Difference between revisions of "Spring (device)" - New World Encyclopedia

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{{otheruses|Spring}}
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[[Image:Springs 009.jpg|thumb|right|250px|[[Helix|Helical]] or ''coil'' springs designed for tension.]]
[[Image:Springs 009.jpg|thumb|right|250px|[[Helix|Helical]] or ''coil'' springs designed for tension]]
 
  
A '''spring''' is a flexible [[elasticity|elastic]] object used to store mechanical [[energy]]. Springs are usually made out of [[hardened steel]]. Small springs can be wound from pre-hardened stock, while larger ones are made from [[annealing (metallurgy)|annealed]] steel and hardened after fabrication. Some [[ferrous and non-ferrous metals|non-ferrous metals]] are also used including [[phosphor bronze]] for parts requiring corrosion resistance and [[beryllium copper]] for springs carrying electrical current (because of its low electrical resistance).  
+
A '''spring''' is a flexible, [[elasticity|elastic]] device used to store mechanical [[energy]]. When a force is applied to a spring, it expands or contracts to a certain extent, and when the force is released, the spring attempts to return to its earlier state.
  
==Types==
+
Springs can be made of a variety of elastic materials, including fluids, but springs used in mechanical devices are generally made of metal. They also vary in shape; familiar shapes being helical, spiral, and flat.
[[Image:Montre Tribaudeau Besancon 01.jpg|thumb|right|250px|A spiral spring]]
+
{{toc}}
[[Image:volute_spring.jpg|thumb|right|250px|A volute spring. Under compression the coils slide over each other, so affording longer travel.]]
+
Based on their behavior, springs are used to move objects, absorb vibrations, and control mechanical shock. For instance, they are useful in clocks, shock absorbers, motorized toys, pogo sticks, [[automobile]] engine valves, and door-closing mechanisms. Technically, a wooden [[Bow (weapon)|bow]] is a form of spring.
The most common types of spring are:
+
 
 +
==Historical appearance==
 +
 
 +
Simple, non-coiled springs, such as the [[Bow (weapon)|bow]] (used with an arrow), have been used through much of human history. In the Bronze Age, more sophisticated spring devices were used, as indicated by the spread of tweezers in many cultures. [[Ctesibius of Alexandria]] developed a method for making [[bronze]] with spring-like characteristics by producing an alloy of bronze with an increased proportion of tin, then hardening it by hammering after it was cast.
 +
 
 +
[[Coiled springs]] appeared early in the fifteenth century,<ref>[http://www.madehow.com/Volume-6/Springs.html Springs] How Products Are Made. Retrieved April 3, 2010.</ref> leading to the development of the first spring-powered clocks in that century.<ref>White Jr., Lynn, ''Medieval Technology and Social Change''. (New York: Oxford Univ. Press, 1966, p. 126-127. ISBN 0195002660).</ref><ref>Usher, Abbott Payson, ''[http://books.google.com/books?id=xuDDqqa8FlwC&pg=PA305&sig=_SRpwfz0YBAjt2aGxXhmRkZ16GQ A History of Mechanical Inventions]'' (New York: Dover, 1988, p. 305. ISBN 048625593X). Retrieved April 3, 2010.</ref><ref>Dohrn-van Rossum, Gerhard, ''[http://books.google.com/books?id=53K32RiEigMC&pg=PA121&sig=5huN81ukYRbSlxq4MsToTDIXYDY History of the Hour: Clocks and Modern Temporal Orders]''. (Chicago: Univ. of Chicago Press, 1997, p. 121. ISBN 0226155102). Retrieved April 3, 2010.</ref> By the sixteenth century, the first large, spring-powered watches were produced.
  
*[[Coil spring]] or [[helix|helical]] spring - a spring (made by winding a wire around a cylinder) and the [[Cone (geometry)|conical]] spring - these are types of [[torsion spring]], because the wire itself is twisted when the spring is compressed or stretched. These are in turn of two types:
+
== Materials used for springs ==
**''Tension springs'' are designed to become longer under load. Their turns are normally touching in the unloaded position, and they have a hook, eye or some other means of attachment at each end.
 
