SherbyNet - /page/wikibook/entry.mu

Micron Document

<!DOCTYPE html>

<title>Frank–Read source</title>

</head>

Frank–Read source

</h1>

</header>

In <a href="Materials_science" title="Materials science">materials science</a>, a Frank–Read source is a mechanism explaining the generation of multiple <a href="Dislocation" title="Dislocation">dislocations</a> in specific well-spaced <a href="Slip_(materials_science)" title="Slip (materials science)">slip</a> planes in <a href="Crystal" title="Crystal">crystals</a> when they are <a href="Deformation_(physics)" title="Deformation (physics)">deformed</a>. When a crystal is deformed, in order for slip to occur, dislocations must be generated in the material. This implies that, during deformation, dislocations must be primarily generated in these planes. <a href="Cold_work" class="mw-redirect" title="Cold work">Cold working</a> of metal increases the number of dislocations by the Frank–Read mechanism. Higher dislocation density increases <a href="Yield_strength" class="mw-redirect" title="Yield strength">yield strength</a> and causes <a href="Work_hardening" title="Work hardening">work hardening</a> of metals.

The mechanism of dislocation generation was proposed by and named after British physicist <a href="Charles_Frank_(physicist)" title="Charles Frank (physicist)">Charles Frank</a> and Thornton Read.

In 2024, Cheng Long and coworkers demonstrated that the Frank-Read mechanism can generate <a href="Disclination" title="Disclination">disclination</a> loops in nematic liquid crystals.<a href="#cite_note-FrankReadNematic-1">[1]</a> This finding suggests that the Frank-Read mechanism may arise in a broader class of materials containing <a href="Topological_defect" title="Topological defect">topological defect</a> lines.

<div class="mw-heading mw-heading2"><h2 id="History">History</h2></div>

Charles Frank detailed the history of the discovery from his perspective in <a href="Proceedings_of_the_Royal_Society" title="Proceedings of the Royal Society">Proceedings of the Royal Society</a> in 1980.<a href="#cite_note-Frank1-2">[2]</a>

In 1950 <a href="Charles_Frank_(physicist)" title="Charles Frank (physicist)">Charles Frank</a>, who was then a research fellow in the physics department at the <a href="University_of_Bristol" title="University of Bristol">University of Bristol</a>, visited the United States to participate in a conference on crystal <a href="Plasticity_(physics)" title="Plasticity (physics)">plasticity</a> in <a href="Pittsburgh" title="Pittsburgh">Pittsburgh</a>. Frank arrived in the United States well in advance of the conference to spend time at a naval laboratory and to give a lecture at <a href="Cornell_University" title="Cornell University">Cornell University</a>. When, during his travels in Pennsylvania, Frank visited Pittsburgh, he received a letter from fellow scientist <a href="John_D._Eshelby" title="John D. Eshelby">Jock Eshelby</a> suggesting that he read a recent paper by Gunther Leibfried. Frank was supposed to board a train to Cornell to give his lecture at Cornell, but before departing for Cornell he went to the library at <a href="Carnegie_Institute_of_Technology" class="mw-redirect" title="Carnegie Institute of Technology">Carnegie Institute of Technology</a> to obtain a copy of the paper. The library did not yet have the journal with Leibfried's paper, but the staff at the library believed that the journal could be in the recently arrived package from Germany. Frank decided to wait for the library to open the package, which did indeed contain the journal. Upon reading the paper he took a train to Cornell, where he was told to pass the time until 5:00, as the faculty was in meeting. Frank decided to take a walk between 3:00 and 5:00. During those two hours, while considering the Leibfried paper, he formulated the theory for what was later named the Frank–Read source.

A couple of days later, he traveled to the conference on crystal plasticity in Pittsburgh where he ran into Thornton Read in the hotel lobby. Upon encountering each other, the two scientists immediately discovered that they had come up with the same idea for dislocation generation almost simultaneously (Frank during his walk at Cornell, and Thornton Read during tea the previous Wednesday) and decided to write a joint paper on the topic. The mechanism for dislocation generation described in that paper<a href="#cite_note-FrankRead-3">[3]</a> is now known as the Frank–Read source.

