MA3233 AY06-07 Sem 1
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山西医科大学学报,2021年5月,第52卷第5期-697•SematD:在自身免疫性和感染性疾病中的一种新型免疫调节剂刘亨晶02,曹莉婷、,,温雪、,,于晓辉、*,张久聪0(中国人民解放军联勤保障部队第九四o医院消化内科,兰州734050;7甘肃中医药大学临床医学院;8宁夏医科大学临床医学院;*通讯作者,E-ma/:******************;^同通讯作者,£-]68匚1:20811/40117@)关键词:SemabD;自身免疫性疾病;感染性疾病中图分类号:R392文献标志码:A文章编号:1067-6712(2722)65-0757-65DOI:16.4753/P issu.1067-6612.2622.65.622SemaphoPn是一个分泌型和膜结合蛋白的大家族,具有高度保守的520个氨基酸的信号结构域,根据结构属性分为5类,最早作为轴突导向在神经元发育中发挥关键作用,近年来因其在免疫系统中的功能受到越来越多的关注。
SemaphoPnUD(SemabD,又称CD102-是SemaphoPn家族中的第IV类信号素,通过与其受体Plexin-Pl和CD77相互作用,在T 细胞的活化、抗体的产生和免疫调节过程中发挥着重要作用。
许多研究报道SemabD在自身免疫性和感染性疾病患者中表达异常,并且与病情严重程度密切相关[2],成为目前研究的热点,因此本文就相关研究进行简要综述。
0Sema4D的结构、表达和受体SemabD是一类跨膜糖蛋白,分子量为150kD,由862个氨基酸组成,其分子结构包括Sema结构域、免疫球蛋白结构域、疏水性跨膜区和细胞质尾部⑶o SemabD在人体中分布广泛,神经系统中主要分布在脑和周围神经系统以及淋巴组织中,在静止的T细胞上表达丰富,其表达随T细胞的活化上调,B 细胞和树突状细胞等抗原提呈细胞上表达微弱,血小板、粒细胞等也存在其表达。
S e m a pD主要以膜结合型和可溶型两种形式存在,都具有生物活性,当免疫细胞激活时,细胞膜上Semab D的表达增强,随后导致某些基质金属蛋白酶(mat/x metahop/teinusa, MMPs)在细胞膜附近聚集诱导Semab D胞外结构域的脱落,产生02kD生物活性可溶性的SemabD (soludic SemabD,s Sema4D)。
第3期闫志航,等:电脉冲轧制6061Al电热耦合模型及电弧加热机理分析(0)为热源中心的最大通量(单位:W/m2);C为浓度系数(单位:m-2);r为距热源中心的径向距离(单位:m)。
q=k×S×¶∆T¶d(16)式中 k是导热系数;S是接触面积;d是导热距离;∆T是温差。
高斯热源的一个变体使用以下方程拟合得到图6e的热源方程。
q(r)=qmax×e(-(a×x2+b×z2))(17)拟合结果a=31.20,b=10.90。
使用Gauss2D方程拟合图6h的热源方程:q=qmax ×e()-0.5×()x-xc w12-0.5×()y-yc w22+c(18)式中 x c=0,y c=0,w1=w2=0.05,c=35.04。
3 结论(1)当加载800 A的电流时,电脉冲辅助轧制工艺可以在两板的界面处产生温度为4 000 K或更高的电弧,但这不是稳定的焊接电弧,而是瞬时电弧,可用于铝合金板材的瞬时加热及氧化膜的去除。
当加载更高的电流时,会产生更高温度的电弧。
(2)电脉冲辅助轧制后板材表面可以形成焊点,结合本研究的模拟可得出,加载高频电流时两板间可以达到产生电弧的条件,且电弧首次产生的时间为1/4个脉冲周期,电弧呈现椭圆凹形,由上下凸起之间的间距和曲率确定。
加载更高频率的脉冲电流可以使一定时间内产生的电弧数量增加,即加热次数更多。
(3)采用切片法分别对两个方向的热源进行拟合,得到了有效的热源拟合方程。
电弧的产生也为电脉冲辅助轧制提供了新的研究方向。
参考文献:[1] Roh J H, Seo J J, Hong S T,et al. The mechanical be‐havior of 5052-H32 aluminum alloys under a pulsedelectric current[J]. International Journal of Plasticity,2014,58:84-99.[2] Wang X,Xu J,Shan D, et al. Modeling of thermal and mechanical behavior of a magnesium alloy AZ31 dur‐ing electrically-assisted micro-tension[J].InternationalJournal of Plasticity,2016,85:230-257.[3] Ren X W,Wang Z J,Fang X,et al. The plastic flowmodel in the healing process of internal microcracks inpre-deformed TC4 sheet by pulse current[J]. Materials& Design,2020,188:108428.[4] Rahnama A,Qin R. Room temperature texturing of aus‐tenite/ferrite steel by electropulsing[J]. Scientific Re‐ports,2017,7:42732.[5] Zhang X, Li H, Zhan M, et al. Extraordinary effect of the δ phase on the electrically-assisted deformation re‐sponses of a Ni-based superalloy[J]. Materials Charac‐terization,2018,144:597-604.[6] Li D,Yu E,Liu Z. Microscopic mechanism and nu‐merical calculation of electroplastic effect on metal'sflow stress[J]. Materials Science and Engineering: A,2013,580:410-413.[7] Zhang X,Li H,Zhan M, et al. Electron force-induced dislocations annihilation and regeneration of a superal‐loy through electrical in-situ transmission electron mi‐croscopy observations[J]. Journal of Materials Science& Technology,2020,36:79-83.[8] Molotskii M, Fleurov V V. Magnetic effects in electro‐plasticity of metals[J]. Phys Rev B Condens Matter,1995,52(22):15829-15834.[9] Kim M J, Yoon S, Park S, et al. Elucidating the origin of electroplasticity in metallic materials[J]. AppliedMaterials Today,2020,21:100874.[10] Yang X D, Li X H, Li Q. Discharge crater formation simulation coupled by thermo-fluid analysis of arcplasma in EDM[J]. Procedia CIRP,2020,95:232-237.[11] Guan C, Ding J, Yao X, et al. Study on Short-circuit current interruption characteristics of Double-breakfast vacuum circuit breaker within the minimum arcingtime[J]. International Journal of Electrical Power &Energy Systems, 2023,147:108865.