**''Compression springs'' are designed to become shorter when loaded. Their turns are not touching in the unloaded position, and they need no attachment points. A ''[[volute]]'' spring is a compression spring in the form of a cone so that under compaction the coils are not forced against each other, thus permitting longer travel.
 
  
*[[Leaf spring]] - a flat springy sheet, used in vehicle [[suspension (vehicle)|suspension]]s. electrical [[switch]]es, [[bow (weapon)|bow]]s.
+
As noted above, various elastic materials can be used to make springs. Even fluids under pressure demonstrate spring-like properties. Most springs, however, are made of metal, particularly [[hardened steel]]. Small springs can be wound from pre-hardened stock, while larger ones are made from [[annealing (metallurgy)|annealed]] steel and hardened after fabrication. Some [[ferrous and non-ferrous metals|non-ferrous metals]] are also used, including [[phosphor bronze]] for parts requiring corrosion resistance, and [[beryllium copper]] for springs carrying electrical current (because its electrical resistance is low).
  
* [[V-spring]] - used in antique [[firearm]] mechanisms such as the [[wheellock]], [[flintlock]] and [[percussion cap]] locks.
+
==Types of springs==
  
*[[Spiral spring]] or 'clock spring' - a spring of the type as used in [[clock]]s, [[galvanometer]]s, and places where electricity must be carried to partially-rotating devices such as [[steering wheel]]s.
+
[[Image:Montre Tribaudeau Besancon 01.jpg|thumb|right|250px|A [[balance spring|spiral hair spring]].]]
  
*[[springboard|Cantilever spring]] - a spring which is fixed only at one end.
+
Springs are classified according their properties.
  
Other types include:
+
Depending on the load, they may be classified as:
*[[Belleville washer]] or [[Belleville washer|Belleville spring]] - a disc shaped spring commonly used to apply tension to a bolt (and also in the initiation mechanism of pressure-activated [[land mine|landmines]]).
+
*Tension/Extension spring
 +
*Compression spring
 +
*Torsional spring
  
*Spring [[Washer (mechanical)|washer]] - used to apply a constant tensile force along the axis of a [[fastener]].
+
In the case of tension/extension springs and compression springs, there is axial load. On the other hand, the torsional spring has torsional force.
  
*[[Torsion spring]] -  any spring designed to be twisted rather than compressed or extended.
+
Depending on the material of the spring, it can be classified as:
 +
*Wire/Coil spring
 +
*Flat spring
  
*[[Gas spring]] - a volume of gas which is compressed.
+
The most common types of spring are:
 +
*[[springboard|Cantilever spring]] - a spring that is fixed at only one end.
 +
*[[Coil spring]] or [[helix|helical]] spring - a spring (made by winding a wire around a cylinder) and the [[Cone (geometry)|conical]] spring - these are types of [[torsion spring]], because the wire itself is twisted when the spring is compressed or stretched. These are in turn of two types:
 +
**''Compression springs'' are designed to become shorter when loaded. Their turns are not touching in the unloaded position, and they need no attachment points.
 +
***A ''[[volute spring]]'' is a compression spring in the form of a cone, designed so that under compression the coils are not forced against each other, thus permitting longer travel.
 +
**''Tension'' or ''extension springs'' are designed to become longer under load. Their turns are normally touching in the unloaded position, and they have a hook, eye or some other means of attachment at each end.
 +
* Hairspring or [[balance spring]] -  a delicate spiral torsion spring used in [[watch]]es, [[galvanometer]]s, and places where electricity must be carried to partially-rotating devices such as [[steering wheel]]s without hindering the rotation.
 +
*[[Leaf spring]] - a flat springy sheet, used in vehicle [[suspension (vehicle)|suspension]]s, electrical [[switch]]es, [[bow (weapon)|bow]]s.
 +
* [[V-spring]] - used in antique [[firearm]] mechanisms such as the [[wheellock]], [[flintlock]] and [[percussion cap]] locks.
  
