Vectors - Properties of Scalar Product

  • The scalar product of two vectors is denoted by a dot (·) between the vectors.
  • The scalar product of two vectors is commutative: A · B = B · A.
  • The scalar product of two parallel vectors is equal to the product of their magnitudes: A · B = |A||B|.
  • The scalar product of two perpendicular vectors is zero: A · B = 0.
  • The scalar product of a vector with itself is equal to the square of its magnitude: A · A = |A|^2.

Vectors - Properties of Scalar Product (contd.)

  • The scalar product of two vectors can be expressed in terms of their components:
    • A · B = AₓBₓ + AᵧBᵧ + A₂B₂.
  • The scalar product can also be written using the magnitudes and angle between the vectors:
    • A · B = |A||B| cosθ.
  • If the value of the scalar product is positive, the angle between the vectors is acute.
  • If the value of the scalar product is negative, the angle between the vectors is obtuse.

Vectors - Properties of Scalar Product (contd.)

  • The scalar product of two vectors can be used to find the angle between them:
    • cosθ = (A · B) / (|A||B|).
  • The scalar product can also be written using the unit vectors i, j, and k:
    • A · B = AₓBₓ + AᵧBᵧ + A₂B₂ = |A||B| cosθ.
  • The angle between two vectors can be calculated as:
    • cosθ = (AₓBₓ + AᵧBᵧ + A₂B₂) / (|A||B|).

Example 1

Find the scalar product of two vectors A = 3i + 2j and B = 5i + 4j. Solution: A · B = (3)(5) + (2)(4) = 15 + 8 = 23.

Example 2

Calculate the angle between two vectors C = 4i + 3j and D = 2i - 2j. Solution: C · D = (4)(2) + (3)(-2) = 8 - 6 = 2. |C| = √(4² + 3²) = √(16 + 9) = √25 = 5. |D| = √(2² + (-2)²) = √(4 + 4) = √8. cosθ = C · D / (|C||D|) = 2 / (5√8) ≈ 0.1788. θ ≈ arccos(0.1788) ≈ 80.43 degrees.

Equation for Projection

The scalar product A · B can be used to find the projection of a vector A onto another vector B. Projection of A onto B = |A| cosθ = (A · B) / |B|.

Slide 11: Vectors - Properties of Scalar Product (contd.)

  • The scalar product of two vectors can also be negative when the vectors are in opposite directions.
  • The scalar product of two vectors can be used to find the work done by a force when it is applied along a certain direction.
  • The scalar product can be used to solve problems related to the equilibrium of a particle.
  • The scalar product can be used to calculate the distance between a point and a line.
  • The scalar product can be used to find the area of a parallelogram.

Slide 12: Example 3

Find the work done by a force of 10 N in displacing an object along a vector A = 3i + 4j. Solution: Work done = Force × Displacement × cosθ. Since the force and displacement are parallel, θ = 0 degrees. Work done = 10 × |A| × cos0 = 10 × √(3² + 4²) × 1 = 10 × 5 = 50 J.

Slide 13: Example 4

Calculate the area of a parallelogram with two adjacent sides A = 2i + j and B = 4i + 3j. Solution: Area of parallelogram = |A × B|. |A × B| = |(2)(3) - (1)(4)| = |6 - 4| = 2.

Slide 14: Unit Vectors

  • Unit vectors have a magnitude of 1.
  • The unit vectors in the x, y, and z directions are represented as i, j, and k, respectively.
  • Any vector can be expressed as a linear combination of the unit vectors.

Slide 15: Example 5

Express the vector C = 3i - 4j + 2k as a linear combination of the unit vectors i, j, and k. Solution: C = 3i - 4j + 2k.

Slide 16: Orthogonal Vectors

  • Orthogonal vectors are perpendicular to each other.
  • The dot product of orthogonal vectors is zero.
  • Two vectors A and B are orthogonal if their scalar product, A · B, is equal to zero.

Slide 17: Example 6

Check whether the vectors E = 3i - 2j + k and F = 4i + 6j - 5k are orthogonal. Solution: E · F = (3)(4) + (-2)(6) + (1)(-5) = 12 - 12 - 5 = -5. Since the scalar product is not equal to zero, the vectors E and F are not orthogonal.

