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Preparation and characterization of electrospun silver nanowires/ZnO/PVP composite transparent conductive film 电纺银纳米线/ZnO/PVP 复合透明导电膜的制备与表征
IF 1.9 4区 物理与天体物理 Q3 PHYSICS, APPLIED Pub Date : 2024-04-05 DOI: 10.1142/s0217984924410161
Ching-Ho Hsie, Pin-Hsuan Chiu, Yu-Shu Chien, Wei-Ming Chiu, Chen-Feng Kuan, Chane-Yuan Yang

In this study, a silver nanowires (AgNWs)/nano-zinc oxide (ZnO)/polyvinylpyrrolidone (PVP) film is fabricated as an alternative to indium tin oxide transparent conductive films (TCFs). AgNWs are prepared by the polyol method with PVP as a dispersant to prevent Ag nanoparticles agglomeration during AgNWs formation. Nano-ZnO is synthesized using sol–gel method. AgNWs/ZnO/PVP TCFs are prepared using the electrostatic spinning and spin coating methods for comparison. It is found that the best PVP/AgNO3 molar ratio is 3.5:1. FTIR and XRD analyses show that 500°C calcination leads to better crystallinity and purity of nano-ZnO. Four-point prober analysis indicates that the higher the AgNWs content, the lower the TCF sheet resistance. The best sheet resistance of AgNWs/ZnO/PVP TCF by the electrostatic spinning method is obtained as 81 Ω/sq, and the light transmittance is 85.3%. Moreover, in the 5-week stability test, the sheet resistance of the electrospun TCF increases by 6.17%, much lower than 24.9% of the spin coated TCF. It is verified that the elecrospun AgNWs/ZnO/PVP composite TCF is a promising alternative to the traditional ITO TCFs.

本研究制作了银纳米线(AgNWs)/纳米氧化锌(ZnO)/聚乙烯吡咯烷酮(PVP)薄膜,作为氧化铟锡透明导电薄膜(TCFs)的替代品。AgNW 采用多元醇法制备,PVP 作为分散剂可防止 AgNW 形成过程中的 Ag 纳米颗粒团聚。纳米氧化锌采用溶胶-凝胶法合成。采用静电纺丝法和旋涂法制备 AgNWs/ZnO/PVP TCF,并进行比较。结果发现,最佳的 PVP/AgNO3 摩尔比为 3.5:1。傅立叶变换红外光谱和 XRD 分析表明,500°C 煅烧能使纳米氧化锌的结晶度和纯度更高。四点探针分析表明,AgNWs 含量越高,TCF 薄膜电阻越低。通过静电纺丝法,AgNWs/ZnO/PVP TCF 的最佳薄层电阻为 81 Ω/sq,透光率为 85.3%。此外,在 5 周的稳定性测试中,电纺 TCF 的薄层电阻增加了 6.17%,远低于旋涂 TCF 的 24.9%。实验证明,电纺 AgNWs/ZnO/PVP 复合 TCF 是替代传统 ITO TCF 的理想选择。
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引用次数: 0
Numerical simulation of the residual stress of solid oxide fuel cells with a three-dimensional nonplanar cathode–electrolyte interface 具有三维非平面阴极-电解质界面的固体氧化物燃料电池残余应力的数值模拟
IF 1.9 4区 物理与天体物理 Q3 PHYSICS, APPLIED Pub Date : 2024-04-05 DOI: 10.1142/s0217984924503445
Dingxi Xue, Yufeng Du, Chaoxia Huo, Bingyao Yi, Guojun Li, Keqin Liu

The longevity of solid oxide fuel cells is influenced by internal residual stresses, which may induce deformation or fracturing of components. This study investigates the residual stress distribution at the nonplanar cathode–electrolyte interface by approximating the actual interface with trigonometric functions and developing a three-dimensional (3D) model. The model reveals that the stress patterns at nonplanar interfaces can elucidate the genesis of interfacial cracks. During fabrication, anode contraction results in compressive stress within the electrolyte and tensile stress within the anode, with thermal discrepancies between layers being the primary cause of residual stresses. The reduction process diminishes these stresses, thus enhancing the mechanical integrity of the cell. Mitigating interface nonplanarity is beneficial for minimizing residual stress. At each interface crest, the electrolyte exhibits a local minimum in compressive stress, and a local maximum in shear stress occurs between each crest and trough. Furthermore, decreasing the initial porosity and NiO volume fraction can slightly lessen interlayer thermal discrepancies, with little effect on residual stresses.