 +
Other types include:
 +
*[[Belleville washer]] or Belleville spring - a disc-shaped spring commonly used to apply tension to a bolt (and in the initiation mechanism of pressure-activated [[land mine|landmines]]).
 +
*[[Constant-force spring]] - a tightly rolled ribbon that exerts a nearly constant force as it is unrolled.
 +
*[[Gas spring]] - a volume of compressed gas.
 +
*[[Ideal Spring]] - the notional spring used in physics: it has no weight, mass, or damping losses.
 +
*[[Mainspring]] - a spiral ribbon shaped spring used as a power source in [[watch]]es, [[clock]]s, [[music box]]es, windup [[toy]]s, and [[mechanically powered flashlight]]s
 
*[[Rubber band]] - a tension spring where energy is stored by stretching the material.
 
*[[Rubber band]] - a tension spring where energy is stored by stretching the material.
 +
*Spring [[Washer (mechanical)|washer]] - used to apply a constant tensile force along the axis of a [[fastener]].
 +
*[[Torsion spring]] -  any spring designed to be twisted rather than compressed or extended. Used in [[Torsion beam suspension|torsion bar]] vehicle suspension systems.
 +
*[[Constant-force spring|Negator spring]] -  a thin metal band slightly concave in cross-section. When coiled it adopts a flat cross-section but when unrolled it returns to its former curve, thus producing a constant force throughout the displacement and ''negating'' any tendency to re-wind. The commonest application is the retracting steel tape rule.<ref>Samuel, Andrew, and John Weir, ''Introduction to Engineering Design: Modelling, Synthesis and Problem Solving Strategies'', 2nd ed. (Oxford, England: Butterworth-Heinemann, 1999, p. 134. ISBN 0750642823).</ref>
 +
*[[Wave spring]] - a thin spring-washer into which waves have been pressed.<ref>Davis, Thomas Bieber, and Carl A. Nelson, Sr., ''Audel Mechanical Trades Pocket Manual'', 4th ed. (Hoboken, NJ: Wiley, 2003, p. 275. ISBN 9780764541704).</ref>
  
==Physics==
+
==Theory==
 
[[Image:SpringsInParallel.svg|right|thumb|280px|Two springs attached to a wall and a mass. In a situation like this, the two springs can be replaced by one with a spring constant of k<sub>eq</sub>=k<sub>1</sub>+k<sub>2</sub>.]]
 
[[Image:SpringsInParallel.svg|right|thumb|280px|Two springs attached to a wall and a mass. In a situation like this, the two springs can be replaced by one with a spring constant of k<sub>eq</sub>=k<sub>1</sub>+k<sub>2</sub>.]]
 +
 +
In classical [[physics]], a spring can be thought of as a device that absorbs [[potential energy]] when it is extended or compressed. The extension or compression strains the bonds between the [[atom]]s of the [[elasticity|elastic]] material.
  
 
===Hooke's Law===
 
===Hooke's Law===
 
{{main|Hooke's Law}}
 
{{main|Hooke's Law}}
  
Springs that are only stretched or compressed slightly obey Hooke's law, which states the force with which the spring pushes back is linearly proportional to the distance from its equilibrium length:
+
If the spring undergoes only slight stretching or compression, it obeys [[Hooke's law]] of [[theory of elasticity|elasticity]]. This law was named after British physicist [[Robert Hooke]], who discovered the principle in 1676.
 +
 
 +
In simple terms, Hooke's law states that the force with which a spring pushes back toward its equilibrium position is linearly proportional to the distance from its equilibrium length. More precisely, Hooke's law states that the extension of an elastic rod (its distended length minus its relaxed length) is linearly proportional to its [[Tension (mechanics)|tension]], the [[force]] used to stretch it. Likewise, the contraction (negative extension) is proportional to the [[Physical compression|compression]] (negative tension).
 +
 
 +
This law is valid only approximately, and only when the deformation (extension or contraction) is small compared to the spring's overall length. For deformations beyond the [[Tensile strength|elastic limit]], atomic bonds get broken or rearranged, and a spring may snap, buckle, or become permanently deformed. Many materials have no clearly defined elastic limit, and Hooke's law cannot be meaningfully applied to these materials.
 +
 
 +
In mathematical terms, Hooke's law can be written as:
 
:<math> F=-kx, \ </math>
 
:<math> F=-kx, \ </math>
 
where
 
where
: ''x'' is the distance the spring is elongated by,
+
: ''x'' is the distance through which the spring has been elongated or compressed,
 
: ''F'' is the restoring force exerted by the spring, and
 
: ''F'' is the restoring force exerted by the spring, and
: ''k'' is the '''spring constant''' or '''force constant''' of the spring.
+
: ''k'' is the ''spring constant'' or ''force constant'' of the spring.
  
