Addition and Subtraction of Vectors

 

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Scalar quantities can be added algebraically. for example, 4 kg of sugar and 3 kg of sugar, when combined together in any way, always give 7 kg of sugar. This is not always there in case of vectors, since they possess directions, also, in addition to the magnitudes.

Following are the some points regarding vector addition:

(a) Addition or composition of vectors means finding the resultant of a number of vectors acting on a body.

(b) The vectors can be added geometrically and not algebraically.

(c) Vectors, whose resultant is to be calculated behave independent of each other. In other words, each vector behaves as if the other vectors were absent.

(d) Vector addition is commutative.

So,\vec{a}+\vec{b} =\vec{b}+\vec{a} 

It means that the law of addition of vectors is independent of the order of vectors.

Graphical Representation of Vector Addition

                         geometrical-method 

To find \vec{a}+\vec{b} , shift  vector \vec{b} such that its initial point coincides with the terminal point of vector \vec{a}. Now, the vector whose initial point coincides with the initial point of vector \vec{a} , and terminal point coincides with the terminal point of vector \vec{b}  represents \vec{a}+\vec{b} as shown in the above figure. 

To find \vec{b}+\vec{a}, shift \vec{a} such that its initial point coincides with the terminal point \vec{b}. A vector whose initial point coincides with the initial point of \vec{b} and terminal point coincides with the terminal point of \vec{a} represents \vec{b}+\vec{a}.


                       addition-of-two-vectors 

Triangle’s Law of Vector Addition

It is a law for the addition of two vectors. It can be stated as follows:

“If two vectors are represented (in magnitude and direction) by the two sides of a triangle, taken in the same order, then their resultant in represented (in magnitude and direction) by the third side of the triangle taken in opposite order.”

Consider two vectors \vec{A} and \vec{B} [Below Figure] acting, simultaneously, on a body. Represent vector \vec{B} by the line \vec{OB}. At A draw another line \vec{OA} representing \vec{B}. Join OC. Then \vec{OC} (=\vec{R}) gives the resultant of  \vec{A} and \vec{B}. It can be noted that  \vec{OB} and \vec{BC} are in same order while \vec{R} is in opposite order. This is in accordance with the triangle’s law.

So, \vec{R} = \vec{OC}

         = \vec{A} + \vec{B}

        = \vec{B}+\vec{A}

It is, further, clear that the order of vectors in vector addition is immaterial. So, vector addition is commutative. 

If θ is the angle between \vec{A} and \vec{B}, then the magnitude of the resultant vector \vec{R} will be,

R = √(A2+ B2 )+ 2AB cos θ

and

if ? is the angle between \vec{B} and \vec{R} then,

? = tan-1 [A sinθ/(B+A cosθ)]  

If three vectors acting, simultaneously, on a particle can be represented by the three sides of a triangle taken in the same order, then the particle will remain in equilibrium. 

Mathematically, it can be expressed as follows:

\vec{A}+\vec{B}+\vec{C}=0

Law of Parallelogram of Vectors

The addition of two vectors may also be understood by the law of parallelogram. It states that “if two vectors acting simultaneously at a point are represented in magnitude and direction by the two sides of a parallelogram drawn from a point, their resultant is given in magnitude and direction by the diagonal of the parallelogram passing through that point.”

According to this law if two vectors \vec{P} and  \vec{Q} are represented by two adjacent sides of a parallelogram both pointing outwards as shown in the figure below , then the diagonal drawn through the intersection of the two vectors represents the resultant (i.e. vector sum of \vec{P} and  \vec{Q}). If Q is displacement from position AD to BC by displacing it parallel to itself, this method becomes equivalent to the triangle method. 

                              parallelogram-method 

In case of addition of two vectors by parallelogram method as shown in figure, the magnitude of resultant will be given by, 

                                       (AC)2 = (AE)2 + (EC)2 

                               or R2 = (P + Q cos θ)2 (Q sin θ)2

                               or R = √(P2+ Q2 )+ 2PQcos θ 

And the direction of resultant from vector P will be given by
 
                              tan ? = CE/AE = Qsinθ/(P+Qcosθ) 

                                  ? = tan-1 [Qsinθ/(P+Qcosθ)]  

Special Cases

(a) When  θ = 0°, cos θ = 1 , sin θ = 0°

Substituting for cos θ in equation R = √(P2+ Q2 )+ 2PQcos θ, we get,

R = √(P2+ Q2 )+ 2PQcos θ

   = (P+ Q)2

or R = P+Q (maximum)

Substituting for sin θ  and cos θ  in equation ? = tan-1 [Qsinθ/(P+Qcosθ)], we get,

? = tan-1 [Qsinθ/(P+Qcosθ)]  

   = tan-1 [(Q×0)/(P+(Q×1))]

  = tan-1(0)

 = 0°

The resultant of two vectors acting in the same directions is equal to the sum of the two. The direction of resultant coincides with those of the two vectors.