[12] Wu H, Chang Y, Guan Z, et al. Arc shape and micro‐structural analysis of TIG welding with an alternatingcusp-shaped magnetic field[J]. Journal of MaterialsProcessing Technology, 2021,289:116912.[13] Wang B, Zhu D, Ding R, et al. Simulation of arc cra‐ter formation and evolution on plasma facing materials[J]. Nuclear Materials and Energy,2021,27:100964.[14] Zhao S, Zhang C, Zhang Y, et al. Influence of Partial Arc on Electric Field Distribution of Insulator Stringsfor Electrified Railway Catenary[J]. Energies,2019,12(17), 3295.编辑部网址:http://29Electric Welding MachineVol.54 No.3Mar. 2024第 54 卷 第 3 期2024 年3 月热处理对激光选区熔化制备CX 不锈钢微观组织与性能的影响陈锦伊1, 陈信豪1, 马晶晶1, 张可召1*, 冯时2, 严春妍1, 包晔峰11.河海大学 机电工程学院,江苏 常州 2130222.江苏柏灵激光智能设备有限公司,江苏 常州 213022摘 要:采用激光选区熔化技术(SLM )制备了CX 不锈钢(Corrax Stainless Steel ),并对沉积态、固溶态、固溶时效态三种条件下的CX 不锈钢进行显微组织分析和室温拉伸性能测试。
SCM7B32/33隔离过程电流/电压输入模块说明SCM7B32 电流输入模块从现场接受4-20mA或0-20mA范围的输入信号并向过程控制系统提供高电平输出(图1)。
电流与电压的转换在模块内部发生,该模块经工厂校准以保证最高的精度。
SCM7B33 电压输入模块从现场接受+1V -+5V和0-+5V范围的输入信号,并向过程控制系统提供高电平输出。
作为替代方案,SCM7B33可以与外部 250Ω电阻器 (Dataforth SCM7BXR1 或同类元件)一起使用,接受4-20mA 或0-20mA范围的输入信号。
使用外部感测电阻可以在不中断电流回路情况下拆除模块。
所有SCM7B33s 都装有SCM7BXR1电阻器出厂。
这些模块整合了五极滤波法,通过吸取Thomson (Bessel)和But-terworth两种特性的优点,使时间和频率的响应达到最大。
滤波器的一极在隔离安全栅的现场一侧,另外四极在过程控制一侧。
在现场侧初步滤波之后(转换-仅SCM7B32),输入信号由专用的斩波电路斩波处理,并在变压器隔离安全栅的两端传送,抑制共模尖脉冲和电涌的传输,然后信号经再建和滤波供过程控制系统输出。
模块接受14 - 35VDC宽范围电源 (标称+24VDC )。
它们紧凑的包装(2.13”x1.705”x0.605” 最大)节省了空间,对高通道密度的应用十分理想。
它们可以使用任何一种“-DIN”后面板的设计,采用DIN 轨条安装十分方便。
Figure 1: SCM7B32/33 Block Diagram s特性• 接受电流或电压输入。
• 提供高电平电压输出。
• 1500Vrms 变压器隔离• 精度, ±0.03% of 量程典型,±0.1% 最大• ANSI/IEEE C37.90.1 瞬变保护• 120Vrms 以内连续输入保护• 噪声, 500µV 峰值 (5MHz), 300µV RMS (100kHz)• CMRR, 达 105dB• 100Hz以上每10倍频程衰减80dB • 容易 DIN 轨条安装• 经CSA 认证, FM 批准• 符合CE 和 ATEX 规定For information call 800-444-7644 70Visit our website 71S C M 7B技术规范典型在 25°C 和 +24VDC模块SCM7B32SCM7B33输入信号范围 4-20mA, 0-20mA+1 to +5V , 0 至 +5V偏置电流 N/A±0.1nA电阻 正常 <100Ω 2M Ω 断电 <100Ω 2M Ω 过载 30k Ω2M Ω 保护 连续 120Vrms 最大 * 瞬变 ANSI/IEEE C37.90.1*输出信号范围(1) ††有效可用功率(1) 40mW * 电阻 <1Ω* 保护连续对地短路 * 电压/电流 极限 ±12V, ±14mA*CMV (输入-至-输出) 连续 1500Vrms* 瞬变ANSI/IEEE C37.90.1*CMRR (50或60Hz)105dB *精度(2) ±0.03% 量程 典型, *±0.1% 量程 最大非线性(3) ±0.01% 量程 典型, *±0.02% 量程 最大稳定性 (-40°C 至 +85°C) 增益 ±35ppm/°C * 输入偏移 N/A (4)* 输出偏移 ±0.003% 量程/°C*噪声在 5MHz 带宽峰值500µV * 在10Hz 至 100kHz 带宽RMS 300µV * 在 0.1Hz 至10Hz 带宽峰值 1µV RTI*频率和时间响应 带宽, -3dB100Hz* NMR (-3dB 在 100Hz) 100Hz 以上每10倍频程80dB* 阶跃响应, 90% 量程 5ms*电源电压 14 to 35VDC* 电流(1) 12mA * 灵敏度 ±0.0001%/%V S*机械尺寸 2.13” x 1.705” x 0.605” 最大 * (高)(宽)(深)54.1mm x 43.3mm x 15.4mm 最大*环境工作温度范围-40°C 至 +85°C * ATEX 组 II, 类别 3 -20°C 至+40°C * 存放温度范围 -40°C 至 +85°C * 相对湿度0 to 95% 无凝露*发射 EN61000-6-4 ISM, 组 1 * 辐射, 传导类 A *抗扰性 EN61000-6-2 ISM, 组 1* RF性能 A ±0.5% 量程误差* ESD, EFT, 电涌,电压骤降性能 B*注解:*技术规范与以前的型号相同(1) 输出范围和电源电流技术规范根据最小输出负载电阻。
2021年第6期广东化工第48卷总第440期 · 1 ·溶胶凝胶法制备二硫化钼干凝胶复合电极和电化学性能表征简旻坤(厦门理工学院材料科学与工程学院,福建厦门361024)[摘要]通过溶胶凝胶法在泡沫镍表面滴涂二硫化钼干凝胶复合材料来制备析氢电极。
通过改变不同的溶液配比来改变复合材料的形貌和结构,利用泡沫镍和复合材料的高催化性、高比表面积和高电导性的特性,研究不同形貌和结构的复合电极对析氢效果的影响。
运用多种分析测试技术对制备的复合材料进行表征,并通过电化学方法对复合电极的析氢性能进行研究,研究表明当0.01 mol·L-1钼酸钠-0.4 mol·L-1硫脲配比溶液在水热反应下生成二硫化钼,然后通过溶胶凝胶法制备二硫化钼无机干凝胶滴涂在泡沫镍表面,复合材料的电催化析氢性能最好。
