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一模物理答案_2025年3月_250328太原市2025年高三年级模拟考试(一)(全科)_太原市2025年高三年级模拟考试(一)物理

  • 2026-03-09 14:34:26 2026-02-10 20:43:27

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一模物理答案_2025年3月_250328太原市2025年高三年级模拟考试(一)(全科)_太原市2025年高三年级模拟考试(一)物理
一模物理答案_2025年3月_250328太原市2025年高三年级模拟考试(一)(全科)_太原市2025年高三年级模拟考试(一)物理
一模物理答案_2025年3月_250328太原市2025年高三年级模拟考试(一)(全科)_太原市2025年高三年级模拟考试(一)物理
一模物理答案_2025年3月_250328太原市2025年高三年级模拟考试(一)(全科)_太原市2025年高三年级模拟考试(一)物理
一模物理答案_2025年3月_250328太原市2025年高三年级模拟考试(一)(全科)_太原市2025年高三年级模拟考试(一)物理
一模物理答案_2025年3月_250328太原市2025年高三年级模拟考试(一)(全科)_太原市2025年高三年级模拟考试(一)物理

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太原市 2025 年高三年级模拟考试(一) 物理参考答案与评分建议 一、选择题:本题共7小题,每小题4分,共28分。在每小题给出的四个选项中,只有一 项是符合题目要求的。 题号 1 2 3 4 5 6 7 答案 D B D A B D A 二、多项选择题:本题包含3小题,每小题6分,共18分。在每小题给出的四个选项中, 至少有两个选项正确,全部选对的得6分,选对但不全的得3分,有选错的得0分。 题号 8 9 10 答案 BC AC ABD 三、实验题:本题包含2小题,共15分。请将正确答案填在题中横线上或按要求作答。 11.(6分) k br (1)A(2分) (2) (2分) (2分) r kg 12.(9分) (1)分压式(1分) (2)截止(或极限)(1分) (3)Oa (1分) (4)Ob(1分) 3.91015(3.6~ 4.31015)(2分) ke(1分) (1分) (5)右(1分)四、计算题:本题包含3小题,共39分。解答应写出必要的文字说明、方程式和重要演算 步骤,只写出最后答案的不能得分。有数值计算的题,答案中必须明确写出数值和单位。 13.(1)M到达bb时速度为v 1 v2 F mg m 1 ···················································································1分 N R F  F 2mg N 压 v  gR ····························································································1分 1 方法一: M从aa到bb,依能量守恒 1 mgR  mv2 Q·················································································1分 2 1 Q r 1 N   ·······················································································1分 Q 2r 2 1 Q  mgR························································································1分 N 4 方法二: M从aa到bb,依动能定理   1 mgR W  mv2 0······································································1分 安 2 1 W Q 安 Q Q Q 2Q ·············································································1分 M N N 1 Q  mgR························································································1分 N 4 (2)M到达bb时,N解除锁定,M减速,N加速,最后分别做匀速运动 N切割磁感线的有效长度为L, v 、v 水平向右 M N B2Lv  BLv ····················································································1分 M N M减速过程,依动量定理,以右为正 I2LBt mv mv ······································································1分 M 1 N加速过程,依动量定理,以右为正 ILBt mv 0··············································································1分 N1 v  gR ························································································1分 M 5 2 v  gR ························································································1分 N 5 14.(1)电子在间距为r 的轨道上运动时 n e2 v2 k  m ························································································3分 r2 r n n 2 nh r mv  n 2π ke2 v 2mr n n2h2 r  ······················································································1分 n 2π2ke2m (2)方法一:电子偶素中电子的总动能、势能分别为 1 E 2 mv2 ·····················································································1分 k 2 1 e2 E  k ·························································································1分 k 2 r n e2 E k ··························································································1分 p r n E  E E n k p π2k2e4m E  ···················································································1分 n n2h2 方法二:电子偶素中电子或正电子的动能、势能分别为 1 E  mv2 ··························································································1分 k 2 1 e2 E  k ·························································································1分 k 4 r n e2 E k ··························································································1分 p r n E 2E E n k pπ2k2e4m E  ···················································································1分 n n2h2 (3)电子偶素由第一激发态跃迁到基态时,放出光子的频率为 h E E ························································································1分 2 1 π2k2e4m E  ···················································································1分 2 4h2 π2k2e4m E  ··················································································· 1分 1 h2 3π2k2e4m  ······················································································1分 4h3 15.(1)方法一: 火箭在点火预热阶段喷出气体,火箭对气体的平均作用力为F,依动量定理,以下为正 Ft mv 0······················································································3分 0 0 火箭获得的平均推力F F  F································································································1分 mv F  0 ·····························································································1分 t 0 方法二: 火箭在点火预热阶段喷出气体,火箭对气体的平均作用力为F, Fm a·····························································································2分 0 v a  0 ································································································1分 t 0 火箭获得的平均推力F F  F································································································1分 mv F  0 ·····························································································1分 t 0 (2)运载物、燃料在喷出气体的过程中动量守恒,以上为正  Mv 3m v 0················································································3分 2 1 3mv v  1 ···························································································1分 2 M (3)方法一: 以地面为参考系,以上为正,第一级燃料燃烧后,运载物获得的速度大小为v , 运1 依动量守恒定律 (M 2m)v m(-vv )0····························································1分 运1 运1 第二级燃料燃烧后,运载物获得的速度大小为v 运2 (M m)v m(-vv )(M 2m)v ·············································1分 运2 运2 运1 第三级燃料燃烧后,运载物获得的速度大小为v 3 Mv m(vv )(M m)v ······························································1分 3 3 运2 mv 解得:v  运1 M 3m mv mv v   运2 M 3m M 2m mv mv mv v    ···················································2分 3 M 3m M 2m M m 方法二: 以火箭为参考系,以上为正,第一级燃料燃烧后,运载物获得的速度增量为v ,第二级燃 1 料燃烧后,运载物获得的速度增量为v ,第三级燃料燃烧后,运载物获得的速度增量为v , 2 3 依动量守恒定律 (M 2m)v m(-vv )0····························································1分 1 1 (M m)v m(-vv )0·····························································1分 2 2 Mv m(-vv )0······································································1分 3 3 mv v  1 M 3m mv v  2 M 2m mv v  3 M mmv mv mv v v v v    ···································2分 3 1 2 3 M 3m M 2m M m 同理:若把质量为3m的燃料分成n份,运载物最终获得的速度为v n 3m 3m 3m 3m 3m v v v v v v  n  n  n  n  n ·····2分 n M n 3m M  n1 3m M  n2 3m M 2 3m M 1 3m n n n n n 3mv 3mv 3mv 3mv 3mv v      n nMn3m nM(n1)3m nM(n2)3m nM23m nM13m 依题目已知条件,当n时 M 3m v vln ··················································································1分 n M