 
===Simple harmonic motion===
 
===Simple harmonic motion===
{{main|Harmonic oscillator}}
+
 
Since force is equal to mass, ''m'', times acceleration, ''a'', the force equation looks like:
+
Given that [[force]] (''F'') is equal to [[mass]] (''m'') times [[acceleration]], ''a'', the force equation can be written as:
 
::<math>F = - k x = m a. \,</math>
 
::<math>F = - k x = m a. \,</math>
 +
 
[[Image:Simple harmonic motion.png|thumb|right|280px|The displacement, ''x'', as a function of time. The amount of time that passes between peaks is called the [[period]].]]
 
[[Image:Simple harmonic motion.png|thumb|right|280px|The displacement, ''x'', as a function of time. The amount of time that passes between peaks is called the [[period]].]]
But acceleration is just the second time [[derivative]] of x, so
+
 
 +
Given that acceleration is the second time [[derivative]] of x, one can write:
 
::<math> - k x = m \frac{d^2 x}{dt^2}. \,</math>
 
::<math> - k x = m \frac{d^2 x}{dt^2}. \,</math>
Re-arranging results in a [[differential equation]]
+
Rearranging the results, one gets the following [[differential equation]]:
::<math>\frac{d^2 x}{dt^2} + \frac{k}{m} x = 0, \,</math>
+
::<math>\frac{d^2 x}{dt^2} + \frac{k}{m} x = 0 \,</math>
the solution of which is the sum of a [[sine]] and [[cosine]]:
+
The solution of this equation is the sum of a [[sine]] and a [[cosine]]:
 
::<math> x(t) = A \sin \left( t \sqrt{\frac{k}{m}} \right) + B \cos \left(t \sqrt{\frac{k}{m}} \right). \, </math>
 
::<math> x(t) = A \sin \left( t \sqrt{\frac{k}{m}} \right) + B \cos \left(t \sqrt{\frac{k}{m}} \right). \, </math>
 
The graph of this function is displayed in the image on the right.
 
The graph of this function is displayed in the image on the right.
  
==Theory==
+
== Zero-length springs ==
  
In classical [[physics]], a spring can be seen as a device that stores [[potential energy]] by straining the bonds between the [[atom]]s of an [[elasticity|elastic]]  material.
+
"Zero-length spring" is the standard term for a spring that exerts zero force when it has zero length. In practice, a spring with "negative" length (in which the coils press together when the spring is relaxed) is combined with an extra length of inelastic material.
  
[[Hooke's law]] of [[theory of elasticity|elasticity]] states that the extension of an elastic rod (its distended length minus its relaxed length) is linearly proportional to its [[Tension (mechanics)|tension]], the [[force]] used to stretch it. Similarly, the contraction (negative extension) is proportional to the [[Physical compression|compression]] (negative tension).  
+
This type of spring was developed in 1932 by [[Lucien LaCoste]] for use in a vertical [[seismograph]]. A spring with zero length can be attached to a mass on a hinged boom, such that the force on the mass is almost exactly balanced by the vertical component of the force from the spring, whatever the position of the boom. This creates a pendulum with a very long period.
 +
Long-period pendulums enable [[seismometer]]s to sense the slowest waves from earthquakes. The LaCoste suspension with zero-length springs is also used in [[gravimeter]]s because it is very sensitive to changes in gravity.
  
This law actually holds only approximately, and only when the deformation (extension or contraction) is small compared to the rod's overall length.  For deformations beyond the [[Tensile strength|elastic limit]], atomic bonds get broken or rearranged, and a spring may snap, buckle, or permanently deform.  Many materials have no clearly defined elastic limit, and Hooke's law can not be meaningfully applied to these materials.  
+
Springs for closing doors are often made to have roughly zero length so that they will exert force even when the door is almost closed, allowing the door to close firmly.
  