[关键词]泡沫镍;二硫化钼;无机干凝胶;析氢反应[中图分类号]TQ [文献标识码]A [文章编号]1007-1865(2021)06-0001-02Preparation and Hydrogen Evolution Performance of MoS2 Combination Electrodeby Sol-gel ProcessJian Minkun(School of Materials Science and Engineering Xiamen University of Technology, Xiamen 361024, China) Abstract:Hydrogen evolution electrode was produced by MoS2inorganic xerogel on nickel foam by sol-gel process. The morphology and structure of combination electrode was controlled by changing the solution proportioning. The high catalytic activity, high specific surface area, and high electrical conductivity have advantage for the combination electrode, we have investigated the electrocatalytic activity with different morphologies and structures for hydrogen evolution reaction (HER). The research show that MoS2 prepared by 0.01 mol/L sodium molybdate -0.4 mol/L thiourea through the hydrothermal reaction, than produce the MoS2 inorganic xerogel to drop on the nickel foam, the combination electrode has the best electrocatalytic activity.Keywords: Nickel foam;MoS2;Inorganic xerogel;Hydrogen evolution reaction1 引言经济和科技的不断进步为人类社会的发展提供动力,同时也带来了很多环境问题。
NATIONAL UNIVERSITY OF SINGAPOREMATHEMATICS SOCIETYPAST YEAR PAPER SOLUTIONSwith credits to Zheng ShaoxuanMA3233Algorithmic Graph TheoryAY2006/2007Sem1Question1(i).v1v2 v3 v4v5v6v7v8v9v10v11v12v13v14Tip:it is a good idea to count the cycles containing v10in a systemetic,categorised manner.One such way is to count the cycles via the cycle lengths.Furthermore,observe that the graph is bipartite since it admits a2-colouring.Hence,the only cycles that are possible within this graph are even cycles.By further observation we notice that there are no C12-s or C14-s possible in this graph of14vertices.Hence,we shall consider the four types of cycles:C4,C6,C8and C10.C4:v10v14v13v9v10,v10v12v11v9v10,v10v9v7v8v10.C6:v10v14v13v9v11v12v10,v10v14v13v9v7v8v10,v10v12v11v9v7v8v10,v10v9v7v5v6v8v10.C8:v10v14v13v9v7v5v6v8v10,v10v12v11v9v7v5v6v8v10,v10v9v7v5v1v2v6v8v10,v10v9v7v5v3v4v6v8v10.C10:v10v14v13v9v7v5v3v4v6v8v10,v10v14v13v9v7v5v1v2v6v8v10,v10v12v11v9v7v5v3v4v6v8v10,v10v12v11v9v7v5v1v2v6v8v10.(ii)As mentioned,G is bipartite and henceχ(G)=2.In particular,7of the14vertices of G has to be coloured‘1’and the other7is coloured‘2’(try it out!).For the graph H withχ(H)=2and witha maximum number of edges,H has to be a complete bipartite graph,and since G is a spanningsubgraph of H,H has two partite sets of7vertices each.Hence,by counting the number of edges in a complete bipartite graph as described,e(H)=7×7=49.(iii)Observe that,in particular,v1,v2,v3,and v4are vertices with degree2.As such,if G is hamiltonian, the edges v1v2,v2v6,v6v4,v4v3,v3v5,and v5v1must be in the resultant hamiltonian cycle since both edges incident to a vertex of degree2must be traversed.However,these6edges form a cycle by themselves,a contradiction!Hence G is not hamiltonian.(You can make a similar argument using v11,v12,v13and v14instead.)Wefind that1additional edge added to G is enough so that the resultant graph is hamiltonian,and hence the least number of new edges to be added to G is indeed1.One such edge is v1v12(there are other similar examples),and the resultant graph and hamiltonian cycle is as shown below:v1v2 v3 v4v5v6v7v8v9v10v11v12v13v14(iv)An eulerian graph is one that has all vertices with even degree.In the original G,only2vertices, v7and v8has odd degree;the rest have even degree.These two vertices are adjacent.For G to be eulerian alone,we can add one edge from v7to v8.However,the resultant graph becomesa multigraph which is not wanted.Hence one edge is not enough to satisfy the requirements asstated in the question.Consider adding two edges.To get rid of the odd degrees of v7and v8,and not to convert any other vertices to have odd degree,one edge must be incident to v7,one to v8,and both these edges must be incident to the same vertex at the other end.By symmetry we consider this other vertex to be only either v1or v5.If this vertex is v5,then the resultant graph becomes a multigraph which is not wanted.If this vertex