固体氧化物燃料电池的寿命受内部残余应力的影响,残余应力可能导致组件变形或断裂。本研究通过三角函数近似实际界面并建立三维(3D)模型,研究了非平面阴极-电解质界面的残余应力分布。该模型揭示了非平面界面的应力模式,可以阐明界面裂纹的成因。在制造过程中,阳极收缩会在电解液中产生压应力,在阳极中产生拉应力,层间的热差异是产生残余应力的主要原因。还原工艺可减少这些应力,从而提高电池的机械完整性。减少界面非平面性有利于最大限度地减少残余应力。在每个界面波峰处,电解质会产生局部最小压应力,而在每个波峰和波谷之间会产生局部最大剪应力。此外,降低初始孔隙率和氧化镍体积分数可略微减小层间热差异,但对残余应力影响不大。
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引用次数: 0
High-performance quasi-2D perovskite solar cells enabled by using π-conjugated spacer 利用π-共轭间隔物实现高性能准二维过氧化物太阳能电池
IF 1.9 4区 物理与天体物理 Q3 PHYSICS, APPLIED Pub Date : 2024-04-05 DOI: 10.1142/s0217984924410021
Shahnawaz, Chih-Yu Fang, Chih-Yu Chang

The excellent photoelectric properties and low fabrication cost of perovskite solar cells have attracted extensive research attention. Despite this, long-term stability issues associated with perovskite solar cells continue to pose a significant barrier to commercialization. A new generation of two-dimensional (2D) and quasi-2D perovskites and newly introduced members of the 2D material family, have attracted growing attention due to their excellent stability and physical properties in contrast to their three-dimensional (3D) counterparts. Herein, we have presented the feasibility of using 4,4-dipyridyl as an additive material for quasi-2D perovskite solar cells. As a result of the addition of 4,4-dipyridyl, the solar cell device achieves a power conversion efficiency of 17.92% and a fill factor of 76.5%. Additionally, this strategy can be expanded to quasi-2D perovskite solar cells with an open-circuit voltage of 1.05V.