Hooke's law is actually a mathematical consequence of the fact that the potential energy of the rod is a minimum when it has its relaxed length. Any smooth function of one variable approximates a [[quadratic function]] when examined near enough to its minimum point; and therefore the force &mdash; which is the [[derivative]] of energy with respect to displacement &mdash; will approximate a [[linear function]].
+
==Notes==
 +
<references/>
  
Contrary to popular belief, springs do not appreciably "[[Creep (deformation)|creep]]" or get "tired" with age.  Spring steel has a very high resistance to creep under normal loads.  The sag observed in older [[automobiles]] is really due to the springs being occasionally compressed beyond their yield point, causing plastic deformation.  This can happen when the vehicle hits a large bump or pothole, especially when heavily loaded.  Most vehicles will accumulate a number of such impacts over their working life, leading to a lower ride height and eventual bottoming-out of the suspension.
+
== References ==
<!--Must explain how torsion and bending springs work, i.e. how they can be analyzed in terms of infinitesimal rod springs, and that they too satisfy Hooke's law. Must also note that a helical spring is a torsion spring, not a simple rod spring. —>
 
  
==Toys==
+
* Associated Spring Corporation. 1964. ''Handbook of Mechanical Spring Design''. Bristol, CT: Associated Spring Corp. ASIN: B000TRJQEU.
{{mainarticle|Slinky}}
 
  
==Wikibooks modules==
+
* Brown, A. A. D. 1981. ''Mechanical Springs''. Engineering Design Guides, 42. [S.l.]: Published for the Design Council, the British Standards Institution, and the Council of Engineering Institutions by Oxford University Press. ISBN 0198591810.
*[http://wikibooks.org/wiki/Physics_Study_Guide/Springs Springs (Physics Study Guide)]
 
  
==External links==
+
* Dohrn-van Rossum, Gerhard. 1997. ''History of the Hour: Clocks and Modern Temporal Orders.'' Chicago: Univ. of Chicago Press. ISBN 0226155102.
  
*[http://www.allrite.com/helix.html Left Hand Versus Right Hand Wound Springs]
+
* Usher, Abbott Payson. 1988. ''A History of Mechanical Inventions.'' New York: Dover. ISBN 048625593X.
  
*[http://www.acewirespring.com/configuration.html Spring Design & Spring Configuration]
+
* Wahl, A. M. 1963. ''Mechanical Springs''. New York: McGraw-Hill. OCLC 562873.
 
 
*[http://www.acewirespring.com/spring-guide.html Spring Type Gallery]
 
 
 
*[http://yarchive.net/bike/tired_springs.html The Myth Of "Tired" Springs]
 
 
 
*[http://home.earthlink.net/~bazillion/intro.html Everything You Want To Know About Springs]
 
  
 +
==External links==
 +
All links retrieved February 8, 2023.
 +
* [http://www.madehow.com/Volume-6/Springs.html Springs]. How Products Are Made.
 
*[http://www.springmasters.com/spring-terminology.html Spring Terminology]
 
*[http://www.springmasters.com/spring-terminology.html Spring Terminology]
  
Line 95: Line 125:
 
[[Category:Physics]]
 
[[Category:Physics]]
  
{{credit|132002086}}
+
{{credits|Spring_(device)|132002086|Spring_(device)|351693409}}

Latest revision as of 16:14, 8 February 2023

Helical or coil springs designed for tension.

A spring is a flexible, elastic device used to store mechanical energy. When a force is applied to a spring, it expands or contracts to a certain extent, and when the force is released, the spring attempts to return to its earlier state.

Springs can be made of a variety of elastic materials, including fluids, but springs used in mechanical devices are generally made of metal. They also vary in shape; familiar shapes being helical, spiral, and flat.

Based on their behavior, springs are used to move objects, absorb vibrations, and control mechanical shock. For instance, they are useful in clocks, shock absorbers, motorized toys, pogo sticks, automobile engine valves, and door-closing mechanisms. Technically, a wooden bow is a form of spring.

