[{"data":1,"prerenderedAt":-1},["ShallowReactive",2],{"$fxAeyta8r7ce3oc2mCGOpiOlM_amIfOAaguIr6ozmeTE":3},{"answer":4,"createTime":5,"id":6,"options":7,"origin":11,"question":18,"related":19,"source":29,"type":30},[],"2024-11-09 19:07:01",165192173,[8,9,10],"按角度个数平均分配","按导线边数平均分配","按边长成正比例分配",{"count":12,"courseId":13,"courseImg":14,"courseName":15,"workId":16,"workName":17},20,"021add7dcbbd066e76cb63a6e0699a8c","https:\u002F\u002Ftihai-oss-cloud.itihey.com\u002Fimg\u002F7e2d5ad53be3d12aacc56ee37db405b7.jpg","测量学－22程管","work_38660251","小地区控制测量(二)","导线坐标增量闭合差的调整方法是将闭合差反符号后",[20,31,40,49,58,67,76,85,94,97],{"answer":21,"createTime":5,"id":22,"options":23,"question":28,"source":29,"type":30},[],165192165,[24,25,26,27],"45&deg;","315&deg;","225&deg;","135&deg;","已知A点坐标为(12345.7,437.8),B点坐标为(12322.2,461.3),则AB边的坐标方位角aAB","v1",0,{"answer":32,"createTime":5,"id":33,"options":34,"question":39,"source":29,"type":30},[],165192166,[35,36,37,38],"真子午线北端","坐标纵轴北端","磁子午线北端","任意方向","坐标方位角的起算方向为",{"answer":41,"createTime":5,"id":42,"options":43,"question":48,"source":29,"type":30},[],165192167,[44,45,46,47],"从控制到碎部","从碎部到控制","控制与碎部并行","测图与放样并行","测量工作的基本原则是从整体到局部、从高级到低级和( )",{"answer":50,"createTime":5,"id":51,"options":52,"question":57,"source":29,"type":30},[],165192168,[53,54,55,56],"-80&quot;","+80&quot;","359&deg;59&prime;20&Prime;","-40&quot;","下图为闭合导线,方位角闭合差为: \u003Cimg src=\"https:\u002F\u002Ftihai-oss-cloud.itihey.com\u002Fimg\u002Ffa4d228ed3c25e2d7125aceb471b17bc.webp\">",{"answer":59,"createTime":5,"id":60,"options":61,"question":66,"source":29,"type":30},[],165192169,[62,63,64,65],"&alpha;起+&sum;&beta;-&alpha;终-n&times;180&deg;","&sum;&beta;内-(n-2) &times;180&deg;","&alpha;终+&sum;&beta;-&alpha;起-n&times;180&deg;","没有角度闭合差","闭合导线的角度闭合差计算公式为",{"answer":68,"createTime":5,"id":69,"options":70,"question":75,"source":29,"type":30},[],165192170,[71,72,73,74],"附合导线","闭合导线","支导线","导线网","下列哪一种导线形式不能计算角度闭合差和坐标闭合差",{"answer":77,"createTime":5,"id":78,"options":79,"question":84,"source":29,"type":30},[],165192171,[80,81,82,83],"同符号平均分配","同符号与角度大小成正比分配","反符号与角度大小成正比分配","反符号平均分配","导线测量中角度闭合差的分配原则是",{"answer":86,"createTime":5,"id":87,"options":88,"question":93,"source":29,"type":30},[],165192172,[89,90,91,92],"1\u002F4000","1\u002F3500","1\u002F3900","1\u002F4500","已知一导线横坐标增量闭合差为-0.08米,纵坐标增量闭合差为+0.06米,导线全长为390.000米,则该导线的全长相对闭和差为",{"answer":95,"createTime":5,"id":6,"options":96,"question":18,"source":29,"type":30},[],[8,9,10],{"answer":98,"createTime":5,"id":99,"options":100,"question":105,"source":29,"type":30},[],165192174,[101,102,103,104],"63&deg;26&prime;06&Prime;","296&deg;33&prime;54&Prime;","116&deg;33&prime;54&Prime;","27&deg;33&prime;54&Prime;","已知E、F两点间的纵坐标增量&Delta;XEF = -50.00m,横坐标增量为&Delta;YEF =100.00m,则其坐标方位角为"]