由于包晶体太阳能电池具有出色的光电特性和较低的制造成本,因此吸引了广泛的研究关注。尽管如此,与过氧化物太阳能电池相关的长期稳定性问题仍然是实现商业化的一大障碍。新一代二维(2D)和准 2D 包晶石以及新引入的 2D 材料家族成员,因其与三维(3D)材料相比具有优异的稳定性和物理性能而日益受到关注。在此,我们介绍了使用 4,4′-二吡啶作为准二维包晶太阳能电池添加材料的可行性。由于添加了 4,4′-二吡啶基,太阳能电池装置的功率转换效率达到 17.92%,填充因子达到 76.5%。此外,这种策略还可扩展到开路电压为 1.05V 的准二维过氧化物太阳能电池。
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引用次数: 0
The wake characteristics and hydrodynamic forces of a near-wall circular cylinder with the splitter plate 带分流板的近壁圆筒的尾流特性和水动力
IF 1.9 4区 物理与天体物理 Q3 PHYSICS, APPLIED Pub Date : 2024-03-27 DOI: 10.1142/s0217984924503160
Yulu Liu, Yubing Li, Jianghua Li, Jiankang Zhou, Xiang Qiu
<p>Flow around a near-wall circular cylinder with the splitter plate is numerically performed at Reynolds number of 500, with the objective of investigating the wake characteristics and hydrodynamic forces. Five gap ratios <span><math altimg="eq-00001.gif" display="inline" overflow="scroll"><mi>G</mi><mo stretchy="false">∕</mo><mi>D</mi><mo>=</mo><mn>0</mn><mo>.</mo><mn>1</mn><mo>,</mo><mn>0</mn><mo>.</mo><mn>3</mn><mo>,</mo><mn>0</mn><mo>.</mo><mn>5</mn><mo>,</mo><mn>0</mn><mo>.</mo><mn>7</mn></math></span><span></span> and <span><math altimg="eq-00002.gif" display="inline" overflow="scroll"><mn>0</mn><mo>.</mo><mn>9</mn></math></span><span></span> (<i>G</i> is the gap between the lower surface of the cylinder and the wall, <i>D</i> is the diameter of the cylinder) are selected, and the splitter plate length <span><math altimg="eq-00003.gif" display="inline" overflow="scroll"><mi>L</mi><mo stretchy="false">∕</mo><mi>D</mi></math></span><span></span> ranges from 0 to <span><math altimg="eq-00004.gif" display="inline" overflow="scroll"><mn>4</mn><mo>.</mo><mn>5</mn></math></span><span></span>. The flow characteristics of an isolated cylinder with the splitter plate are investigated first for comparison, and four wake flow modes are observed, which include 2S mode (<span><math altimg="eq-00005.gif" display="inline" overflow="scroll"><mi>L</mi><mo stretchy="false">∕</mo><mi>D</mi><mo>≤</mo><mn>0</mn><mo>.</mo><mn>1</mn><mn>5</mn></math></span><span></span>), P+S mode (<span><math altimg="eq-00006.gif" display="inline" overflow="scroll"><mn>0</mn><mo>.</mo><mn>3</mn><mo>≤</mo><mi>L</mi><mo stretchy="false">∕</mo><mi>D</mi><mo>≤</mo><mn>1</mn><mo>.</mo><mn>0</mn></math></span><span></span>), 2S+S mode (<span><math altimg="eq-00007.gif" display="inline" overflow="scroll"><mn>1</mn><mo>.</mo><mn>2</mn><mn>5</mn><mo>≤</mo><mi>L</mi><mo stretchy="false">∕</mo><mi>D</mi><mo>≤</mo><mn>2</mn><mo>.</mo><mn>0</mn></math></span><span></span>) and 2P mode (<span><math altimg="eq-00008.gif" display="inline" overflow="scroll"><mi>L</mi><mo stretchy="false">∕</mo><mi>D</mi><mo>≥</mo><mn>3</mn><mo>.</mo><mn>0</mn></math></span><span></span>). As <span><math altimg="eq-00009.gif" display="inline" overflow="scroll"><mi>L</mi><mo stretchy="false">∕</mo><mi>D</mi></math></span><span></span> increases from 0 to <span><math altimg="eq-00010.gif" display="inline" overflow="scroll"><mn>0</mn><mo>.</mo><mn>7</mn><mn>5</mn></math></span><span></span>, the mean drag coefficient (<span><math altimg="eq-00011.gif" display="inline" overflow="scroll"><mover accent="true"><mrow><msub><mrow><mi>C</mi></mrow><mrow><mi>D</mi></mrow></msub></mrow><mo accent="true">¯</mo></mover></math></span><span></span>) is decreased, and there is a slight increase of <span><math altimg="eq-00012.gif" display="inline" overflow="scroll"><mover accent="true"><mrow><msub><mrow><mi>C</mi></mrow><mrow><mi>D</mi></mrow></msub></mrow><mo accent="true">¯</mo></mover></math></span><span></span> for <span><mat
在雷诺数为 500 的条件下,对带分流板的近壁圆形气缸周围的流动进行了数值计算,目的是研究尾流特征和流体动力。选择了五个间隙比 G∕D=0.1、0.3、0.5、0.7 和 0.9(G 为圆柱体下表面与壁面之间的间隙,D 为圆柱体直径),分流板长度 L∕D 为 0 至 4.5。首先对比研究了带分流板的孤立圆柱体的流动特性,观察到四种唤醒流动模式,包括 2S 模式(L∕D≤0.15)、P+S 模式(0.3≤L∕D≤1.0)、2S+S 模式(1.25≤L∕D≤2.0)和 2P 模式(L∕D≥3.0)。当 L∕D 从 0 增加到 0.75 时,平均阻力系数(CD¯)减小,当 0.75<L∕D≤1.25 时,CD¯略有增加。此外,在 L∕D=0.75 和 L∕D=1.0 的情况下,阻力有非常明显的降低,CD¯ 分别降低了 39% 和 38%。详细研究了带有分流板的近壁气缸的湍流特性和流体动力,观察到五种湍流状态,包括湍流涡合并状态 I、合并涡附着状态 II、稳定流状态 III、壁面剪切层伸长状态 IV 和上剪切层附着状态 V。当 G∕D≥0.3 时,随着 L∕D 从 0 增加到 1.0,斯特劳哈尔数(St)减小,当 L∕D=1.25 时,斯特劳哈尔数增大。在 L∕D≥1.25 时,近壁圆柱体的 St 比孤立圆柱体的大,St 的增大受到偏转间隙流的影响。此外,流体动力学特性也受到壁面的影响。当 G∕D>0.1 时,CD¯ 随 L∕D 的变化与孤立圆柱体相似。研究发现,当 G∕D>0.3 时,L∕D=0.75 和 L∕D=1.0 的情况下仍能显著降低阻力,并且随着 G∕D 的增大,所有 L∕D 的情况下 CD¯ 都会增大。