<div class="mw-heading mw-heading2"><h2 id="Mechanism">Mechanism</h2></div>

The Frank–Read source is a mechanism based on dislocation multiplication in a slip plane under <a href="Shear_stress" title="Shear stress">shear stress</a>.<a href="#cite_note-Hosford-4">[4]</a><a href="#cite_note-Khan-5">[5]</a>

Consider a straight dislocation in a crystal slip plane with its two ends, A and B, pinned. If a shear stress <math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle \tau }">

</mstyle>

</mrow>

<annotation encoding="application/x-tex">{\displaystyle \tau }</annotation>

</semantics>

</math><img src="./38a7dcde9730ef0853809fefc18d88771f95206c.svg" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -0.338ex; width:1.202ex; height:1.676ex;" alt="{\displaystyle \tau }" loading="lazy"> is exerted on the slip plane then a force <math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle F=\tau \cdot bx}">

</mstyle>

</mrow>

<annotation encoding="application/x-tex">{\displaystyle F=\tau \cdot bx}</annotation>

</semantics>

</math><img src="./317cfb69dbab82864cad49be03f0e88623898bd3.svg" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -0.338ex; width:10.048ex; height:2.176ex;" alt="{\displaystyle F=\tau \cdot bx}" loading="lazy">, where b is the <a href="Burgers_vector" title="Burgers vector">Burgers vector</a> of the dislocation and x is the distance between the pinning sites A and B, is exerted on the dislocation line as a result of the shear stress. This force acts <a href="Perpendicular" title="Perpendicular">perpendicularly</a> to the line, inducing the dislocation to lengthen and curve into an arc.

The bending force caused by the shear stress is opposed by the line <a href="Tension_(physics)" title="Tension (physics)">tension</a> of the dislocation, which acts on each end of the dislocation along the direction of the dislocation line away from A and B with a magnitude of <math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle Gb^{2}}">

<msup>

</mrow>

</msup>

</mstyle>

</mrow>

<annotation encoding="application/x-tex">{\displaystyle Gb^{2}}</annotation>

</semantics>

</math><img src="./71bcd0a5cac7552645627503624c3921bb70e187.svg" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -0.338ex; width:3.879ex; height:2.676ex;" alt="{\displaystyle Gb^{2}}" loading="lazy">, where G is the <a href="Shear_modulus" title="Shear modulus">shear modulus</a>. If the dislocation bends, the ends of the dislocation make an angle with the horizontal between A and B, which gives the line tensions acting along the ends a <a href="Vertical_direction" class="mw-redirect" title="Vertical direction">vertical</a> <a href="Vector_component" class="mw-redirect" title="Vector component">component</a> acting directly against the force induced by the shear stress. If sufficient shear stress is applied and the dislocation bends, the vertical component from the line tensions, which acts directly against the force caused by the shear stress, grows as the dislocation approaches a semicircular shape.

When the dislocation becomes a semicircle, all of the line tension is acting against the bending force induced by the shear stress, because the line tension is perpendicular to the <a href="Horizontal_plane" class="mw-redirect" title="Horizontal plane">horizontal</a> between A and B. For the dislocation to reach this point, it is thus evident that the equation:<a href="#cite_note-Hosford-4">[4]</a><a href="#cite_note-Khan-5">[5]</a>

<msup>

</mrow>

</msup>

</mstyle>

</mrow>

<annotation encoding="application/x-tex">{\displaystyle F=\tau \cdot bx=2Gb^{2}}</annotation>

</semantics>

</math><img src="./b1f7443fec214e5592e7bda1ca7b8b50acfec4c2.svg" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -0.338ex; width:18.187ex; height:2.676ex;" alt="{\displaystyle F=\tau \cdot bx=2Gb^{2}}" loading="lazy"></dd></dl>

must be satisfied, and from this we can solve for the shear stress:<a href="#cite_note-Hosford-4">[4]</a><a href="#cite_note-Khan-5">[5]</a>

<mfrac>

<mrow>

</mrow>

</mfrac>

</mrow>

</mstyle>

</mrow>

<annotation encoding="application/x-tex">{\displaystyle \tau ={\frac {2Gb}{x}}}</annotation>

</semantics>

</math><img src="./d362ba4fe889c487b9f5ad7dc49ec684d03ace81.svg" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -1.838ex; width:9.123ex; height:5.343ex;" alt="{\displaystyle \tau ={\frac {2Gb}{x}}}" loading="lazy"></dd></dl>

This is the stress required to generate dislocation from a Frank–Read source. If the shear stress increases any further and the dislocation passes the semicircular <a href="Equilibrium_state" class="mw-redirect" title="Equilibrium state">equilibrium state</a>, it will spontaneously continue to bend and grow, spiraling around the A and B pinning points, until the segments spiraling around the A and B pinning points collide and cancel. The process results in a dislocation loop around A and B in the slip plane which expands under continued shear stress, and also in a new dislocation line between A and B which, under renewed or continued shear, can continue to generate dislocation loops in the manner just described.

