<?xml version="1.0" encoding="UTF-8"?><rss xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:content="http://purl.org/rss/1.0/modules/content/" xmlns:atom="http://www.w3.org/2005/Atom" version="2.0"><channel><title><![CDATA[Metallurgy Daily Blogs]]></title><description><![CDATA[Metallurgy Daily Blogs]]></description><link>https://blogs.metallurgydaily.in</link><image><url>https://cdn.hashnode.com/res/hashnode/image/upload/v1750601418859/cc89801f-b626-4827-89e6-64a46e496c45.png</url><title>Metallurgy Daily Blogs</title><link>https://blogs.metallurgydaily.in</link></image><generator>RSS for Node</generator><lastBuildDate>Wed, 15 Apr 2026 16:32:50 GMT</lastBuildDate><atom:link href="https://blogs.metallurgydaily.in/rss.xml" rel="self" type="application/rss+xml"/><language><![CDATA[en]]></language><ttl>60</ttl><item><title><![CDATA[Ductile vs Brittle behavior]]></title><description><![CDATA[The behavior of materials under loading can be classified as ductile or brittle depending on if the material undergoes gross plastic deformation. The following figure represents the stress-strain curve for ductile and brittle materials.

As we can se...]]></description><link>https://blogs.metallurgydaily.in/ductile-vs-brittle-behavior</link><guid isPermaLink="true">https://blogs.metallurgydaily.in/ductile-vs-brittle-behavior</guid><dc:creator><![CDATA[Metallurgy Daily]]></dc:creator><pubDate>Sun, 22 Jun 2025 14:18:23 GMT</pubDate><content:encoded><![CDATA[<p>The behavior of materials under loading can be classified as ductile or brittle depending on if the material undergoes gross plastic deformation. The following figure represents the stress-strain curve for ductile and brittle materials.</p>
<p><img alt /></p>
<p>As we can see that a brittle material almost fails at elastic limit. But brittleness is not an absolute property of a material. For example, tungsten is brittle at room temperature and is ductile at high temperatures. The three factors contributing to brittle fracture are : triaxial state of stress, low temperature and high strain rate. All these factors need not be present for a material to show brittle cleavage. A triaxial stress which is present at notch along with low temperature may lead to brittle fracture. Also high strain rate assists those two factors.</p>
<p>For most of the engineering materials ductility is an important criteria. Thus, little amount of ductility is needed for most of the material. Also a material being ductile has its own advantage. A ductile material before failure undergoes plastic deformation thus indicating that it is going to fail. Whereas a brittle fracture is sudden without any warning. Thus most of the place ductile materials are preferred over brittle materials.</p>
<p><img alt /></p>
<p>Usually ductile facture is preceded by gross plastic deformation known as necking which begins from the maximum stress. Necking begins when increase in strength due to strain hardening fails to compensate by the decrease in cross-sectional area. A rupture occurs when a ductile material is drawn down to a line or a point and then fails. The necking introduces a triaxial state of stress in that region. Many cavities are also formed in that region which on continued strain grows into a large crack. This crack grows in a direction perpendicular to the axis of the specimen. It then propagates along 45° i.e. the shear plane. This type of fracture is also known as cup and cone fracture. While the crack growth direction id outwards i.e. transverse to the tensile axis of the specimen, in a microscopic scale the crack actually moves in a zig-zag manner. The preferred sites of void formation are usually in inclusion, secondary phase particles etc. , whereas for pure metal they are grain boundary triple point. Ductility decreases as the void fraction increases, as the strain-hardening exponent n.</p>
]]></content:encoded></item><item><title><![CDATA[The Ellingham Diagram]]></title><description><![CDATA[The Ellingham diagram is the simplest method of representing the relationship between the free energy(ΔG) and temperature of various oxides and sulphides.
In metallurgy, the Ellingham diagram is used to  find out a suitable reducing agent. In the Ell...]]></description><link>https://blogs.metallurgydaily.in/the-ellingham-diagram</link><guid isPermaLink="true">https://blogs.metallurgydaily.in/the-ellingham-diagram</guid><dc:creator><![CDATA[Metallurgy Daily]]></dc:creator><pubDate>Sun, 22 Jun 2025 14:16:14 GMT</pubDate><content:encoded><![CDATA[<p>The Ellingham diagram is the simplest method of representing the relationship between the free energy(ΔG) and temperature of various oxides and sulphides.</p>
<p>In metallurgy, the Ellingham diagram is used to  find out a suitable reducing agent. In the Ellingham diagram the highly stable oxides are found at the bottom and the less stable oxides are found at the top. An element occupying a lower position in the diagram can reduce the oxides of another element present above it. For example, Mg lies below Si thus Mg can be used as a reducing agent for oxides of Si.</p>
<p><strong>Why Ellingham diagram has all straight lines?</strong></p>
<p><strong>Reason for upward slope of lines</strong></p>
<p>The Ellingham diagram is based on a formula given by:</p>
<p>ΔG = ΔH – TΔS</p>
<p>If we draw a graph with ΔG as y-axis and T as x-axis the slope of the curve represents the entropy(ΔS) and the intercept is enthalpy(ΔH). From the above equation we know that enthalpy is independent of temperature and entropy alone depends on temperature. The condition for a reaction to occur or to be spontaneous is to have negative ΔG. Most of the oxides forming reactions are exothermic i.e. ΔH is negative. And if we consider the reaction:</p>