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Five gap ratios &lt;span&gt;&lt;math altimg=\"eq-00001.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;mi&gt;G&lt;/mi&gt;&lt;mo stretchy=\"false\"&gt;∕&lt;/mo&gt;&lt;mi&gt;D&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;5&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;7&lt;/mn&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt; and &lt;span&gt;&lt;math altimg=\"eq-00002.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;9&lt;/mn&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt; (&lt;i&gt;G&lt;/i&gt; is the gap between the lower surface of the cylinder and the wall, &lt;i&gt;D&lt;/i&gt; is the diameter of the cylinder) are selected, and the splitter plate length &lt;span&gt;&lt;math altimg=\"eq-00003.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;mi&gt;L&lt;/mi&gt;&lt;mo stretchy=\"false\"&gt;∕&lt;/mo&gt;&lt;mi&gt;D&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt; ranges from 0 to &lt;span&gt;&lt;math altimg=\"eq-00004.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;mn&gt;4&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;5&lt;/mn&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;. The flow characteristics of an isolated cylinder with the splitter plate are investigated first for comparison, and four wake flow modes are observed, which include 2S mode (&lt;span&gt;&lt;math altimg=\"eq-00005.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;mi&gt;L&lt;/mi&gt;&lt;mo stretchy=\"false\"&gt;∕&lt;/mo&gt;&lt;mi&gt;D&lt;/mi&gt;&lt;mo&gt;≤&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mn&gt;5&lt;/mn&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;), P+S mode (&lt;span&gt;&lt;math altimg=\"eq-00006.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;mo&gt;≤&lt;/mo&gt;&lt;mi&gt;L&lt;/mi&gt;&lt;mo stretchy=\"false\"&gt;∕&lt;/mo&gt;&lt;mi&gt;D&lt;/mi&gt;&lt;mo&gt;≤&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;), 2S+S mode (&lt;span&gt;&lt;math altimg=\"eq-00007.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mn&gt;5&lt;/mn&gt;&lt;mo&gt;≤&lt;/mo&gt;&lt;mi&gt;L&lt;/mi&gt;&lt;mo stretchy=\"false\"&gt;∕&lt;/mo&gt;&lt;mi&gt;D&lt;/mi&gt;&lt;mo&gt;≤&lt;/mo&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;) and 2P mode (&lt;span&gt;&lt;math altimg=\"eq-00008.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;mi&gt;L&lt;/mi&gt;&lt;mo stretchy=\"false\"&gt;∕&lt;/mo&gt;&lt;mi&gt;D&lt;/mi&gt;&lt;mo&gt;≥&lt;/mo&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;). As &lt;span&gt;&lt;math altimg=\"eq-00009.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;mi&gt;L&lt;/mi&gt;&lt;mo stretchy=\"false\"&gt;∕&lt;/mo&gt;&lt;mi&gt;D&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt; increases from 0 to &lt;span&gt;&lt;math altimg=\"eq-00010.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;7&lt;/mn&gt;&lt;mn&gt;5&lt;/mn&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;, the mean drag coefficient (&lt;span&gt;&lt;math altimg=\"eq-00011.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;mover accent=\"true\"&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;C&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;D&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/mrow&gt;&lt;mo accent=\"true\"&gt;¯&lt;/mo&gt;&lt;/mover&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;) is decreased, and there is a slight increase of &lt;span&gt;&lt;math altimg=\"eq-00012.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;mover accent=\"true\"&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;C&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;D&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/mrow&gt;&lt;mo accent=\"true\"&gt;¯&lt;/mo&gt;&lt;/mover&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt; for &lt;span&gt;&lt;mat","PeriodicalId":18570,"journal":{"name":"Modern Physics Letters B","volume":"53 1","pages":""},"PeriodicalIF":1.9,"publicationDate":"2024-03-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140317036","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
New analytical solutions to the nonlinear Schrödinger equation via an improved Cham method in conformable operator 通过保角算子中的改进查姆法求得非线性薛定谔方程的新解析解
IF 1.9 4区 物理与天体物理 Q3 PHYSICS, APPLIED Pub Date : 2024-03-27 DOI: 10.1142/s0217984924503275
Boubekeur Gasmi, Lama Alhakim, Yazid Mati, Alaaeddin Moussa, Haci Mehmet Baskonus