A Frank–Read loop can thus generate many dislocations in a plane in a crystal under applied stress. The Frank–Read source mechanism explains why dislocations are primarily generated on certain slip planes; dislocations are primarily generated in just those planes with Frank–Read sources. It is important to note that if the shear stress does not exceed:<a href="#cite_note-Hosford-4">[4]</a><a href="#cite_note-Khan-5">[5]</a>

<mfrac>

<mrow>

</mrow>

</mfrac>

</mrow>

</mstyle>

</mrow>

<annotation encoding="application/x-tex">{\displaystyle \tau ={\frac {2Gb}{x}}}</annotation>

</semantics>

and the dislocation does not bend past the semicircular equilibrium state, it will not form a dislocation loop and instead revert to its original state.<a href="#cite_note-Hosford-4">[4]</a><a href="#cite_note-Khan-5">[5]</a>

<div class="mw-heading mw-heading2"><h2 id="References">References</h2></div>

/* start https://en.wikipedia.org/ */

.mw-parser-output .reflist{margin-bottom:0.5em;list-style-type:decimal}@media screen{.mw-parser-output .reflist{font-size:90%}}.mw-parser-output .reflist .references{font-size:100%;margin-bottom:0;list-style-type:inherit}.mw-parser-output .reflist-columns-2{column-width:30em}.mw-parser-output .reflist-columns-3{column-width:25em}.mw-parser-output .reflist-columns{margin-top:0.3em}.mw-parser-output .reflist-columns ol{margin-top:0}.mw-parser-output .reflist-columns li{page-break-inside:avoid;break-inside:avoid-column}.mw-parser-output .reflist-upper-alpha{list-style-type:upper-alpha}.mw-parser-output .reflist-upper-roman{list-style-type:upper-roman}.mw-parser-output .reflist-lower-alpha{list-style-type:lower-alpha}.mw-parser-output .reflist-lower-greek{list-style-type:lower-greek}.mw-parser-output .reflist-lower-roman{list-style-type:lower-roman}

/* end https://en.wikipedia.org/ */

</style><div class="reflist">

/* start https://en.wikipedia.org/ */

.mw-parser-output cite.citation{font-style:inherit;word-wrap:break-word}.mw-parser-output .citation q{quotes:"\"""\"""'""'"}.mw-parser-output .citation:target{background-color:rgba(0,127,255,0.133)}.mw-parser-output .id-lock-free.id-lock-free a{background:url("./mw/Lock-green.svg")right 0.1em center/9px no-repeat}.mw-parser-output .id-lock-limited.id-lock-limited a,.mw-parser-output .id-lock-registration.id-lock-registration a{background:url("./mw/Lock-gray-alt-2.svg")right 0.1em center/9px no-repeat}.mw-parser-output .id-lock-subscription.id-lock-subscription a{background:url("./mw/Lock-red-alt-2.svg")right 0.1em center/9px no-repeat}.mw-parser-output .cs1-ws-icon a{background:url("./mw/Wikisource-logo.svg")right 0.1em center/12px no-repeat}body:not(.skin-timeless):not(.skin-minerva) .mw-parser-output .id-lock-free a,body:not(.skin-timeless):not(.skin-minerva) .mw-parser-output .id-lock-limited a,body:not(.skin-timeless):not(.skin-minerva) .mw-parser-output .id-lock-registration a,body:not(.skin-timeless):not(.skin-minerva) .mw-parser-output .id-lock-subscription a,body:not(.skin-timeless):not(.skin-minerva) .mw-parser-output .cs1-ws-icon a{background-size:contain;padding:0 1em 0 0}.mw-parser-output .cs1-code{color:inherit;background:inherit;border:none;padding:inherit}.mw-parser-output .cs1-hidden-error{display:none;color:var(--color-error,#d33)}.mw-parser-output .cs1-visible-error{color:var(--color-error,#d33)}.mw-parser-output .cs1-maint{display:none;color:#085;margin-left:0.3em}.mw-parser-output .cs1-kern-left{padding-left:0.2em}.mw-parser-output .cs1-kern-right{padding-right:0.2em}.mw-parser-output .citation .mw-selflink{font-weight:inherit}@media screen{.mw-parser-output .cs1-format{font-size:95%}html.skin-theme-clientpref-night .mw-parser-output .cs1-maint{color:#18911f}}@media screen and (prefers-color-scheme:dark){html.skin-theme-clientpref-os .mw-parser-output .cs1-maint{color:#18911f}}

