotates about the axis of the spring, twisting it, instead of swinging like an ordinary [[pendulum]]. The force of the spring reverses the direction of rotation, so the wheel oscillates back and forth, driven at the top by the clock's gears.
| |
| | |
| *The ''torsion [[catapult]]'' or [[mangonel]] is a medieval [[siege engine]] invented by the ancient Greeks. It uses a torsion spring consisting of twisted ropes to swing an arm that throws a heavy missile at the enemy with great force.
| |
| | |
| *The ''[[balance spring]]'' or hairspring in mechanical [[watch]]es is a fine spiral-shaped torsion spring that pushes the [[balance wheel]] back toward its center position as it rotates back and forth. The balance wheel and spring function similarly to the torsion pendulum above in keeping time for the watch.
| |
| | |
| *The ''[[D'Arsonval movement]]'' used in mechanical pointer-type meters to measure electrical current is a type of torsion balance (see below). A coil of wire attached to the pointer twists in a magnetic field against the resistance of a torsion spring. Hooke's law ensures that the angle of the pointer is proportional to the current.
| |
| | |
| *A ''DMD'' or [[digital micromirror device]] chip is at the heart of many [[video projectors]]. It uses hundreds of thousands of tiny mirrors on tiny torsion springs fabricated on a silicon surface to reflect light onto the screen, forming the image.
| |
| | |
| ==Torsion balance==
| |
| [[File:Bcoulomb.png|thumb|right|Drawing of Coulomb's torsion balance. From Plate 13 of his 1785 memoir.]]
| |
| The '''torsion balance''', also called '''torsion pendulum''', is a scientific apparatus for measuring very weak forces, usually credited to [[Charles-Augustin de Coulomb]], who invented it in 1777, but independently invented by [[John Michell]] sometime before 1783.<ref>{{Citation|last1=McCormmach|first1=R.|last2=Jungnickel|first2=C.|title=Cavendish|year=1996|publisher=American Philosophical Society|url=http://books.google.com/?id=EUoLAAAAIAAJ|isbn=0-87169-220-1|pages=335–344}}</ref> Its most well-known uses were by Coulomb to measure the [[electrostatic force]] between charges to establish [[Coulomb's Law]], and by [[Henry Cavendish]] in 1798 in the [[Cavendish experiment]]<ref>{{Citation|last=Cavendish|first=H.|year=1798|chapter=Experiments to determine the Density of the Earth|editor-surname=MacKenzie|editor-first=A.S.|publication-date=1900|title=Scientific Memoirs, Vol.9: The Laws of Gravitation|url=http://books.google.com/books?id=O58mAAAAMAAJ|publisher=American Book Co.|pages=59–105}}</ref> to measure the gravitational force between two masses to calculate the density of the Earth, leading later to a value for the [[gravitational constant]].
| |
| | |
| The torsion balance consists of a bar suspended from its middle by a thin fiber. The fiber acts as a very weak torsion spring. If an unknown force is applied at right angles to the ends of the bar, the bar will rotate, twisting the fiber, until it reaches an equilibrium where the twisting force or torque of the fiber balances the applied force. Then the magnitude of the force is proportional to the angle of the bar. The sensitivity of the instrument comes from the weak spring constant of the fiber, so a very weak force causes a large rotation of the bar.
| |
| | |
| In Coulomb's experiment, the torsion balance was an insulating rod with a metal-coated ball attached to one end, suspended by a silk thread. The ball was charged with a known charge of static electricity, and a second charged ball of the same polarity was brought near it. The two charged balls repelled one another, twisting the fiber through a certain angle, which could be read from a scale on the instrument. By knowing how much force it took to twist the fiber through a given angle, Coulomb was able to calculate the force between the balls. Determining the force for different charges and different separations between the balls, he showed that it followed an inverse-square proportionality law, now known as [[Coulomb's law]].
| |
| | |
| To measure the unknown force, the [[Torsion spring#Torsion coefficient|spring constant]] of the torsion fiber must first be known. This is difficult to measure directly because of the smallness of the force. Cavendish accomplished this by a method widely used since: measuring the [[Resonance|resonant vibration period]] of the balance. If the free balance is twisted and released, it will oscillate slowly clockwise and counterclockwise as a [[harmonic oscillator]], at a frequency that depends on the moment of inertia of the beam and the elasticity of the fiber. Since the inertia of the beam can be found from its mass, the spring constant can be calculated.