is v1,then by a similar argument in(1iii)the graph is not hamiltonian (there exists certain edges which must be included in the hamiltonian cycle,which forms a cycle by itself).Hence two edges is not sufficient to satisfy the requirements as stated in the question.Three edges is sufficient to do so,and hence three is the least number of new edges to be added.One way to do so(again there are other ways)is the addition of v1v7,v8v12and v1v12.The resultant graph,with all vertices of even degree,and the hamiltonian cycle is shown below:v1v2 v3 v4v5v6v7v8v9v10v11v12v13v14(v)A spanning tree of G with greatest possible number of cut-vertices is one which has least number of end-vertices.If possible,we try to construct a path which is a spanning tree of G as a path has only2end-vertices,the least possible in any non-trivial graph.Wefind that a spanning path is possible!Since we only require1additional edge in G to form a hamiltonian cycle,there already exists a hamiltonian/spanning path in G.Hence we use the same spanning path as discovered earlier in(1iii)as our desired spanning tree,minus the extra edge v1v12,as shown belowv 1v 2v 3v 4v 5v 6v 7v 8v 9v 10v 11v 12v 13v 14Question 2Define thefollowing graphs as follow:GG 1G 2By considering the removal of the highlighted edge of G ,τ(G )=τ(G 1)+τ(G 2).Hence it suffices to find the number of spanning trees of the two latter graphs.τ(G 2)can be (relatively)easily calculated with the mentioned edge removal method andsome simple manipulation as taught in MA3233.Define the following graphs as such:G 3G 4G5G6G7By considering two identical graphs sharing one single vertex,τ(G2)=(τ(G3))2.By considering the removal of the highlighted edge in G3,τ(G3)=τ(G4)+τ(G5).The highlighted edge in G4 makes no difference to the count of the number of spanning trees,henceτ(G4)=τ(G6).By considering two C3s sharing a common edge,τ(G6)=3×3−1=8.By considering the removal of the highlighted edge of G5,τ(G5)=τ(G6)+τ(G7).By considering two C2s(multigraph)sharing a single vertex,τ(G7)=2×2=4.Therefore,τ(G5)=8+4=12,τ(G4)=8,τ(G3)=8+12=20,and henceτ(G2)=202=400.You may attempt using a similar method tofindτ(G1)andfinally end up with an answer of320, but be warned that the process is extremely tedious and time consuming for this case.Owing to the symmetric nature of the graph,we may attempt using a combinatorial method tofindτ(G1) instead.Recolour the edges of G1as such:G1To count the number of spanning trees of G1,consider the3different and mutually exclusive types of spanning trees possible:(i)where both of the bolded black edges are within the spanning tree; (ii)where exactly one of the bolded black edges is within the spanning tree;(iii)where both the bolded black edges are NOT within the spanning tree.For(i),exactly5edges needs to be removed to form a spanning tree,one from each colour pair as well as one of the four uncoloured and unbolded edges.The number of ways to choose these5 edges is2×2×2×2×4=64.For(ii),wefirst realise there are2ways to choose which of the bolded black edges is to be removed. By symmetry,we only need to consider that the left bolded black edge is removed.4more edges needs to be removed after this:one from the green pair and one from the red pair.For the2 remaining edges to be removed to break all cycles in the graph,we could either do it by removing one from the blue pair and one from the yellow pair,or we could do it by removing one from the uncoloured unbolded edges and one from any of the blue or yellow edges.Hence,the number of ways to choose these edges to form a spanning tree is2(2×2)(2×2+4×4)=160.For (iii),after removing