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SAMN
Physics
CH3平面運動
3-1 平面運動的描述
CH3-平面運動 1
SAMN
Physics
CH3-平面運動 2
銳角三角函數
從角度找邊長的函數關係


90
對邊 =a
鄰邊 = b
斜邊 = c
sin 𝜃 =
𝑎
𝑐
cos 𝜃 =
𝑏
𝑐
tan 𝜃 =
𝑎
𝑏
正弦函數
餘弦函數
正切函數
SAMN
Physics
CH3-平面運動 3
銳角三角函數
sin 30𝑜
=
1
2
sin 37𝑜
=
3
5
sin 𝜃 =
𝑎
𝑐
cos 𝜃 =
𝑏
𝑐
tan 𝜃 =
𝑎
𝑏
sin 45𝑜
=
1
2
SAMN
Physics
CH3-平面運動 4
向量 Vector
具有量值與方向的數學概念,可以用
有向線段來表示。
終點
起點
റ
𝑎
線段的長度表向量的 大小
箭頭的方向表示向量的 方向
位移 、 速度 、 加速度 、 力 等
符號表示:在字母上頭加一箭號來
表向量,如 റ
𝑎
量值為1的向量稱為 單位向量
SAMN
Physics
向量的特性Properties of Vectors
CH3-平面運動 5
•兩個向量如果相等➔具有相同的大小與相同的方向
向量的等值性
Equality of Two Vectors
•任意向量可以平行移動,而不改變原本的性質(大
小、)方向
向量的可移動性
Movement of vectors in a diagram
SAMN
Physics
CH3-平面運動 6
向量 Vector
終點
起點
റ
𝑎
𝑦
𝑥
𝑥軸的分量:𝑎𝑥
𝑦軸的分量:𝑎𝑦
𝜽
量值為1的向量稱為 單位向量
റ
𝑎
Ƹ
i、 Ƹ
j、෠
k
റ
𝑎 = 𝑎𝑥 Ƹ
i + 𝑎𝑦 Ƹ
j
SAMN
Physics
CH3-平面運動 7
向量 Vector
𝑦
𝑥
𝑥軸的分量:𝑎𝑥
𝑦軸的分量:𝑎𝑦
𝜽
റ
𝑎
റ
𝑎 = 𝑎𝑥 Ƹ
i + 𝑎𝑦 Ƹ
j sin𝜃 =
𝑎𝑦
𝑎
𝑎𝑦 = 𝑎 ⋅ sin𝜃
cos𝜃 =
𝑎𝑥
𝑎
𝑎𝑥 = 𝑎 ⋅ cos𝜃
tan𝜃 =
𝑎𝑦
𝑎𝑥
റ
𝑎 = 𝑎𝑥
2
+ 𝑎𝑦
2
SAMN
Physics
CH3-平面運動 8
向量 Vector
A
B
C
O
Vectors in three dimensions
, ,
x y z
x y z
V V i V j V k
V OA V OB V OC
= + +
= = =
SAMN
Physics
CH3-平面運動 9
向量加法與減法
റ
𝑎
𝑏
റ
𝑐
加法型態 റ
𝑐 = റ
𝑎 + 𝑏
sin sin sin
A B C
a b c
  