(b) When  θ = 180°, cos θ = -1 , sin θ = 0°

Substituting for cos θ in equation R = √(P2+ Q2 )+ 2PQcos θ, we get,

R = √(P2+ Q2 )+ 2PQ(-1)

  =√P2+ Q2 – 2PQ

   = (P –  Q)(minimum)

R = P – Q (minimum)

Substituting for sin θ  and cos θ  in equation ? = tan-1 [Qsinθ/(P+Qcosθ)], we get,

? = tan-1 [Qsinθ/(P+Qcosθ)]  

   = tan-1 [(Q×0)/(P+(Q×(-1)))]

  = tan-1(0)

 = 0°

This magnitude of the resultant of two vectors acting in opposite direction is equal to the difference of magnitudes of the two and represents the minimum value. The direction of the resultant is in the direction of the bigger one.

 (c) When  θ = 90°, cos θ = 0 , sin θ = 1

Substituting for cos θ in equation R = √(P2+ Q2 )+ 2PQcos θ, we get,

R = √(P2+ Q2 )+ (2PQ×0)

   = √P2+ Q2 

Substituting for sin θ  and cos θ  in equation ? = tan-1 [Qsinθ/(P+Qcosθ)], we get,

? = tan-1 [Qsinθ/(P+Qcosθ)]  

   = tan-1 [(Q×1)/(P+(Q×(0)))] 

  = tan-1(Q/P)

The resultant of two vectors acting at right angles to each other is equal to the square root of the sum of the squares of the magnitudes of the two vectors. Direction of the resultant depends upon their relative magnitudes. 

Vector Subtraction

The process of subtracting one vector from another is equivalent to adding, vectorially, the negative of the vector to be subtracted. Suppose there are two vectors \vec{A} and \vec{B}, shown in figure (A) and we have to subtract \vec{B} and \vec{A}. It is just the same thing as adding vectors – \vec{B} to \vec{A}. The resultant is shown in figure (B). 

                                   vector-subtraction 
                                              Figure (A) 

                                        resultant-of-vector-subtraction 
                                              Figure (B) 

          vector-subtract 
Properties of Vector Addition:-  Vector addition obeys the following properties.

1. Vector addition is commutative:- It means that the order of vectors to be added together does not affect the result of addition. If two vectors \vec{a} and \vec{b} are to be added together, then

       
                 example-of-vector-addition 
                                        vector-addition-is-commutative 
     2. Vector addition is associative:- While adding three or more vectors together, the mutual grouping of vector does not affect the result.

           Mathematically,

             example-of-associative-vector-addition

  3. Vector addition is distributive:- It means a scalar times the sum of two vectors is equal to the sum of the scalar times of the two vectors, individually.

      Mathematically,

      m\vec{a}+m\vec{b} = m(\vec{a}+\vec{b})

Geometrical Representation of Addition  of Vectors


                                    vector-addition-is-associative 
Magnitude and direction of \vec{a}+\vec{b}:-
Let angle between vector \vec{a} and \vec{b} be θ.
In the figure vector (\vec{OA}) = vector \vec{a} , vector (\vec{AB}) = vector \vec{b}
From Δ ADB,

                                 AD = b cos θ
                                  BD = b sin θ

                              magnitude-and-direction-of-vectors 
In right angled ΔODB,

                      OD = a + b cosθ
                     BD = b sin θ

                    Therefore, OB = √(OD2+BD2 )
                    => |a +b |=√(a2+b2+2ab cos θ)
                   |a +b |max   =  a+b   when θ = 2nπ

                   |a +b |min   =  |a – b|   when θ = (2n + 1)π
                                       (where n = 0, 1, 2, …..)
If a + b  is inclined at an angle α with vector a , then
tan α = ((b sin θ)/(a+b cosθ))

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