This paper presents an improved Cham method as an efficient technique for obtaining analytical exact solutions to nonlinear partial differential equations. We apply this method to solve the nonlinear Schrödinger equation in conformable operator, a challenging equation frequently used in various scientific fields. The method enables us to derive different traveling wave solutions, such as kink, coindal waves, breather waves, periodic singular solutions, and periodic multi-wave solitons. We also provide graphical representations of some of the obtained solutions to help understand their dynamic characteristics. These results highlight the effectiveness and adaptability of the method and demonstrate its potential to solve other partial differential equations.

本文提出了一种改进的 Cham 方法,作为获得非线性偏微分方程解析精确解的有效技术。我们将该方法应用于求解保角算子中的非线性薛定谔方程,这是一个经常用于各种科学领域的具有挑战性的方程。该方法使我们能够推导出不同的行波解,如扭结波、共振波、呼吸波、周期奇异解和周期多波孤子。我们还提供了一些所得解的图示,以帮助理解它们的动态特性。这些结果凸显了该方法的有效性和适应性,并证明了它在求解其他偏微分方程方面的潜力。
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引用次数: 0
Electrically conducting mixed convective nanofluid flow past a nonlinearly slender Riga plate subjected to viscous dissipation and activation energy 受粘性耗散和活化能影响的非线性细长里加板上的导电混合对流纳米流体流动
IF 1.9 4区 物理与天体物理 Q3 PHYSICS, APPLIED Pub Date : 2024-03-27 DOI: 10.1142/s0217984924503366
Bilal Ali, Sidra Jubair, Zafar Mahmood*, Md Irfanul Haque Siddiqui

This paper reports the mass and energy transmission characteristics of an electrically conducting mixed convective nanofluid flow past a stretching Riga plate. An additional effect of viscous dissipation, Arrhenius activation energy and heat source is also studied. The energy and mass transmissions are evaluated by a zero-mass flux of nanoparticle and convective boundary conditions. Buongiorno’s relations are proposed for the Brownian motion and thermophoretic diffusion. The similarity substitutions are employed to derive the non-dimensional set of modeled equations. The obtained set of equations is numerically processed via parametric continuation method (PCM). Several flow factors affecting the velocity, energy, and mass distributions are graphically discussed. It has been perceived that the fluid velocity field declines with the influence of velocity power index (m), while improves with the upshot of modified Hartmann number (Q). The effect of Schmidt number and chemical reaction diminishes the concentration profile φ(η). Furthermore, the energy curve enhances with the effect of thermophoresis factor, Biot and Eckert number.

