Vectors 255
From trigonometry (see Chapter 11),
cosθ=0 a
0 bfrom which, 0a= 0 bcosθ
=Fcosθi.e. the horizontal component ofF=Fcosθ
and sinθ=
ab
0 bfrom which, ab= 0 bsinθ
=Fsinθi.e. the vertical component ofF=Fsinθ
Problem 4. Resolve the force vector of 50N at an
angle of 35◦to the horizontal into its horizontal and
vertical components.The horizontal component of the 50N force,
0 a=50cos35◦=40.96N
The vertical component of the 50N force,
ab=50sin35◦=28.68N
The horizontal and vertical components are shown in
Fig. 24.15.
358
0
40.96N50N 28.68NabFigure 24.15
(Checking: by Pythagoras, 0b=
√
40. 962 + 28. 682
=50Nand θ=tan−^1
(
28. 68
40. 96)
= 35 ◦Thus, the vector addition of components 40.96N and
28.68N is 50N at 35◦)
Problem 5. Resolve the velocity vector of 20m/s
at an angle of− 30 ◦to the horizontal into horizontal
and vertical components.The horizontal component of the 20m/s velocity,
0 a=20cos(− 30 ◦)=17.32m/s
The vertical component of the 20m/s velocity,
ab=20sin(− 30 ◦)=−10m/s
The horizontal and vertical components are shown in
Fig. 24.16.
308
20m/s^2 10m/s17.32m/sba
0Figure 24.16Problem 6. Resolve the displacement vector of
40m at an angle of 120◦into horizontal and vertical
components.Thehorizontal componentof the 40m displacement,
0 a=40cos120◦=−20.0m
The vertical componentof the 40m displacement,
ab=40sin120◦=34.64m
The horizontal and vertical components are shown in
Fig. 24.17.2 20.0N40N1208
034.64N
abFigure 24.1724.6 Addition of vectors by calculation
Two force vectors,F 1 andF 2 , are shown in Fig. 24.18,
F 1 being at an angle ofθ 1 andF 2 being at an angle
ofθ 2.F 1 F 2
F^1sin
1F^2sin
2HV 1
2F 2 cos 2F 1 cos 1Figure 24.18