| |
| | |
| Coulomb first developed the theory of torsion fibers and the torsion balance in his 1785 memoir, ''Recherches theoriques et experimentales sur la force de torsion et sur l'elasticite des fils de metal &c''. This led to its use in other scientific instruments, such as [[galvanometer]]s, and the [[Nichols radiometer]] which measured the [[radiation pressure]] of light. In the early 1900s gravitational torsion balances were used in petroleum prospecting. Today torsion balances are still used in physics experiments. In 1987, gravity researcher A.H. Cook wrote:
| |
| | |
| <blockquote>The most important advance in experiments on gravitation and other delicate measurements was the introduction of the torsion balance by Michell and its use by Cavendish. It has been the basis of all the most significant experiments on gravitation ever since.<ref>{{Citation|last=Cook|first=A.H.|chapter=Experiments in Gravitation|editor-surname=Hawking|editor-first=S.W. and Israel, W.|title=Three Hundred Years of Gravitation|publication-date=1987|publisher=Cambridge University Press|isbn=0-521-34312-7|page=52|year=1987}}</ref></blockquote>
| |
| | |
| ==Torsional harmonic oscillators==
| |
| '''For definition of terms see end of section'''
| |
| | |
| Torsion balances, torsion pendulums and balance wheels are examples of torsional harmonic oscillators that can oscillate with a rotational motion about the axis of the torsion spring, clockwise and counterclockwise, in [[Simple harmonic motion|harmonic motion]]. Their behavior is analogous to translational spring-mass oscillators (see [[Harmonic oscillator#Equivalent systems]]). The general equation of motion is:
| |
| | |
| :<math>I\frac{d^2\theta}{dt^2} + C\frac{d\theta}{dt} + \kappa\theta = \tau(t)</math>
| |
| | |
| If the damping is small, <math>C \ll \sqrt{\frac{\kappa}{I}}\,</math>, as is the case with torsion pendulums and balance wheels, the frequency of vibration is very near the [[Mechanical resonance|natural resonant frequency]] of the system:
| |
| | |
| :<math>f_n = \frac{\omega_n}{2\pi} = \frac{1}{2\pi}\sqrt{\frac{\kappa}{I}}\,</math>
| |
| | |
| Therefore, the period is represented by:
| |
| | |
| :<math>T_n = \frac{1}{f_n} = \frac{2\pi}{\omega_n} = 2\pi \sqrt{\frac{I}{\kappa}}\,</math>
| |
| | |
| The general solution in the case of no drive force (<math>\tau = 0\,</math>), called the transient solution, is:
| |
| | |
| :<math>\theta = Ae^{-\alpha t} \cos{(\omega t + \phi)}\,</math>
| |
| | |
| where:
| |
| | |
| ::<math>\alpha = C/2I\,</math>
| |
| ::<math>\omega = \sqrt{\omega_n^2 - \alpha^2} = \sqrt{\kappa/I - (C/2I)^2}\,</math>
| |
| | |
| ===Applications===
| |
| The balance wheel of a mechanical watch is a harmonic oscillator whose resonant frequency <math>f_n\,</math> sets the rate of the watch. The resonant frequency is regulated, first coarsely by adjusting <math>I\,</math> with weight screws set radially into the rim of the wheel, and then more finely by adjusting <math>\kappa\,</math> with a regulating lever that changes the length of the balance spring.
| |
| | |
| In a torsion balance the drive torque is constant and equal to the unknown force to be measured <math>F\,</math>, times the moment arm of the balance beam <math>L\,</math>, so <math>\tau(t) = FL\,</math>. When the oscillatory motion of the balance dies out, the deflection will be proportional to the force:
| |
| | |
| :<math>\theta = FL/\kappa\,</math>
| |
| | |
| To determine <math>F\,</math> it is necessary to find the torsion spring constant <math>\kappa\,</math>. If the damping is low, this can be obtained by measuring the natural resonant frequency of the balance, since the moment of inertia of the balance can usually be calculated from its geometry, so:
| |
| | |
| :<math>\kappa = (2\pi f_n)^2 I\,</math>
| |
| | |
| In measuring instruments, such as the D'Arsonval ammeter movement, it is often desired that the oscillatory motion die out quickly so the steady state result can be read off. This is accomplished by adding damping to the system, often by attaching a vane that rotates in a fluid such as air or water (this is why magnetic compasses are filled with fluid). The value of damping that causes the oscillatory motion to settle quickest is called the [[Damping|critical damping]] <math>C_c\,</math>:
| |
| | |
| :<math>C_c = 2 \sqrt{\kappa I}\,</math>
| |
| | |
| {| class="wikitable"
| |
| |+ Definition of terms
| |
| |-
| |
| ! Term
| |
| ! Unit
| |
| ! Definition
| |
| |-
| |
| |<math>\theta\,</math>
| |
| | rad
| |
| | Angle of deflection from rest position
| |
| |-
| |
| | <math>I\,</math>
| |
| | <math>\mathrm{kg\,m^2}\,</math>
