文档内容
{{##{{QQQQAABBKKQQIKQwgwgggggQABgBIAbAABChBC4AKwAEwQEC0CgCgmQQkgsApAIhCJSaggMOAQVFCAJAqsAAxAKACSQBFFIABBIAA=A}=#}}#}{{##{{QQQQAABBKKQQIKQwgwgggggQABgBIAbAABChBC4AKwAEwQEC0CgCgmQQkgsApAIhCJSaggMOAQVFCAJAqsAAxAKACSQBFFIABBIAA=A}=#}}#}{{##{{QQQQAABBKKQQIKQwgwgggggQABgBIAbAABChBC4AKwAEwQEC0CgCgmQQkgsApAIhCJSaggMOAQVFCAJAqsAAxAKACSQBFFIABBIAA=A}=#}}#}{{##{{QQQQAABBKKQQIKQwgwgggggQABgBIAbAABChBC4AKwAEwQEC0CgCgmQQkgsApAIhCJSaggMOAQVFCAJAqsAAxAKACSQBFFIABBIAA=A}=#}}#}{{##{{QQQQAABBKKQQIKQwgwgggggQABgBIAbAABChBC4AKwAEwQEC0CgCgmQQkgsApAIhCJSaggMOAQVFCAJAqsAAxAKACSQBFFIABBIAA=A}=#}}#}{{##{{QQQQAABBKKQQIKQwgwgggggQABgBIAbAABChBC4AKwAEwQEC0CgCgmQQkgsApAIhCJSaggMOAQVFCAJAqsAAxAKACSQBFFIABBIAA=A}=#}}#}{{##{{QQQQAABBKKQQIKQwgwgggggQABgBIAbAABChBC4AKwAEwQEC0CgCgmQQkgsApAIhCJSaggMOAQVFCAJAqsAAxAKACSQBFFIABBIAA=A}=#}}#}{{##{{QQQQAABBKKQQIKQwgwgggggQABgBIAbAABChBC4AKwAEwQEC0CgCgmQQkgsApAIhCJSaggMOAQVFCAJAqsAAxAKACSQBFFIABBIAA=A}=#}}#}{{##{{QQQQAABBKKQQIKQwgwgggggQABgBIAbAABChBC4AKwAEwQEC0CgCgmQQkgsApAIhCJSaggMOAQVFCAJAqsAAxAKACSQBFFIABBIAA=A}=#}}#}{{##{{QQQQAABBKKQQIKQwgwgggggQABgBIAbAABChBC4AKwAEwQEC0CgCgmQQkgsApAIhCJSaggMOAQVFCAJAqsAAxAKACSQBFFIABBIAA=A}=#}}#}{{##{{QQQQAABBKKQQIKQwgwgggggQABgBIAbAABChBC4AKwAEwQEC0CgCgmQQkgsApAIhCJSaggMOAQVFCAJAqsAAxAKACSQBFFIABBIAA=A}=#}}#}{{##{{QQQQAABBKKQQIKQwgwgggggQABgBIAbAABChBC4AKwAEwQEC0CgCgmQQkgsApAIhCJSaggMOAQVFCAJAqsAAxAKACSQBFFIABBIAA=A}=#}}#}2024 年 12 月山东名校考试联盟高三年级阶段性检测
物 理 试 题 参 考 答 案 及 评 分 标 准
1 2 3 4 5 6 7 8
A C B D A C B D
9 10 11 12
AD AC AD BD
d ( M +5m ) kd2
13.(4) 增大 (6) (每小问2分,共 6分)
t 2mL
0
14.(1) (3)2596.0或2596.0 大于
(4) 4 (每小问 2分,共 8分)
15.(7分)
(1)包裹与水平托盘保持相对静止并以最大加速度运动时,由牛顿第二定律可得:
f =ma............................................................................................................................(2 分)
1
此状态下滑动摩擦力大小为: f =mg
2
当托盘倾角增大到时,包裹恰好开始下滑,由受力平衡得:
f ' =mg sin......................................................................................................................(. 1分)
1
此状态下滑动摩擦力大小为: f ' =mg cos
2
f f '
由题意知: 1 = 1 =1.25
f f '
2 2
3
解得:tan= .................................................................................................................(. 1分)
4
(2)包裹下滑过程中,由牛顿第二定律可得:
mgsin−mg cos=ma'..............................................................................................(. 1分)
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解得:v=1.2m/s...........................................................................................................(1分)
16. (9分)
(1)小球恰好能在竖直面内完成圆周运动,则小球在最高点时由牛顿第二定律得:
v2
mg=m 1 ......................................................................................................................(1分)
l
小球从最高点运动到轻绳水平的过程中,由动能定理得:
1 1
mgl = mv2 − mv2........................................................................................................(2分)
2 2 1
解得:v= 3gl...............................................................................................................(1分)
(2)小球运动到最低点时,绳子的拉力最大。小球从最高点运动到最低点的过程中,由动能
1 1
定理得:mg 2l = mv2 − mv2............................................................................................(1分)
2 2 2 1
v2
小球在最低点时由牛顿第二定律得:T −mg=m 2 ...........................................................(1分)
l
此时对支架(包括底座)受力分析得:F =T +Mg..........................................................(1 分)
N
由牛顿第三定律得:N = F
N
( )
解得:N = M +6m g...............................................................................................................(1 分)
(3)先减小后增大...................................................................................................................(1 分)
17.(14分)
(1)设离子在区域Ⅰ中的加速度大小为a ,由牛顿第二定律得
1
qE =ma ............................................................................................................................(2分)
1
离子恰好到区域Ⅰ下边界时,有
0−(v cos30)2 = −2a L...................................................................................................(. 2分)
1 1
8qEL
解得:v = ...........................................................................................................(. 1分)
1 3m
(2)设离子初速度大小为v ,到区域Ⅰ下边界时速度沿 y轴分量大小为v ,在区域Ⅱ中的加速
2 y