Historical appearance

Simple, non-coiled springs, such as the bow (used with an arrow), have been used through much of human history. In the Bronze Age, more sophisticated spring devices were used, as indicated by the spread of tweezers in many cultures. Ctesibius of Alexandria developed a method for making bronze with spring-like characteristics by producing an alloy of bronze with an increased proportion of tin, then hardening it by hammering after it was cast.

Coiled springs appeared early in the fifteenth century,[1] leading to the development of the first spring-powered clocks in that century.[2][3][4] By the sixteenth century, the first large, spring-powered watches were produced.

Materials used for springs

As noted above, various elastic materials can be used to make springs. Even fluids under pressure demonstrate spring-like properties. Most springs, however, are made of metal, particularly hardened steel. Small springs can be wound from pre-hardened stock, while larger ones are made from annealed steel and hardened after fabrication. Some non-ferrous metals are also used, including phosphor bronze for parts requiring corrosion resistance, and beryllium copper for springs carrying electrical current (because its electrical resistance is low).

Types of springs

A spiral hair spring.

Springs are classified according their properties.

Depending on the load, they may be classified as:

  • Tension/Extension spring
  • Compression spring
  • Torsional spring

In the case of tension/extension springs and compression springs, there is axial load. On the other hand, the torsional spring has torsional force.

Depending on the material of the spring, it can be classified as:

  • Wire/Coil spring
  • Flat spring

The most common types of spring are:

  • Cantilever spring - a spring that is fixed at only one end.
  • Coil spring or helical spring - a spring (made by winding a wire around a cylinder) and the conical spring - these are types of torsion spring, because the wire itself is twisted when the spring is compressed or stretched. These are in turn of two types:
    • Compression springs are designed to become shorter when loaded. Their turns are not touching in the unloaded position, and they need no attachment points.
      • A volute spring is a compression spring in the form of a cone, designed so that under compression the coils are not forced against each other, thus permitting longer travel.
    • Tension or extension springs are designed to become longer under load. Their turns are normally touching in the unloaded position, and they have a hook, eye or some other means of attachment at each end.
  • Hairspring or balance spring - a delicate spiral torsion spring used in watches, galvanometers, and places where electricity must be carried to partially-rotating devices such as steering wheels without hindering the rotation.
  • Leaf spring - a flat springy sheet, used in vehicle suspensions, electrical switches, bows.
  • V-spring - used in antique firearm mechanisms such as the wheellock, flintlock and percussion cap locks.

Other types include:

  • Belleville washer or Belleville spring - a disc-shaped spring commonly used to apply tension to a bolt (and in the initiation mechanism of pressure-activated landmines).
  • Constant-force spring - a tightly rolled ribbon that exerts a nearly constant force as it is unrolled.
  • Gas spring - a volume of compressed gas.
  • Ideal Spring - the notional spring used in physics: it has no weight, mass, or damping losses.
  • Mainspring - a spiral ribbon shaped spring used as a power source in watches, clocks, music boxes, windup toys, and mechanically powered flashlights
  • Rubber band - a tension spring where energy is stored by stretching the material.
  • Spring washer - used to apply a constant tensile force along the axis of a fastener.
  • Torsion spring - any spring designed to be twisted rather than compressed or extended. Used in torsion bar vehicle suspension systems.
  • Negator spring - a thin metal band slightly concave in cross-section. When coiled it adopts a flat cross-section but when unrolled it returns to its former curve, thus producing a constant force throughout the displacement and negating any tendency to re-wind. The commonest application is the retracting steel tape rule.[5]
  • Wave spring - a thin spring-washer into which waves have been pressed.[6]

Theory

Two springs attached to a wall and a mass. In a situation like this, the two springs can be replaced by one with a spring constant of keq=k1+k2.

In classical physics, a spring can be thought of as a device that absorbs potential energy when it is extended or compressed. The extension or compression strains the bonds between the atoms of the elastic material.

Hooke's Law

If the spring undergoes only slight stretching or compression, it obeys Hooke's law of elasticity. This law was named after British physicist Robert Hooke, who discovered the principle in 1676.