the 2black edges,we need to remove 3more edges such that all cycles are broken.One way to do so is to choose 3out of the 4colours,and remove 1edge from each of the 3colour pairs.The other way is to first remove 1of the 4unbolded uncoloured edges,then remove 1out of the 4blue or yellow edges to break the blue-yellow C 4as well as 1out of the 4green or red edges to break the green-red C 4.Take note that removing 2or more of the unbolded uncoloured edges disconnects the graph and hence we do not consider the cases for doing so.Hence,the number of ways to choose these edges to form a spanning tree is 43 ×2×2×2+4×4×4=96.By summing the results of the three cases,τ(G 1)=64+160+96=320.Therefore,the number of spanning trees of G ,τ(G )=320+400=720.Question 3v 1v 2v 3v 4v 5v 67v 8139451214596114549Apply Edmond’s algorithm to the above graph:There are 4odd vertices in the graph,v 1,v 2,v 3and v 4.The least weight and path of least weight between each pair of these vertices are:•v 1−v 2:13(via v 1v 2),•v 1−v 3:18(via v 1v 5v 6v 3),•v 1−v 4:15(via v 1v 5v 4),•v 2−v 3:14(via v 2v 7v 3),•v 2−v 4:19(via v 2v 7v 6v 5v 4),•v 3−v 4:14(via v 3v 4).The weights of the 3possible pairings between these 4vertices are:•v 1−v 2and v 3−v 4:13+14=27,•v 1−v 3and v 2−v 4:18+19=37,•v 1−v 4and v 2−v 3:15+14=29.The minimum weight pairing is v 1−v 2and v 3−v 4.We append the paths of least weights of the two paths within the minimum weight pairing into the original graph.We obtain:v 1v 2v 3v 4v 5v 6v 7v 81394512145961145491314Using Fluerry’s algorithm,we construct a closed trail of this new graph which contains all its edges.One such trail can be v 1v 2v 1v 8v 2v 7v 8v 5v 4v 3v 4v 6v 3v 7v 6v 5v 1,and this is also the closed walk with minimum weight which contains all the edges in the original graph.(there are many other possible answers).The weight of our closed walk is (27)+(5+4+9+6+11+4+12+13+9+5+4+14+9+5)=137.Question 4Apply Dijkstra’s algorithm to the graph as drawn in the question.We begin with this table listing the shortest distances from u 9to each of the other vertices,as well as the previous vertex on the path of shortest distance as will be determined when performing the algorithm.Vertexu 1u 2u 3u 4u 5u 6u 7u 8u 9Current shortest distance from u 9∞∞∞∞∞∞∞∞0Previous vertex on path of shortest distance --------NA Is it the fixed shortest possible distance?--------YFocus on u 9,having shortest distance of 0from u 9.u 6,u 7and u 8are unfixed vertices adjacent to u 9.Path u 6−u 9passing through u 6u 9has distance of 4+0=4,which is smaller than its current value of ∞.Path u 7−u 9passing through u 7u 9has distance of 5+0=5,which is smaller than its current value of ∞.Path u 8−u 9passing through u 8u 9has distance of 3+0=3,which is smaller than its current value of ∞.Hence update table on new shortest distances from u 9,of u 6,u 7and u 8:Vertexu 1u 2u 3u 4u 5u 6u 7u 8u 9Current shortest distance from u 9∞∞∞∞∞4530Previous vertex on path of shortest distance -----u 9u 9u 9NA Is it the fixed shortest possible distance?--------Y Among the unfixed shortest distances,u 8has the shortest distance of 3from u 9.Hence fix u 8.Vertexu 1u 2u 3u 4u 5u 6u 7u 8u 9Current shortest distance from u 9∞∞∞∞∞4530Previous vertex on path of shortest distance -----u 9u 9u 9NA Is it the fixed shortest possible distance?