度大小为a ,有
2
v2 −(v cos30)2 =−2a L.................................................................................................(. 1分)
y 2 1
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q = ma ..........................................................................................................................(. 1分)
2 2
5
0−v2 = −2a( L−2L)....................................................................................................(1分)
y 2 2
v
tan= y ...............................................................................................................(1 分)
v sin30
2
15
解得:tan= ............................................................................................................(. 1分)
5
(3)设离子恰能进入第四象限时的初速度大小为v ,到区域Ⅰ下边界时速度沿y轴分量大小为
3
v ',在区域Ⅱ中的加速度大小关于 y的平均值为a ,有
y 3
v '2−(v cos30)2 =−2a L................................................................................................(. 1分)
y 3 1
qE
a = .............................................................................................................................(1分)
3 2m
0−v '2 = −2a L.................................................................................................................(. 1 分)
y 3
初速度大小大于v 的离子可进入第四象限,则
3
qEL
6 −v
m 3
=
qEL qEL
6 −
m m
解得:η=80%.....................................................................................................................(. 1分)
18.(16分)
(1)物块A、木板B 和物块 C 恰好能够保持静止状态,对物块 A、木板B 和物块 C 受力分
析得:m g+ ( m +m ) gcos37= ( m +m ) gsin37.............................................................(. 2分)
3 2 1 2 1 2
解得:m =1kg..........................................................................................................................(. 1分)
3
1
x = gt2
(2)(i)轻绳伸直前,物块C 始终做自由落体运动,运动的位移为: 1 2 ............(1分)
物块 A、木板B 先做匀减速直线运动直到与传送带速度相同,由牛顿第二定律得:
( m +m ) gsin37+ ( m +m ) gcos37= ( m +m ) a ..............................................................(1 分)
1 2 2 1 2 1 2 1
解得:a =10m/s2
1
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此阶段所用时间和位移为:t = 0 1
11 a
1
v +v
x = 0 1t ..............................................................................(1 分)
2 2 11
解得:t =1s x =13m
11 2
物块 A、木板B 与传送带共速后,继续做匀减速直线运动直到轻绳伸直,由牛顿第二定律得:
( ) ( ) ( )
m +m gsin37− m +m gcos37= m +m a
1 2 2 1 2 1 2 2
解得:a =2m/s2
2
1
此阶段的位移为:x =v ( t −t ) − a ( t −t )2.........................................................................(. 1分)
3 1 1 11 2 2 1 11
x = x +x
轻绳伸直时: 1 2 3
解得:x =7m
3
t =2s..........................................................................................................(1分)
1
(ii)在0~t 内,木板B与传送带之间的相对位移为:s = x −vt
11 1 2 111
t ~ t 内,木板B 与传送带之间的相对位移为:s =v ( t −t ) −x .................................(1 分)
11 1 2 1 1 11 3
0-t 内B 与传送带间因摩擦产生的热量 Q:Q= ( m +m ) gcos37 ( s +s ) ..............(1 分)
1 2 1 2 1 2
解得:Q=120J............................................................................................................................(1 分)
v = gt
(iii)轻绳伸直前瞬间,物块 C 的速度为: 2 1
( )
v =v −a t −t
物块 A、木板B 速度为: 3 1 2 1 11
v =20m/s v =6m/s
解得: 2 3
轻绳伸直时,将木板B 和物块 C 是为一个系统,系统的内力远大于外力,系统动量守恒:
( )
m v +m v = m +m v
2 3 3 2 2 3 4.....................................................................................................(2分)
v =13m/s
解得: 4
轻绳伸直后,在木板B 和物块 C 与传送带速度相同之前,对木板B 和物块C 受力分析,由牛
顿第二定律得:
( ) ( )
m gsin37+m gcos37+ m +m gcos37−m g = m +m a
2 1 1 2 1 2 3 2 3 3
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t = 4 1
2 a
所用时间为: 3
5
t = s
解得: a 3 =22m/s2 2 22
mgcos37−mgsin37=ma
对物块 A受力分析,由牛顿第二定律得: 1 1 1 1 4
v =v +a t
当木板 B 和物块C 与传送带速度相同时,物块 A得速度为: 5 3 4 2
137
v = m/sv
解得: a 4 =1m/s2 5 22 1 .............................................................................(1分)
当木板 B 和物块C 与传送带共速之后,对木板B 和物块 C 受力分析,由牛顿第二定律得:
( ) ( )
m gsin37+m gcos37− m +m gcos37−m g = m +m a
2 1 1 2 1 2 3 2 3 5
a =2m/s2
解得: 5
v=v −a t =v +a t
当物块 A、木板B 与物块C 到达共速时: 1 5 3 5 4 3..................................(1分)
75
v= m/s
解得: 11 ................................................................................................................(1分)
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