In simple terms, Hooke's law states that the force with which a spring pushes back toward its equilibrium position is linearly proportional to the distance from its equilibrium length. More precisely, Hooke's law states that the extension of an elastic rod (its distended length minus its relaxed length) is linearly proportional to its tension, the force used to stretch it. Likewise, the contraction (negative extension) is proportional to the compression (negative tension).

This law is valid only approximately, and only when the deformation (extension or contraction) is small compared to the spring's overall length. For deformations beyond the elastic limit, atomic bonds get broken or rearranged, and a spring may snap, buckle, or become permanently deformed. Many materials have no clearly defined elastic limit, and Hooke's law cannot be meaningfully applied to these materials.

In mathematical terms, Hooke's law can be written as:

where

x is the distance through which the spring has been elongated or compressed,
F is the restoring force exerted by the spring, and
k is the spring constant or force constant of the spring.

Simple harmonic motion

Given that force (F) is equal to mass (m) times acceleration, a, the force equation can be written as:

The displacement, x, as a function of time. The amount of time that passes between peaks is called the period.

Given that acceleration is the second time derivative of x, one can write:

Rearranging the results, one gets the following differential equation:

The solution of this equation is the sum of a sine and a cosine:

The graph of this function is displayed in the image on the right.

Zero-length springs

"Zero-length spring" is the standard term for a spring that exerts zero force when it has zero length. In practice, a spring with "negative" length (in which the coils press together when the spring is relaxed) is combined with an extra length of inelastic material.

This type of spring was developed in 1932 by Lucien LaCoste for use in a vertical seismograph. A spring with zero length can be attached to a mass on a hinged boom, such that the force on the mass is almost exactly balanced by the vertical component of the force from the spring, whatever the position of the boom. This creates a pendulum with a very long period. Long-period pendulums enable seismometers to sense the slowest waves from earthquakes. The LaCoste suspension with zero-length springs is also used in gravimeters because it is very sensitive to changes in gravity.

Springs for closing doors are often made to have roughly zero length so that they will exert force even when the door is almost closed, allowing the door to close firmly.

Notes

  1. Springs How Products Are Made. Retrieved April 3, 2010.
  2. White Jr., Lynn, Medieval Technology and Social Change. (New York: Oxford Univ. Press, 1966, p. 126-127. ISBN 0195002660).
  3. Usher, Abbott Payson, A History of Mechanical Inventions (New York: Dover, 1988, p. 305. ISBN 048625593X). Retrieved April 3, 2010.
  4. Dohrn-van Rossum, Gerhard, History of the Hour: Clocks and Modern Temporal Orders. (Chicago: Univ. of Chicago Press, 1997, p. 121. ISBN 0226155102). Retrieved April 3, 2010.
  5. Samuel, Andrew, and John Weir, Introduction to Engineering Design: Modelling, Synthesis and Problem Solving Strategies, 2nd ed. (Oxford, England: Butterworth-Heinemann, 1999, p. 134. ISBN 0750642823).
  6. Davis, Thomas Bieber, and Carl A. Nelson, Sr., Audel Mechanical Trades Pocket Manual, 4th ed. (Hoboken, NJ: Wiley, 2003, p. 275. ISBN 9780764541704).

References
ISBN links support NWE through referral fees

  • Associated Spring Corporation. 1964. Handbook of Mechanical Spring Design. Bristol, CT: Associated Spring Corp. ASIN: B000TRJQEU.
  • Brown, A. A. D. 1981. Mechanical Springs. Engineering Design Guides, 42. [S.l.]: Published for the Design Council, the British Standards Institution, and the Council of Engineering Institutions by Oxford University Press. ISBN 0198591810.
  • Dohrn-van Rossum, Gerhard. 1997. History of the Hour: Clocks and Modern Temporal Orders. Chicago: Univ. of Chicago Press. ISBN 0226155102.
  • Usher, Abbott Payson. 1988. A History of Mechanical Inventions. New York: Dover. ISBN 048625593X.
  • Wahl, A. M. 1963. Mechanical Springs. New York: McGraw-Hill. OCLC 562873.

External links

All links retrieved February 8, 2023.

Credits

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