<p>2Mg<sub>(s)</sub> + O<sub>2(g)</sub> = 2MgO<sub>(s)</sub> + Heat</p>
<p>Here we can see that there is a phase transformation taking place from gaseous phase to solid phase. Thus due to this reason the entropy decreases and becomes negatives(-ΔS).Thus if we consider this in the free energy equation, we get :</p>
<p>ΔG = ΔH – T(-ΔS)</p>
<p>ΔG = ΔH + T(ΔS)</p>
<p>Here, if we consider ΔG as y(since we considered it as y-axis), ΔH as c, ΔS as m, T as x(since we considered it as x-axis) we get the straight line equation:</p>
<p>y = mx + c</p>
<p>Thus, this explain why the Ellingham diagram has all straight lines  rather than curves. Also for this condition if we consider in terms of graph we get a straight line with positive slope i.e. sloping upwards.</p>
<p>Another important point to note is that, the Gibbs free energy(ΔG) here is considers as Standard free energy of formation of oxides kJ/mole for O<sub>2</sub> . Thus, that’s the reason why only one mole of O<sub>2</sub> is considered for all reactions.</p>
<p><strong>Exceptions in Ellingham diagram</strong>  </p>
<p>There are two exceptions in the Ellingham diagram. They are as follows.</p>
<p>Let us consider the following reaction :</p>
<p>C<sub>(s)</sub> + O<sub>2(g) </sub> \= CO<sub>2(g)</sub></p>
<p>Here, we can see that one molecule of gas(O<sub>2(g)</sub>)  produces one molecule of gas(CO<sub>2(g)</sub>).As the entropy of solids are the lowest thus it can be considered as negligible. Thus, there is no net entropy and the line is almost horizontal.</p>
<p>Let us consider another reaction :</p>
<p> 2C<sub>(s)</sub> + O<sub>2(g) </sub> \= 2CO<sub>(g)</sub></p>
<p>Here, we can see that one molecule of gas produces two molecule of gas i.e. the entropy increases and becomes positive(+ΔS). Thus if we consider this in the Gibbs free energy equation, we get :</p>
<p>ΔG = ΔH - T(ΔS)</p>
<p>This above equation is a representation of negative slope i.e. we get a line sloping downwards.</p>
<p><strong>Limitations of Ellingham diagram</strong></p>
<ol>
<li><p>The Ellingham diagram doesn’t explain the kinetics of the reduction.</p>
</li>
<li><p>In Ellingham diagram all the reactants and products are considered to be in equilibrium. As we know that, it’s not always true.</p>
</li>
</ol>
]]></content:encoded></item><item><title><![CDATA[The Iron-carbon Phase Diagram]]></title><description><![CDATA[Of all binary alloy systems the one that is possibly the most important for a metallurgist is the iron and carbon system. We know that both steel and cast iron play a important role in structural applications and they both are iron-carbon system.

Pu...]]></description><link>https://blogs.metallurgydaily.in/the-iron-carbon-phase-diagram</link><guid isPermaLink="true">https://blogs.metallurgydaily.in/the-iron-carbon-phase-diagram</guid><category><![CDATA[metallurgydaily]]></category><category><![CDATA[Metallurgy]]></category><category><![CDATA[Metallurgy Industry]]></category><dc:creator><![CDATA[Metallurgy Daily]]></dc:creator><pubDate>Sun, 22 Jun 2025 14:09:14 GMT</pubDate><enclosure url="https://cdn.hashnode.com/res/hashnode/image/upload/v1750600894060/dd215dca-1057-4154-9170-62cb165d1a55.jpeg" length="0" type="image/jpeg"/><content:encoded><![CDATA[<p><mark>Of all binary alloy systems the one that is possibly the most important for a metallurgist is the iron and carbon system. We know that both steel and cast iron play a important role in structural applications and they both are iron-carbon system.</mark></p>
<p><img src="https://cdn.hashnode.com/res/hashnode/image/upload/v1750601599126/1d3d2b92-d088-450d-8506-b5e5883e42d9.png" alt class="image--center mx-auto" /></p>
<p>Pure iron, upon heating, experiences changes in its crystal structure until 1538°C and melts there. At room temperature, it is present in a stable form called ferrite (α), which has a BCC crystal structure. The ferrite transforms to austenite (γ) at 912°C, which has an FCC crystal structure. At 1394°C, it again undergoes a phase transformation to δ-ferrite, which has a BCC crystal structure. Pure iron finally melts at 1538°C. All these changes can be seen on the left vertical axis of the Fe-C phase diagram.</p>
<p>In the composition axis at 6.7% formation of a intermediate compound known as Fe<sub>3</sub>C(Cementite) or iron carbide is observed. In real world all steels and cast iron have carbon content less than 6.7%. Thus in the Fe-C system consideration only upto 6.7% C is taken. Here, 6.7% C is considered as 100% Fe<sub>3</sub>C. Between 0.02-0.76% C  it is considered as Hypo eutectoid steel  and between 0.76-2.14% C it is considered as Hypereutectoid steel.</p>
<p>Carbon is a interstitial compound here and forms solid solution with α,δ and ט. In BCC α ferrite only small concentration of carbon is soluble about 0.02% at 727°C. The limited solubility is explained by the size and shape of BCC interstitial position. The maximum solubility of carbon in ט is about 2.14% at 1147°C. The δ-ferrite is same as α except for the fact that it occurs at higher temperature.</p>
<p>Eutectic reaction for Fe-C system(1147°C):</p>
<p><strong>L ⇌ ט + Fe₃C</strong></p>
<p>Eutectoid reaction for Fe-C system(727°C):</p>
<p><strong>ט ⇌ α + Fe₃C</strong></p>
<p>Peritectic reaction for Fe-C system(1493°C):</p>
<p><strong>δ + L ⇌ ט</strong></p>
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