本文报告了导电混合对流纳米流体流经拉伸里加板时的质量和能量传输特性。此外,还研究了粘性耗散、阿伦尼乌斯活化能和热源的额外影响。通过纳米粒子的零质量通量和对流边界条件对能量和质量传输进行了评估。提出了布朗运动和热泳扩散的 Buongiorno 关系。利用相似性替换法推导出非线性方程组。得到的方程组通过参数延续法(PCM)进行数值处理。对影响速度、能量和质量分布的几个流动因素进行了图解讨论。研究发现,流体速度场随着速度功率指数(m)的影响而减小,而随着修正哈特曼数(Q)的增加而增大。施密特数和化学反应的影响减小了浓度曲线 φ(η)。此外,能量曲线会随着热泳系数、毕奥特数和埃克特数的影响而增强。
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引用次数: 0
On the rising dynamics of a Taylor bubble in sudden/gradual expansion tubes filled with viscoelastic liquids 关于充满粘弹性液体的突然/逐渐膨胀管中泰勒气泡的上升动力学
IF 1.9 4区 物理与天体物理 Q3 PHYSICS, APPLIED Pub Date : 2024-03-27 DOI: 10.1142/s0217984924503287
Yunsong Li, Qixin Ba, Wenjun Yuan, Mei Mei, Jia Zhang

In this paper, the rise behaviors of Taylor bubbles are investigated in sudden/gradual tubes filled with viscoelastic media via grid adaptive direct numerical simulations (DNS). The exponential Phan–Thien–Tanner (PTT) constitutive model is used to describe the viscoelastic rheological characteristics, and the phase interface is captured via the volume of fluid (VOF) method. The effects of tube structure (diameter ratio and structural angle) and fluid elasticity (expressed by the Weissenberg number Wi) on bubble dynamics have been studied. Our results indicate that bubbles are prone to rupture in the expansion tubes, mainly due to the dual effects of the wall and the elastic relaxation. The fluid elasticity suppresses the jet effect in a sudden expansion tube. Meantime, as the structural angle or the diameter ratio increases, the wall effect is weakened on axial or radial scales, inhibiting the bubble rupture. A large structure angle attenuates the wall effect, while changes in the diameter ratio slow down the radial momentum transfer near the wall region, both of which favor bubble integrity. We also obtain an exponential relationship between the critical rupture time and the structure angle. The dynamical Taylor bubbles can be operated by the structure of the tube and surrounding fluid viscoelasticity, which is of great significance in chemical engineering applications involving complex non-Newtonian fluids.

本文通过网格自适应直接数值模拟(DNS)研究了泰勒气泡在充满粘弹性介质的突变/渐变管中的上升行为。采用指数 Phan-Thien-Tanner (PTT) 构成模型描述粘弹性流变特性,并通过流体体积 (VOF) 方法捕捉相界面。研究了管道结构(直径比和结构角)和流体弹性(用魏森伯格数 Wi 表示)对气泡动力学的影响。研究结果表明,气泡在膨胀管中容易破裂,主要是由于管壁和弹性松弛的双重影响。流体弹性抑制了突然膨胀管中的喷射效应。同时,随着结构角或直径比的增大,壁面效应在轴向或径向尺度上减弱,从而抑制气泡破裂。较大的结构角会减弱管壁效应,而直径比的变化则会减缓管壁区域附近的径向动量传递,这两者都有利于气泡的完整性。我们还得到了临界破裂时间与结构角之间的指数关系。动态泰勒气泡可以通过管的结构和周围流体的粘弹性来操作,这在涉及复杂非牛顿流体的化学工程应用中具有重要意义。
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引用次数: 0
Four-component combined integrable equations possessing bi-Hamiltonian formulations 具有双哈密顿公式的四分量组合可积分方程
IF 1.9 4区 物理与天体物理 Q3 PHYSICS, APPLIED Pub Date : 2024-03-27 DOI: 10.1142/s0217984924503196
Wen-Xiu Ma