/* end https://en.wikipedia.org/ */

</style><cite id="CITEREFLong2024" class="citation journal cs1">Long, Cheng (11 March 2024). <a rel="nofollow" class="external text" href="https://journals.aps.org/prx/abstract/10.1103/PhysRevX.14.011044">"Frank-Read Mechanism in Nematic Liquid Crystals"</a>. Physical Review X. 14: 011044. <a href="ArXiv_(identifier)" class="mw-redirect" title="ArXiv (identifier)">arXiv</a>:<a rel="nofollow" class="external text" href="https://arxiv.org/abs/2212.01316">2212.01316</a>. <a href="Doi_(identifier)" class="mw-redirect" title="Doi (identifier)">doi</a>:<a rel="nofollow" class="external text" href="https://doi.org/10.1103%2FPhysRevX.14.011044">10.1103/PhysRevX.14.011044</a>. Retrieved 2025-01-04.</cite>

</li>

<li id="cite_note-Frank1-2"><a href="#cite_ref-Frank1_2-0">^</a> <cite class="citation journal cs1">"The Beginnings of Solid State Physics". <a href="Proceedings_of_the_Royal_Society#Proceedings_of_the_Royal_Society_A" title="Proceedings of the Royal Society">Proceedings of the Royal Society A</a>. 371 (1744). <a href="Royal_Society" title="Royal Society">Royal Society of London for the Improvement of Natural Knowledge</a>: 136–138. 1980-06-10. <a href="Bibcode_(identifier)" class="mw-redirect" title="Bibcode (identifier)">Bibcode</a>:<a rel="nofollow" class="external text" href="https://ui.adsabs.harvard.edu/abs/1980RSPSA.371..136.">1980RSPSA.371..136.</a>. <a href="Doi_(identifier)" class="mw-redirect" title="Doi (identifier)">doi</a>:<a rel="nofollow" class="external text" href="https://doi.org/10.1098%2Frspa.1980.0069">10.1098/rspa.1980.0069</a>. <a href="S2CID_(identifier)" class="mw-redirect" title="S2CID (identifier)">S2CID</a> <a rel="nofollow" class="external text" href="https://api.semanticscholar.org/CorpusID:195958648">195958648</a>.</cite>

</li>

<li id="cite_note-FrankRead-3"><a href="#cite_ref-FrankRead_3-0">^</a> <cite id="CITEREFFrankRead_Jr1950" class="citation journal cs1">Frank, F. C.; Read Jr, W. T. (1950). "Multiplication Processes for Slow Moving Dislocations". Physical Review. 79 (4): 722–723. <a href="Bibcode_(identifier)" class="mw-redirect" title="Bibcode (identifier)">Bibcode</a>:<a rel="nofollow" class="external text" href="https://ui.adsabs.harvard.edu/abs/1950PhRv...79..722F">1950PhRv...79..722F</a>. <a href="Doi_(identifier)" class="mw-redirect" title="Doi (identifier)">doi</a>:<a rel="nofollow" class="external text" href="https://doi.org/10.1103%2FPhysRev.79.722">10.1103/PhysRev.79.722</a>.</cite>

</li>

<li id="cite_note-Hosford-4">^ <a href="#cite_ref-Hosford_4-0">a</a> <a href="#cite_ref-Hosford_4-1">b</a> <a href="#cite_ref-Hosford_4-2">c</a> <a href="#cite_ref-Hosford_4-3">d</a> <a href="#cite_ref-Hosford_4-4">e</a> <cite id="CITEREFHosford2005" class="citation book cs1">Hosford, William F. (2005). Mechanical Behavior of Materials. <a href="Cambridge_University_Press" title="Cambridge University Press">Cambridge University Press</a>. <a href="ISBN_(identifier)" class="mw-redirect" title="ISBN (identifier)">ISBN</a> <bdi>978-0-521-84670-7</bdi>.</cite>

</li>

<li id="cite_note-Khan-5">^ <a href="#cite_ref-Khan_5-0">a</a> <a href="#cite_ref-Khan_5-1">b</a> <a href="#cite_ref-Khan_5-2">c</a> <a href="#cite_ref-Khan_5-3">d</a> <a href="#cite_ref-Khan_5-4">e</a> <cite id="CITEREFKhan,_A._S.Huang,_S1989" class="citation book cs1">Khan, A. S., A. S.; Huang, S (1989). Continuum Theory of Plasticity. <a href="Amsterdam" title="Amsterdam">Amsterdam</a>: <a href="Elsevier" title="Elsevier">Elsevier</a>.</cite>

</li>

</ol></div></div></div><div><div class="zim-footer">

This article is issued from <a class="external text" title="Last edited on 2025-01-06" href="https://en.wikipedia.org/wiki/?title=Frank%E2%80%93Read_source&oldid=1267664425">Wikipedia</a>. The text is available under <a class="external text" href="https://creativecommons.org/licenses/by-sa/4.0/deed.en">Creative Commons Attribution-Share Alike 4.0</a> unless otherwise noted. Additional terms may apply for the media files.

</div>

</div></div>

</div>

</main>

</div>

</body></html>