-------YYFocus on u 8,having shortest distance of 3from u 9.u 4,u 6and u 7are unfixed vertices adjacent to u 8.Path u 4−u 9passing through u 4u 8has distance of 7+3=10,which is smaller than its currentvalue of∞.Path u6−u9passing through u6u8has distance of2+3=5,which is larger than its current value of4.Path u7−u9passing through u7u8has distance of6+3=9,which is larger than its current value of5.Hence update table on new shortest distances from u9,of u4:Vertex u1u2u3u4u5u6u7u8u9 Current shortest distance from u9∞∞∞10∞4530 Previous vertex on path of shortest distance---u8-u9u9u9NAIs it thefixed shortest possible distance?-------Y Y Among the unfixed shortest distances,u6has the shortest distance of4from u9.Hencefix u6.Vertex u1u2u3u4u5u6u7u8u9 Current shortest distance from u9∞∞∞10∞4530 Previous vertex on path of shortest distance---u8-u9u9u9NAIs it thefixed shortest possible distance?-----Y-Y YFocus on u6,having shortest distance of4from u9.u4and u5are unfixed vertices adjacent to u6. Path u4−u9passing through u4u6has distance of4+4=8,which is smaller than its current value of10.Path u5−u9passing through u5u6has distance of3+4=7,which is smaller than its current value of∞.Hence update table on new shortest distances from u9,of u4and u5:Vertex u1u2u3u4u5u6u7u8u9 Current shortest distance from u9∞∞∞874530 Previous vertex on path of shortest distance---u6u6u9u9u9NAIs it thefixed shortest possible distance?-----Y-Y Y Among the unfixed shortest distances,u7has the shortest distance of5from u9.Hencefix u7.Vertex u1u2u3u4u5u6u7u8u9 Current shortest distance from u9∞∞∞874530 Previous vertex on path of shortest distance---u6u6u9u9u9NAIs it thefixed shortest possible distance?-----Y Y Y YFocus on u7,having shortest distance of5from u9.u3and u4are unfixed vertices adjacent to u7. Path u3−u9passing through u3u7has distance of5+5=10,which is smaller than its current value of∞.Path u4−u9passing through u4u7has distance of4+5=9,which is larger than its current value of8.Hence update table on new shortest distances from u9,of u3:Vertex u1u2u3u4u5u6u7u8u9 Current shortest distance from u9∞∞10874530 Previous vertex on path of shortest distance--u7u6u6u9u9u9NAIs it thefixed shortest possible distance?-----Y Y Y Y Among the unfixed shortest distances,u5has the shortest distance of7from u9.Hencefix u5.Vertex u1u2u3u4u5u6u7u8u9 Current shortest distance from u9∞∞10874530 Previous vertex on path of shortest distance--u7u6u6u9u9u9NAIs it thefixed shortest possible distance?----Y Y Y Y YFocus on u5,having shortest distance of7from u9.u1,u2and u4are unfixed vertices adjacent to u5.Path u1−u9passing through u1u5has distance of3+7=10,which is smaller than its current value of∞.Path u2−u9passing through u2u5has distance of7+7=14,which is smaller than its current value of∞.Path u4−u9passing through u4u5has distance of9+7=16,which is larger than its current value of8.Hence update table on new shortest distances from u9,of u1and u2: Vertex u1u2u3u4u5u6u7u8u9 Current shortest distance from u9101410874530 Previous vertex on path of shortest distance u5u5u7u6u6u9u9u9NAIs it thefixed shortest possible distance?----Y Y Y Y Y Among the unfixed shortest distances,u4has the shortest distance of8from u9.Hencefix u4.Vertex u1u2u3u4u5u6u7u8u9 Current shortest distance from u9101410874530 Previous vertex on path of shortest distance u5u5u7u6u6u9u9u9NAIs it thefixed shortest possible distance?