| |
| | Moment of inertia
| |
| |-
| |
| | <math>C\,</math>
| |
| | <math>\mathrm{kg\,m^2\,s^{-1}\,{rad}^{-1}}\,</math>
| |
| | Rotational friction (damping)
| |
| |-
| |
| | <math>\kappa\,</math>
| |
| | <math>\mathrm{N\,m\,{rad}^{-1}}\,</math>
| |
| | Coefficient of torsion spring
| |
| |-
| |
| | <math>\tau\,</math>
| |
| | <math>\mathrm{N\,m}\,</math>
| |
| | Drive torque
| |
| |-
| |
| | <math>f_n\,</math>
| |
| | Hz
| |
| | Undamped (or natural) resonant frequency
| |
| |-
| |
| | <math>T_n\,</math>
| |
| | s
| |
| | Undamped (or natural) period of oscillation
| |
| |-
| |
| | <math>\omega_n\,</math>
| |
| | <math>\mathrm{rad\,s^{-1}}\,</math>
| |
| | Undamped resonant frequency in radians
| |
| |-
| |
| | <math>f\,</math>
| |
| | Hz
| |
| | Damped resonant frequency
| |
| |-
| |
| | <math>\omega\,</math>
| |
| | <math>\mathrm{rad\,s^{-1}}\,</math>
| |
| | Damped resonant frequency in radians
| |
| |-
| |
| | <math>\alpha\,</math>
| |
| | <math>\mathrm{s^{-1}}\,</math>
| |
| | Reciprocal of damping time constant
| |
| |-
| |
| | <math>\phi\,</math>
| |
| | rad
| |
| | Phase angle of oscillation
| |
| |-
| |
| | <math>L\,</math>
| |
| | m
| |
| | Distance from axis to where force is applied
| |
| |}
| |
| | |
| ==See also==
| |
| * [[Beam (structure)]]
| |
| | |
| ==References==
| |
| <references/>
| |
| | |
| ==Bibliography==
| |
| * {{Citation|last=Cavendish|first=H.|year=1798|chapter=Experiments to determine the Density of the Earth|editor-surname=MacKenzie|editor-first=A.S.|publication-date=1900|title=Scientific Memoirs, Vol.9: The Laws of Gravitation|url=http://books.google.com/books?id=O58mAAAAMAAJ|publisher=American Book Co.|pages=59–105}}
| |
| * {{Citation|last1=McCormmach|first1=R.|last2=Jungnickel|first2=C.|title=Cavendish|year=1996|publisher=American Philosophical Society|url=http://books.google.com/?id=EUoLAAAAIAAJ|isbn=0-87169-220-1|pages=335–344}}
| |
| * {{Citation|last=Gray|first=Andrew|title=The Theory and Practice of Absolute Measurements in Electricity and Magnetism, Vol.1|year=1888|publisher=McMillan|url=http://www.engineersedge.com/spring_torsion_calc.htm|pages=254–260}}. Detailed account of Coulomb's experiment.
| |
| * {{Citation|title=Charles Augustin de Coulomb biography, Chemistry Dept.|publisher=Hebrew Univ. of Jerusalem|url=http://www.geocities.com/bioelectrochemistry/coulomb.htm|accessdate=August 2, 2007|archiveurl=http://web.archive.org/web/20090806115212/http://geocities.com/bioelectrochemistry/coulomb.htm|archivedate=2009-08-06}}. Shows pictures of the Coulomb torsion balance, and describes Coulomb's contributions to torsion technology.
| |
| * {{Citation|last1=Nichols|first1=E.F.|last2=Hull|first2=G.F|title=The Pressure due to Radiation|date=June 1903|journal=The Astrophysical Journal|volume=17|issue=5|pages=315–351|url=http://books.google.com/?id=8n8OAAAAIAAJ&pg=RA5-PA315|doi=10.1086/141035|bibcode=1903ApJ....17..315N}}. Describes the Nichols radiometer.
| |
| * {{Citation|url=http://www.mssu.edu/seg-vm/pict0349.html|title=Torsion balance, Virtual Geoscience Center|publisher=Society of Exploration Geophysicists|accessdate=2007-08-04}}. Description of how torsion balances were used in petroleum prospecting, with pictures of a 1902 instrument.
| |
| * {{Citation|title=Charles Augustin de Coulomb|encyclopedia=Encyclopaedia Britannica, 9th Ed.|page=452|year=1907|publisher=Werner Co.|volume=6|url=http://books.google.com/?id=IAwEAAAAYAAJ&pg=PA452}}
| |
| | |
| ==External links==
| |
| [[File:Torsion-pendulum.ogg|thumb|Video of a model torsion pendulum oscillating]]
| |
| * [http://www.magnet.fsu.edu/education/tutorials/java/torsionbalance/index.html Torsion balance interactive java tutorial]
| |
| * [http://www.engineersedge.com/spring_torsion_calc.htm Torsion spring calculator]
| |
| * [http://lheawww.gsfc.nasa.gov/~merk/G/Big_G.html Big G measurement, description of 1999 Cavendish experiment at Univ. of Washington, showing torsion balance]
| |
| * [http://www.npl.washington.edu/eotwash/experiments/experiments.html Four torsion balances used in contemporary physics experiments]
| |
| * [http://www.mssu.edu/seg-vm/pict0349.html How torsion balances were used in petroleum prospecting]
| |
| * [http://www.spring-makers-resource.net/torsion-springs.html Mechanics of torsion springs]
| |
| * [http://www.mathalino.com/reviewer/mechanics-and-strength-of-materials/helical-springs Solved mechanics problems involving springs (springs in series and in parallel)]
| |
| | |
| [[Category:Springs (mechanical)]]
| |
| [[Category:Pendulums]]
| |
| [[Category:Articles containing video clips]]
| |
| | |
| [[uk:Торсіон]]
| |