Keeping one vector constant, if direction of other to be added in the first vector is changed continuously,tip of the resultant vector describes a circle. In the following figure vector ra is kept constant. Whenvector rb added to ra changes its direction, the tip of the resultant vector =+rrrr ab describes circle ofradius b with its center at the tip of vector ar. Maximum angle between vector ar and the resultant=+rrrr ab is

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Published July 1, 2025
Vector Algebra
Geometry of Vectors
Resultant of Two Vectors

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Detailed Explanation

1. Visualising the triangle

Placing vectors tip-to-tail forms a triangle O-A-R:

  • OA=aOA = a (length of ra\vec r_a)
  • AR=bAR = b (length of rb\vec r_b)
  • OR=ROR = |\vec R| (length of the resultant)

The angle we care about is φ=AOR\varphi = \angle AOR – the angle at O between ra\vec r_a and R\vec R. It is the angle opposite the fixed side AR=bAR = b.

2. Using the cosine rule at the required angle

With bb known and aa fixed, only the third side OROR can change while RR sweeps the circle.

From the cosine rule on triangle O-A-R at angle φ\varphi:

b2=a2+OR22aORcosφ b^{2} = a^{2} + OR^{2} - 2a\,OR\,\cos\varphi

Solve for cosφ\cos\varphi:

cosφ=a2+OR2b22aOR\cos\varphi = \frac{a^{2} + OR^{2} - b^{2}}{2a\,OR}

Since φ\varphi gets larger when cosφ\cos\varphi gets smaller, we need the minimum value of cosφ\cos\varphi over the allowed range of OROR.

3. Allowed range of OROR

Because OROR is the third side of a triangle with sides aa and bb:

abORa+b|a-b| \le OR \le a+b

4. Extremising cosφ\cos\varphi

Treat f(x)=a2+x2b22ax,xORf(x)=\frac{a^{2}+x^{2}-b^{2}}{2ax},\quad x\equiv OR

Differentiate and set f(x)=0f'(x)=0:

ddxf(x)=12aa2b22ax2=0    x2=a2b2\frac{\mathrm d}{\mathrm dx}f(x)=\frac{1}{2a}-\frac{a^{2}-b^{2}}{2ax^{2}}=0 \;\Longrightarrow\; x^{2}=a^{2}-b^{2}

So an interior extremum exists only if bab\le a:

  • When bab\le a : ORopt=a2b2OR_{\text{opt}}=\sqrt{a^{2}-b^{2}} lies inside the allowed interval.
  • When b>ab>a : the interior root is impossible; the minimum cosφ\cos\varphi occurs at the endpoint OR=ab=baOR=|a-b|=b-a.

5. Evaluate the maximum angle

Case 1: bab \le a

Insert OR=a2b2OR=\sqrt{a^{2}-b^{2}} into cosφ\cos\varphi:

cosφmin=a2b2aa2b2=a2b2a\cos\varphi_{\text{min}}=\frac{a^{2}-b^{2}}{a\sqrt{a^{2}-b^{2}}}=\frac{\sqrt{a^{2}-b^{2}}}{a}

Hence

φmax=arccos ⁣(a2b2a)    or    sinφmax=ba\boxed{\varphi_{\max}=\arccos\!\left(\frac{\sqrt{a^{2}-b^{2}}}{a}\right)} \;\;\text{or}\;\;\boxed{\sin\varphi_{\max}=\frac{b}{a}}

Case 2: bab \ge a

At OR=baOR=b-a, the calculation gives cosφmin=1\cos\varphi_{\min}=-1 so φmax=180\varphi_{\max}=180^{\circ}. The resultant can point exactly opposite to ra\vec r_a.

Most JEE questions implicitly assume b<ab<a to keep the answer neat, therefore you usually quote

φmax=sin1 ⁣(ba)(valid when ba).\boxed{\varphi_{\max}=\sin^{-1}\!\left(\dfrac{b}{a}\right)}\quad (\text{valid when } b\le a).

Simple Explanation (ELI5)

What’s going on here?

Imagine you stand at point O and hold a stick of fixed length a. That stick points to point A – this is your constant vector ra\vec r_a.

Now you get a second stick of length b (vector rb\vec r_b). One end is always tied to point A, but you are free to swing its other end in any direction so that the tip traces a perfect circle of radius b around A.

Every time you add the two sticks tip-to-tail, you get a new combined stick (the resultant R=ra+rb\vec R = \vec r_a + \vec r_b) that runs from O to some point R on that circle.

The question:
How far can the new stick lean away from the old fixed stick?
In other words, what is the biggest angle between ra\vec r_a and the resultant R\vec R while you keep swinging rb\vec r_b all around?

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Step-by-Step Solution

Step-by-step JEE-style solution

Let ra=a|\vec r_a|=a and rb=b|\vec r_b|=b.

  1. Form triangle OAROAR with sides OA=a,  AR=b,  OR=ROA=a,\; AR=b,\; OR=|\vec R|

  2. Angle between ra\vec r_a and R\vec R is φ=AOR\varphi = \angle AOR.

  3. Apply cosine rule at AOR\angle AOR:

b2=a2+OR22aORcosφ(1) b^{2}=a^{2}+OR^{2}-2a\,OR\cos\varphi\tag{1}
  1. Solve for cosφ\cos\varphi:
cosφ=a2+OR2b22aOR(2)\cos\varphi=\frac{a^{2}+OR^{2}-b^{2}}{2a\,OR}\tag{2}
  1. The variable side OROR can vary in the interval abORa+b|a-b|\le OR\le a+b.

  2. Minimise cosφ\cos\varphi (to maximise φ\varphi). Differentiate (2):

dd(OR)cosφ=12aa2b22aOR2=0    OR2=a2b2\frac{\mathrm d}{\mathrm d(OR)}\cos\varphi=\frac{1}{2a}-\frac{a^{2}-b^{2}}{2a\,OR^{2}}=0 \implies OR^{2}=a^{2}-b^{2}
  1. Validity: this root exists only if bab\le a.

  2. Substituting OR=a2b2OR=\sqrt{a^{2}-b^{2}} into (2):

cosφmin=a2+(a2b2)b22aa2b2=a2b2a\cos\varphi_{\min}=\frac{a^{2}+(a^{2}-b^{2})-b^{2}}{2a\sqrt{a^{2}-b^{2}}}=\frac{\sqrt{a^{2}-b^{2}}}{a}
  1. Therefore
sinφmax=ba,so φmax=sin1 ⁣(ba)  (ba)\boxed{\sin\varphi_{\max}=\frac{b}{a}},\quad\text{so }\boxed{\varphi_{\max}=\sin^{-1}\!\left(\dfrac{b}{a}\right)}\;(b\le a)
  1. If b>ab>a, minimum OR=baOR=b-a gives cosφmin=1\cos\varphi_{\min}=-1 hence φmax=180\varphi_{\max}=180^{\circ}.

Hence, under the usual condition b<ab<a (most exam problems), the sought maximum angle is sin1(b/a)\boxed{\sin^{-1}(b/a)}.

Examples

Example 1

Radio antennas using two perpendicular signals – vector addition of field strengths.

Example 2

Aircraft navigation: combining a fixed wind vector with a variable thrust vector to find heading limits.

Example 3

Physics: maximum deflection of a charged particle experiencing a fixed electric field plus a rotating magnetic force.

Visual Representation

References

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