---Y Y Y Y Y Y Focus on u4,having shortest distance of8from u9.u2and u3are unfixed vertices adjacent to u4.Path u2−u9passing through u2u4has distance of6+8=14,which is equal than its current value of14.Path u3−u9passing through u3u4has distance of9+8=17,which is larger than its current value of10.Hence there is no update of the table in this step.Among the unfixed shortest distances,u1has the shortest distance of10from u9(alternatively we can choose u3which also has a distance of10).Hencefix u1.Vertex u1u2u3u4u5u6u7u8u9 Current shortest distance from u9101410874530 Previous vertex on path of shortest distance u5u5u7u6u6u9u9u9NAIs it thefixed shortest possible distance?Y--Y Y Y Y Y Y Focus on u1,having shortest distance of10from u9.u2and u3are unfixed vertices adjacent to u1.Path u2−u9passing through u2u1has distance of4+10=14,which is equal than its current value of14.Path u3−u9passing through u3u1has distance of13+10=13,which is larger than its current value of10.Hence there is no update of the table in this step.Among the unfixed shortest distances,u3has the shortest distance of10from u9.Hencefix u3.Vertex u1u2u3u4u5u6u7u8u9 Current shortest distance from u9101410874530 Previous vertex on path of shortest distance u5u5u7u6u6u9u9u9NAIs it thefixed shortest possible distance?Y-Y Y Y Y Y Y Y Focus on u3,having shortest distance of10from u9.u2is the unfixed vertex adjacent to u3.Path u2−u9passing through u2u3has distance of8+10=18,which is larger than its current value of14.Hence there is no update of the table in this step.Only u2is unfixed at this point.Hencefix u2.We now have ourfinal table,which shows the shortest distances from u9to all the vertices in G:Vertex u1u2u3u4u5u6u7u8u9Shortest distance from u9101410874530Question5(i)This graph is hamiltonian.The hamiltonian cycle is as shown below,where the blue edges indicateedges that have to be included due to vertices having only two possible adjacent edges left that could be in the hamiltonian cycle,red crosses represent edges that are not possible to be in the hamiltonian cycle due to similar logical deductions,and green edges represents the rest of the edges filled in to complete the hamiltonian cycle(your own hamiltonian cycle can have different such green edges,as long as all vertices are in the cycle).v 1v 2v 3v 4v 5v 6v 7v 8v 9v 10v 11v 12v 13v 14v 15v 16v 17v 18v 19v 20v 21v 22v 23v 24v 25w 1w 2w 3w 4w 5X X X XXX XXXXX XX XXX X (ii)Consider the following construction,where the blue edges indicate edges that have to be includeddue to vertices having only two possible adjacent edges left that could be in the hamiltonian cycle,and red crosses represent edges that are not possible to be in the hamiltonian cycle due to similar logical deductions.v 1v 2v 3v 4v 5v 6v 7v 8v 9v 10v 11v 12v 13v 14v 15v 16v 17v 18v 19v 20v 21v 22v 23v 2425w 1w 2w 3w 4w 5X X X XXX XX X X X X X XXX XSuppose a hamiltonian cycle exists for this graph.We claim that either v 22v 18or v 22v 17is in the hamiltonian cycle.Suppose not.Then both v 22v 18and v 22v 17are not in the hamiltonian cycle.Hence v 17v 18is in the hamiltonian cycle.Then v 11v 17is not in the hamiltonian cycle otherwise a C 4is formed.Then both v 10v 11and v 10v 17are in the hamiltonian cycle.But this forms a C 5:v 10v 11w 3v 18v 17v 10!A contradiction.With this claim,v 22v 23and v 22v 25are both not in the hamiltonian cycle.Hence,v 25v 23,v 23v 24and v 25v 24are all in the hamiltonian cycle,thus forming a C 3!A contradiction.Hence this graph is not hamiltonian.Question6Consider a graph G.Let people be represented by vertices,and the symmetric relation‘knowing’between two people be represented by an edge between the two respective vertices.The given condition translates as:G has n vertices where n≥4.