= =
正弦定律
餘弦定律
2 2 2
2 cos
c a b ab 
= + +
SAMN
Physics
減法型態
CH3-平面運動 10
向量加法與減法
റ
𝑑 = റ
𝑎 − 𝑏
റ
𝑎
−𝑏
റ
𝑐
𝑏
റ
𝑎
𝑎
sin 𝜃𝐴
=
𝑏
sin 𝜃𝐵
=
𝑐
sin 𝜃𝐶
正弦定律
餘弦定律
𝑐2 = 𝑎2 + 𝑏2 + 2𝑎𝑏 cos 𝜃
SAMN
Physics
CH3-平面運動 11
以解析幾何的計算式來尋找向量量值
റ
𝐴 = 𝑥1 Ƹ
i + 𝑦1 Ƹ
j
റ
𝐴 + 𝐵 = 𝑥1 + 𝑥2 Ƹ
i + 𝑦1 + 𝑦2 Ƹ
j
𝐵 = 𝑥2 Ƹ
i + 𝑦2 Ƹ
j
𝑥1
𝑦1
റ
𝐴
𝑥2
𝑦2 𝐵 𝑥1
𝑦1
റ
𝐴
𝑥2
𝑦2
𝐵
向量加法
A + B
SAMN
Physics
CH3-平面運動 12
以解析幾何的計算式來尋找向量量值
റ
𝐴 = 𝑥1 Ƹ
i + 𝑦1 Ƹ
j
റ
𝐴 − 𝐵 = 𝑥1 − 𝑥2 Ƹ
i + 𝑦1 − 𝑦2 Ƹ
j
𝐵 = 𝑥2 Ƹ
i + 𝑦2 Ƹ
j
𝑥1
𝑦1
റ
𝐴
𝑥2
𝑦2 𝐵
𝑥1
𝑦1
റ
𝐴
𝑥2
𝑦2
𝐵
向量減法
𝑦1 − 𝑦2
𝑥1 − 𝑥2
A − B
SAMN
Physics
CH3-平面運動
13
向量運算-減法
物體在水面上運動,在5秒內速度由6 m/s向東,變成8 m/s向
北,則物體的平均加速度大小為多少? (A) 10 (B) 8 (C) 4
(D) 2 m/s2。
例題4.
SAMN
Physics
平面運動的位置向量與位移向量
CH3-平面運動 14
y
Δറ
𝑟 = റ
𝑟2 − റ
𝑟1
= (𝑥2 Ƹ
i + 𝑦2 Ƹ
j) − (𝑥1 Ƹ
i + 𝑦1 Ƹ
j)
= (𝑥2 − 𝑥1) Ƹ
i + (𝑦2 − 𝑦1) Ƹ
j
= Δ𝑥 Ƹ
i + Δ𝑦 Ƹ
j
റ
𝑟1 = 𝑥1 Ƹ
i + 𝑦1 Ƹ
j
A1的位置向量
റ
𝑟2 = 𝑥2റ
i + 𝑦2റ
j
A2的位置向量
A1到A2的位移向量
SAMN
Physics
平面運動的速度
CH3-平面運動 15
質點在平面運動時候的 移動快慢
及 移動方向 。
x
y
1
r
2
r
P
Q
切線
r

റ
𝑣𝑎𝑣 =
Δറ
𝑟
Δ𝑡
=
റ
𝑟2 − റ
𝑟1
𝑡2 − 𝑡1
റ
𝑣𝑎𝑣 =
Δ𝑥
Δ𝑡
Ƹ
𝐢 +
Δ𝑦
Δ𝑡
Ƹ
𝐣 = 𝑣𝑥 Ƹ
𝐢 + 𝑣𝑦 Ƹ
𝐣
平均速度
瞬時速度
റ
𝑣 = lim
Δ𝑡→0
Δറ
𝑟
Δ𝑡
= lim
Δ𝑡→0
(
Δ𝑥
Δ𝑡
Ƹ
𝐢 +
Δ𝑦
Δ𝑡
Ƹ
𝐣)
= 𝑣𝑥 Ƹ
𝐢 + 𝑣𝑦 Ƹ
𝐣
SAMN
Physics
平面運動的加速度
CH3-平面運動 16
用來描述運動中物體的速度變化
的 快慢 及 移動方向 。
x
y
1
r
2
r
P
Q
r

റ
𝑎𝑎𝑣 =
Δ റ
𝑣
Δ𝑡
=
റ
𝑣2 − 𝑣1
𝑡2 − 𝑡1
റ
𝑎𝑎𝑣 =
Δ𝑣𝑥
Δ𝑡
Ƹ
𝐢 +
Δ𝑣𝑦
Δ𝑡
Ƹ
𝐣 = 𝑎𝑥 Ƹ
𝐢 + 𝑎𝑦 Ƹ
𝐣
平均加速度
瞬時速度
റ
𝑎 = lim
Δ𝑡→0
Δ റ
𝑣
Δ𝑡
= lim
Δ𝑡→0
(
Δ𝑣𝑥
Δ𝑡
Ƹ
𝐢 +
Δ𝑣𝑦
Δ𝑡
Ƹ
𝐣)
= 𝑎𝑥 Ƹ
𝐢 + 𝑎𝑦 Ƹ
𝐣
റ
𝑣1
റ
𝑣2
SAMN
Physics
平面運動中的加速度與速度的關係
CH3-平面運動 17
a
n
a
t
a
在平面運動的質點,可以將路徑某
點的加速度分解成軌跡的 切線 方
向和 法線 方向
切線加速度 റ
𝑎𝑡:加速度沿瞬時速度方向的分量
改變速度大小,不改變速度方向
法線加速度 റ
𝑎𝑛:加速度沿垂直速度方向的分量
改變速度方向,不改變速度量值
SAMN
Physics
平面運動中的加速度與速度的關係
CH3-平面運動 18
P點的法線方向
P
質點P的移
動軌跡
റ
𝑎
റ
𝑎
റ
𝑣
റ
𝑣
加速 且右彎
減速 且右彎

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