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Course by: Sunil Kumar Singh. E-mail the author

# Vector product (application)

Module by: Sunil Kumar Singh. E-mail the author

Summary: Solving problems is an essential part of the understanding process.

Questions and their answers are presented here in the module text format as if it were an extension of the treatment of the topic. The idea is to provide a verbose explanation, detailing the application of theory. Solution presented is, therefore, treated as the part of the understanding process – not merely a Q/A session. The emphasis is to enforce ideas and concepts, which can not be completely absorbed unless they are put to real time situation.

## Representative problems and their solutions

We discuss problems, which highlight certain aspects of the vector product. For this reason, questions are categorized in terms of the characterizing features of the subject matter :

• Condition of parallel vectors
• Unit vector of cross product
• Nature of vector product
• Evaluation of vector product
• Area of parallelogram

### Condition of parallel vectors

#### Example 1

Problem : Determine whether vectors 2ij + 2k and 3i – 3j + 6k are parallel to each other?

Solution : If the two vectors are parallel, then ratios of corresponding components of vectors in three coordinate directions are equal. Here,

a x b x = 2 3 a y b y = 1 3 a z b z = 1 3 a x b x = 2 3 a y b y = 1 3 a z b z = 1 3

The ratios are, therefore, not equal. Hence, given vectors are not parallel to each other.

### Unit vector of cross product

#### Example 2

Problem : Find unit vector in the direction perpendicular to vectors i + j – 2k and 2ij + 3k.

Solution : We know that cross product of two vectors is perpendicular to each of vectors. Thus, unit vector in the direction of cross product is perpendicular to the given vectors. Now, unit vector of cross product is given by :

n = a × b | a × b | n = a × b | a × b |

Here,

a × b = | i j k 1 1 - 2 2 - 1 3 | a × b = | i j k 1 1 - 2 2 - 1 3 |

a × b = { 1 x 3 - ( - 2 x - 1 ) } i + { ( 2 x - 2 ) - 1 x 3 } j + { ( 1 x - 1 ) - 1 x 2 } k a × b = i - 7 j - 3 k a × b = { 1 x 3 - ( - 2 x - 1 ) } i + { ( 2 x - 2 ) - 1 x 3 } j + { ( 1 x - 1 ) - 1 x 2 } k a × b = i - 7 j - 3 k

| a × b | = { 1 2 + ( - 7 ) 2 + ( - 3 ) 2 } | a × b | = { 1 2 + ( - 7 ) 2 + ( - 3 ) 2 }

n = 1 ( 59 ) x ( i - 7 j - 3 k ) n = 1 ( 59 ) x ( i - 7 j - 3 k )

### Nature of vector product

#### Example 3

Problem : Verify vector equality B = C, if AxB = AxC.

Solution : Let θ 1 θ 1 and θ 2 θ 2 be the angles for first and second pairs of cross products. Then,

A × B = A × C AB sin θ 1 n 1 = AC sin θ 2 n 2 B sin θ 1 n 1 = C sin θ 2 n 2 A × B = A × C AB sin θ 1 n 1 = AC sin θ 2 n 2 B sin θ 1 n 1 = C sin θ 2 n 2

It is clear that B=C is true only when sin θ 1 n 1 = sin θ 2 n 2 sin θ 1 n 1 = sin θ 2 n 2 . It is always possible that the angles involved or the directions of cross products are different. Thus, we can conclude that B need not be equal to C.

### Evaluation of vector product

#### Example 4

Problem : If a.b = |axb| for unit vectors a and b, then find the angle between unit vectors.

Solution : According to question,

a . b = | a × b | ab cos θ = ab sin θ tan θ = 1 x 1 x tan 45 ° θ = 45 ° a . b = | a × b | ab cos θ = ab sin θ tan θ = 1 x 1 x tan 45 ° θ = 45 °

#### Example 5

Problem : Prove that :

| a . b | 2 - | a × b | 2 = a 2 x b 2 x cos | a . b | 2 - | a × b | 2 = a 2 x b 2 x cos

Solution : Expanding LHS, we have :

| a . b | 2 - | a × b | 2 = ( ab cos θ ) 2 - ( ab sin θ ) 2 = a 2 b 2 ( cos 2 θ - sin 2 θ ) | a . b | 2 - | a × b | 2 = = a 2 b 2 cos 2 θ | a . b | 2 - | a × b | 2 = ( ab cos θ ) 2 - ( ab sin θ ) 2 = a 2 b 2 ( cos 2 θ - sin 2 θ ) | a . b | 2 - | a × b | 2 = = a 2 b 2 cos 2 θ

### Area of parallelogram

#### Example 6

Problem : The diagonals of a parallelogram are represented by vectors 3i+j+k and i-j-k. Find the area of parallelogram.

Solution : The area of parallelogram whose sides are formed by vectors a and b, is given by :

Area = | a × b | Area = | a × b |

However, we are given in question vectors representing diagonals – not the sides. But, we know that the diagonals are sum and difference of vectors representing sides of a parallelogram. It means that :

a + b = 3 i + j + k a + b = 3 i + j + k

and

a - b = i - j - k a - b = i - j - k

Now the vector product of vectors representing diagonals is :

( a + b ) × ( a - b ) = a × a - a × b + b × a + b × ( - b ) = - a × b + b × a ( a + b ) × ( a - b ) = a × a - a × b + b × a + b × ( - b ) = - a × b + b × a

Using anti-commutative property of vector product,

( a + b ) × ( a - b ) = - 2 a × b ( a + b ) × ( a - b ) = - 2 a × b

Thus,

a × b = - 1 2 x ( a + b ) × ( a - b ) a × b = - 1 2 x ( a + b ) × ( a - b )

a × b = - 1 2 | i j k 3 1 1 1 - 1 - 1 | a × b = - 1 2 | i j k 3 1 1 1 - 1 - 1 |

a × b = - 1 2 x { ( 1 x - 1 - 1 x - 1 ) i + ( 1 x 1 - 3 x - 1 ) j + ( 3 x - 1 - 1 x 1 ) k } a × b = - 1 2 x ( 4 j - 4 k ) a × b = - 2 j + 2 k a × b = - 1 2 x { ( 1 x - 1 - 1 x - 1 ) i + ( 1 x 1 - 3 x - 1 ) j + ( 3 x - 1 - 1 x 1 ) k } a × b = - 1 2 x ( 4 j - 4 k ) a × b = - 2 j + 2 k

The volume of the parallelogram is :

| a × b | = { ( - 2 ) 2 + 2 2 } = 2 2 units | a × b | = { ( - 2 ) 2 + 2 2 } = 2 2 units

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