∀distinct u,v,w∈V(G),if uw/∈E(G), then vw∈E(G)(otherwise w is a‘person’that neither u or v knows).The question asks to prove that G is hamiltonian.If G is a complete graph then it is straightforward that G is hamiltonian.Consider G to be not a complete graph.There exists distinct u,v∈V(G)such that uv/∈E(G).We claim that ∀w∈V(G)\{u,v},uw∈E(G)and vw∈E(G).Suppose not.Then∃w∈V(G)\{u,v}such that,without loss of generality,uw/∈E(G).But now consider w and v:uw/∈E(G)and uv/∈E(G),violating the given condition!A contradiction.Hence the claim is true.Hence,for all distinct non-adjacent x,y∈V(G),d(x)=n−2and d(y)=n−2.Hence d(x)+d(y)= 2n−4>n for n≥4.Therefore,by Ore’s Theorem,G is hamiltonian.Question7(i)Note:This question requires a resolution to the girth of graphs without any cycles,e.g.trees.It isgenerally considered that a tree has infinite girth.If a tree is considered to be a graph with‘girth at least6’,then simple counter examples to the statement exists,such as:The graph above has a disconnected complement and hence is not hamiltonian.We shall now only consider graphs withfinite girths,i.e.,graphs which contains cycles.Given G,a graph with cycles with girth at least6,consider any adjacent vertices x and y in G.Let N(x)be the set of vertices adjacent to x,N(y)be the set of vertices adjacent to y and S be the set of vertices adjacent to neither x or y.No vertex falls in both N(x)and N(y),or else for any such vertex w,xwyx is a C3,a contradiction to the girth requirement.Also,no pairs of vertices in N(x)are adjacent,otherwise for any such a pair of vertices u and v,xuvx is a C3,another contradiction.By a similar argument no pairs of vertices in N(y)are adjacent.Also,no vertex in N(x)is adjacent with vertices in N(y),otherwise for any such a pair of vertices u∈N(x)and v∈N(y),xuvyx is a C4,another contradiction.We claim that|S|≥2.Suppose not.If|S|=0,then G has no cycles,which is what we did not want.If|S|=1,let the only vertex in S be z.z is adjacent to at most one vertex in N(x), otherwise for two vertices u,v∈N(x)that z is adjacent to,xuzv is a C4,a contradiction.By a similar argument z is adjacent to at move one vertex in N(y).If z is not adjacent to all vertices in N(x),or not adjacent to all vertices in N(y),then G has no cycles by considering all previous conditions.Hence z is adjacent to exactly one vertex in N(x),p,and exactly one vertex in N(y), q.But xpzqyx is a C5,another contradiction!Hence|S|≥2.Consider G.x and y are non-adjacent vertices in G.In G,d(x)=|N(y)|+|S|,and d(y)= |N(x)|+|S|.Hence d(x)+d(y)=|N(x)|+|N(y)|+|S|+|S|≥|N(x)|+|N(y)|+|S|+2=v(G)=v(G).This holds for any non-adjacent x and y in G.Hence by Ore’s Theorem,G is hamiltonian.(ii)Suppose G is disconnected.Consider the vertex v∈G where d(v)=∆(G)= n2.There existsn− n2−1=n2−1vertices in G not adjacent to v.Let the set of these vertices be S.Since G is assumed to be disconnected,there exists a vertex w in S such that v and w are in different components of G,otherwise all vertices in G are in the same component as v and theMA3233Algorithmic Graph Theory AY2006/2007Sem1 graph is connected.Hence,w is not adjacent to any vertices in G\S.Hence w can only be adjacentto vertices in S. Hence,d(w)<|S|= n2−1=δ(G),a contradiction!Therefore G is connected.(iii)Since n≡1(mod4),the number of vertices in G is paring G and G,all corresponding vertices u∈V(G)and u ∈V(G)can be paired up such that d(u)+d(u )=n−1.Since G is self complementary,G∼=G.Suppose there is no vertex with degree n−12.∀u∈V(G),∃distinct v∈V(G)such that d(u)+d(v)=n−1(distinct since their degrees would not be thesame).Since there are an odd number of vertices,we can form up n−12disjoint pairs of verticeswith degree sums of n−1,with one vertex left over.Call this leftover vertex x.The degree of x is the sum of total degrees of all vertices in G,subtracted by n−12pairs of(n−1).Hence,d(x)= n2−(n−1)n−12=12(n(n−1)−(n−1)(n−1))=n−12,a contradiction!Hence thereexists a vertex with degree n−12.NUS Math LaTeXify Proj Team Page:11of11NUS Mathematics Society。