This paper aims to generate a Liouville integrable Hamiltonian hierarchy by introducing a specific matrix eigenvalue problem with four components. The adopted approach is the zero curvature formulation. A bi-Hamiltonian formulation is furnished through applying the trace identity, which shows the Liouville integrability of the resulting hierarchy. Two examples of generalized combined nonlinear Schrödinger equations and modified Korteweg–de Vries equations are presented.

本文旨在通过引入一个包含四个组成部分的特定矩阵特征值问题,生成一个 Liouville 可积分哈密顿层次结构。采用的方法是零曲率公式。通过应用迹特征,本文提出了一种双哈密顿形式,这显示了所产生的层次结构的Liouville可积分性。此外,还介绍了两个广义组合非线性薛定谔方程和修正的 Korteweg-de Vries 方程的例子。
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引用次数: 0
Hybrid nanofluid flow and heat transfer in symmetric porous ducts with CuO nanoparticles and multi-walled carbon nanotubes under peristaltic motion CuO纳米颗粒和多壁碳纳米管在对称多孔管道中的混合纳米流体在蠕动运动下的流动和传热
IF 1.9 4区 物理与天体物理 Q3 PHYSICS, APPLIED Pub Date : 2024-03-27 DOI: 10.1142/s0217984924503330
Noreen Sher Akbar, Javaria Akram, M. Fiaz Hussain, E. N. Maraj, Taseer Muhammad

This study focuses on the analysis of peristaltic transport of a hybrid nanofluid comprising deionized water as a base fluid and the multi-walled carbon nanotubes (MWCNTs) and copper oxide (CuO) as nanoparticles within a sinusoidal wavy porous duct, taking into consideration the influence of heat generation or absorption. The inaugural literature piece addresses the utilization of hybrid nanofluid in the context of peristaltic flow within ducts. To simplify the analysis, we have converted the non-dimensional equations into a two-dimensional (2D) coordinate system using the assumptions of a very long wavelength (δ<1) and low Reynolds number (Re). The non-dimensional equations governing the behavior of the hybrid nanofluid are then solved numerically using the finite volume method. Numerical solutions for temperature and the 2D peristaltic flow are obtained with the assistance of the Mathematics software MATLAB. These solutions are subsequently represented graphically using MATLAB software. The graphical results highlight several key findings for important parameters. First, it is observed that the pressure rise, temperature profile, and pressure gradient in the hybrid nanofluid (CuMWCNTs/H2O) flow increases as heat generation increases. Furthermore, an increase in the nanoparticle volume fraction of both nanoparticles leads to a decrease in the pressure rise and pressure gradient in the hybrid nanofluid flow. Additionally, the widening of the channel reduces the pressure gradient and pressure rise in the CuMWCNTs/H2O hybrid nanofluid. The analysis also includes the visualization of streamlines for peristaltic transport. These streamlines reveal that an increase in amplitude results in larger bolus sizes, while heightened heat generation has the opposite effect, decreasing bolus sizes. The results of this investigation can be found in various cooling devices as flows in the ducts are very frequently utilized for the cooling process of engines. A further topic is common in applications related to microfluidics, heat exchangers, and biomedical devices where peristaltic pumping is employed. Our results are in 100% agreement with the existing literature in special cases.

