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Physics · Ch 2 — Mathematical Methods

Resolution of vectors

2.4

Resolution of vectors

Just as two or more vectors can be combined into a single resultant vector, a single vector can conversely be expressed as the sum of two or more vectors along chosen fixed directions:

V⃗=V1n^1+V2n^2+V3n^3— (2.11)\vec V = V_1\hat n_1+V_2\hat n_2+V_3\hat n_3 \qquad \text{--- (2.11)}

where n^1,n^2,n^3\hat n_1,\hat n_2,\hat n_3 are unit vectors along the chosen directions and V1,V2,V3V_1, V_2, V_3 are called the components of V⃗\vec V along those directions. This process of splitting a vector into its components is called resolution of the vector. Components can, in principle, be found along any set of directions, but when the chosen directions are mutually perpendicular, the components are called rectangular components.

Rectangular components in two dimensions. Consider a vector R⃗=OC⃗\vec R = \vec{OC} starting at the origin of a rectangular coordinate system. Dropping perpendiculars from C to the x-axis (meeting it at A) and to the y-axis (meeting it at B) gives the two rectangular components RxR_x and RyR_y of R⃗\vec R along the x- and y-axes. By the parallelogram law,

R⃗=R⃗x+R⃗y=Rxi^+Ryj^\vec R = \vec R_x+\vec R_y = R_x\hat i+R_y\hat j

If θ\theta is the angle R⃗\vec R makes with the x-axis, then

Rx=Rcos⁡θ— (2.12),Ry=Rsin⁡θ— (2.13)R_x = R\cos\theta \qquad \text{--- (2.12)}, \qquad R_y = R\sin\theta \qquad \text{--- (2.13)}

Squaring and adding these gives the magnitude of R⃗\vec R:

R=Rx2+Ry2— (2.14)R = \sqrt{R_x^2+R_y^2} \qquad \text{--- (2.14)}

and the direction of R⃗\vec R is

θ=tan⁡−1(RyRx)— (2.15)\theta = \tan^{-1}\left(\dfrac{R_y}{R_x}\right) \qquad \text{--- (2.15)} …

Figure 2.8Resolution of a vector into rectangular components

What this figure shows. A rectangular (x-y) coordinate system with origin O. A vector R⃗=OC⃗\vec R=\vec{OC} is drawn from the origin to point C somewhere in the plane, at angle θ\theta to the x-axis. Perpendiculars are dropped from C to meet the x-axis at point A and the y-axis at point B, so that OA⃗\vec{OA} is the rectangular component R⃗x\vec R_x along the x-axis and OB⃗\vec{OB} is the rectangular component R⃗y\vec R_y along the y-axis (the dashed construction lines from C to A and C to B complete a rectangle OACB with OC as its diagonal). The angle θ\theta between R⃗\vec R and the x-axis is marked at O. No numeric coordinate values are pri …

Misc Ex.2.4Unit vector along a given vector

Worked out. Given the vector V⃗=3i^+4j^\vec V = 3\hat i+4\hat j, the problem asks for the unit vector pointing in the same direction as V⃗\vec V. The method first computes the magnitude ∣V⃗∣=32+42=5|\vec V|=\sqrt{3^2+4^2}=5, then divides the vector by its own magnitude, V^=V⃗/∣V⃗∣\hat V = \vec V/|\vec V|, to obtain a vector of magnitude exactly 1 pointing the same way — a direct, concrete application of the general unit-vector de …

Misc Ex.2.5Comparing magnitudes of two vectors

Worked out. Given two vectors a⃗=i^+2j^\vec a = \hat i+2\hat j and b⃗=2i^+j^\vec b = 2\hat i+\hat j, the problem asks for their magnitudes, and whether the two vectors are equal. The method computes ∣a⃗∣=12+22=5|\vec a|=\sqrt{1^2+2^2}=\sqrt5 and ∣b⃗∣=22+12=5|\vec b|=\sqrt{2^2+1^2}=\sqrt5 — the magnitudes turn out to be equal — but then checks the EQUALITY-OF-VECTORS condition (corresponding components must match, ax=bxa_x=b_x and ay=bya_y=b_y), finding ax≠bxa_x\ne b_x and ay≠bya_y\ne b_y, so despite having equal magnitude the two vectors are NOT …