本研究重点分析了以去离子水为基础流体,以多壁碳纳米管(MWCNTs)和氧化铜(CuO)为纳米颗粒的混合纳米流体在正弦波形多孔管道内的蠕动传输,同时考虑了热量产生或吸收的影响。首篇文献探讨了在管道内蠕动流的背景下利用混合纳米流体的问题。为了简化分析,我们使用超长波长(δ<1)和低雷诺数(Re)假设,将非一维方程转换为二维(2D)坐标系。然后使用有限体积法对控制混合纳米流体行为的非二维方程进行数值求解。在数学软件 MATLAB 的帮助下,获得了温度和二维蠕动流的数值解。随后使用 MATLAB 软件以图形表示这些解。图形结果突出了重要参数的几个关键发现。首先,可以观察到混合纳米流体(CuMWCNTs/H2O)流动中的压力上升、温度曲线和压力梯度随着发热量的增加而增大。此外,两种纳米粒子体积分数的增加会导致混合纳米流体中的压力上升和压力梯度下降。此外,通道的拓宽也降低了 CuMWCNTs/H2O 混合纳米流体中的压力梯度和压力上升。分析还包括蠕动输送流线的可视化。这些流线显示,振幅的增加会导致栓塞尺寸增大,而热量产生的增加则会产生相反的效果,使栓塞尺寸减小。这项研究的结果可以在各种冷却设备中找到,因为管道中的流动经常被用于发动机的冷却过程。此外,在与微流控、热交换器和生物医学设备相关的应用中,蠕动泵的使用也是一个常见的话题。在特殊情况下,我们的研究结果与现有文献100%一致。
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引用次数: 0
Heat generation effects on the MHD Nimonic 80A-Fe3O4 water hybrid nanofluid flow over a wedge with influence of shape factor of nanoparticles 纳米颗粒形状因子对楔形上 MHD Nimonic 80A-Fe3O4 水混合纳米流体流动的发热效应的影响
IF 1.9 4区 物理与天体物理 Q3 PHYSICS, APPLIED Pub Date : 2024-03-27 DOI: 10.1142/s0217984924502919
Anomitra Chakraborty, Pranitha Janapatla

This study reports both MagnetoHydroDynamics (MHD) and heat generation aspects of a water-based hybrid nanofluid flow with various shapes of the nanoparticles involving Nimonic 80A and Fe3O4, over a moving wedge. Similarity transformations were adapted to obtain non-dimensional equations and solved using MATLAB bvp4c code. All the results and graphs were formulated after a positive outcome of our results with that available in existing literature. Nusselt number, which signifies the heat transfer rate in a flow, increased with an increase in empirical shape factors of the nanoparticle with a contrasting decrease in the drag experienced during the flow, represented by the skin friction coefficient. The velocity profile decreased at a rate of 0.75% for M=0.6 to M=0.8 due to the augmenting Lorentz forces while it augmented by 18.9% for an augmenting velocity ratio parameter from R=0.0 to R=0.5 due to the no-slip boundary conditions. Both the Nusselt number and skin friction coefficients decreased with an increase in magnetic parameter. An increase in the nanoparticle concentration resulted in an incrementing streamline value along with increasing temperature profile due to increasing thermal conductivity of the fluid flow system. The physical significance of the study involves in its applications in nuclear, steel industries, MRI scanning for its anti-corrosive and high thermal conductivity properties.

本研究报告了在移动楔形体上的水基混合纳米流体流动的磁流体动力学(MHD)和发热方面的情况,该流体中的纳米粒子形状各异,包括 Nimonic 80A 和 Fe3O4。通过相似变换获得了非一维方程,并使用 MATLAB bvp4c 代码进行了求解。所有结果和图表都是在我们的结果与现有文献中的结果相比较后得出的。表示流动中热传导率的努塞尔特数随着纳米粒子经验形状系数的增加而增加,而流动过程中的阻力(以表皮摩擦系数表示)则相反地减小。由于洛伦兹力的增强,M=0.6 到 M=0.8 的速度曲线下降了 0.75%,而由于无滑动边界条件,R=0.0 到 R=0.5 的增强速度比参数则增加了 18.9%。随着磁性参数的增加,努塞尔特数和皮肤摩擦系数都有所下降。由于流体流动系统的热导率增加,纳米粒子浓度的增加导致流线值增加,温度曲线也随之增加。这项研究的物理意义在于其抗腐蚀和高导热性能在核工业、钢铁工业和核磁共振扫描中的应用。
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引用次数: 0
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Modern Physics Letters B
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