Slide 18: Cross Product

  • The cross product of two vectors is denoted by the symbol × between the vectors.
  • The cross product of two vectors is not commutative: A × B = -B × A.
  • The cross product of two parallel vectors is equal to zero: A × B = -B × A = 0.

Slide 19: Cross Product (contd.)

  • The cross product of two vectors can be expressed in terms of their components:
    • A × B = (AᵧB₂ - A₂Bᵧ)i + (A₂Bₓ - AₓB₂)j + (AₓBᵧ - AᵧBₓ)k.
  • The cross product can also be written using the magnitudes and angle between the vectors:
    • |A × B| = |A||B| sinθ.
  • The cross product of two vectors gives a result that is orthogonal to both vectors.

Slide 20: Example 7

Find the cross product of two vectors G = 2i + j - 3k and H = 3i + 4j + 2k. Solution: G × H = [(1)(2) - (-3)(4)]i + [(-3)(3) - (2)(2)]j + [(2)(4) - (1)(3)]k = [2 - (-12)]i + [(-9) - 4]j + [8 - 3]k = 14i - 13j + 5k.

Slide 21: Application of Cross Product

  • The cross product of two vectors can be used to find the moment of a force.
  • The moment of a force is a measure of its tendency to rotate an object about an axis.
  • The magnitude of the moment of a force F about a point P is given by: |M| = |F||r| sinθ, where |F| is the magnitude of the force, |r| is the perpendicular distance from the point P to the line of action of the force, and θ is the angle between the force and the vector r.

Slide 22: Example 8

Find the moment of a force of 8 N about a point P, located at a distance of 5 m from the line of action of the force. The angle between the force and the vector r is 60 degrees. Solution: |M| = (8)(5) sin60 = (8)(5)(√3/2) = 20√3 Nm.

Slide 23: Scalar Triple Product

  • The scalar triple product of three vectors A, B, and C is denoted by (A × B) · C.
  • The scalar triple product can be used to find the volume of a parallelepiped.
  • The volume V of a parallelepiped formed by three vectors A, B, and C is given by: V = |(A × B) · C|.

Slide 24: Example 9

Find the volume of a parallelepiped with sides A = 3i + j - 2k, B = 2i + 4j + 5k, and C = -i + 2j + 3k. Solution: V = |(A × B) · C| = |(14i + 11j + 10k) · (-i + 2j + 3k)| = |(-14) + 22 + 30| = 38 cubic units.

Slide 25: Vector Triple Product

  • The vector triple product of three vectors A, B, and C is denoted by A × (B × C).
  • The vector triple product can be used to find the moment of a force about an axis.
  • The moment of a force F about an axis defined by a unit vector ĥ is given by: M = F × (r × ĥ), where r is the position vector of the point of application of the force relative to the axis.

Slide 26: Example 10

Find the moment of a force of 10 N about an axis defined by the unit vector ĥ = i + 2j - k, with the force applied at a point located at r = 2i - 3j + 4k. Solution: M = (10) × [(2i - 3j + 4k) × (i + 2j - k)] = (10) × [(6i + 2j - 3k) × (i + 2j - k)] = (10) × (-3i + 15j + 14k) = -30i + 150j + 140k Nm.

Slide 27: Distributive Property of Cross Product

  • The cross product of two vectors satisfies the distributive property over addition: A × (B + C) = (A × B) + (A × C).
  • Similarly, the cross product of a scalar and a vector satisfies the distributive property: k(A × B) = (kA) × B = A × (kB).

Slide 28: Example 11

Simplify the expression A × (B + C), where A = i + 2j - k, B = 4i - 3j + 2k, and C = 2i + j - 4k. Solution: A × (B + C) = (i + 2j - k) × [(4i - 3j + 2k) + (2i + j - 4k)] = (i + 2j - k) × (6i - 2j - 2k) = (i + 2j - k) × (-6i + 2j + 2k) = -10i + 10j + 10k.

Slide 29: Applications of Vectors in Physics

  • Vectors play a crucial role in various branches of physics, including mechanics, electromagnetism, and quantum mechanics.
  • They are used to represent physical quantities such as force, velocity, acceleration, electric field, magnetic field, and more.
  • Vectors help in understanding the direction, magnitude, and interactions of these physical quantities.
  • They are essential in solving problems related to motion, forces, energy, and other concepts in physics.

Slide 30: Summary

  • The scalar product of two vectors allows us to find the angle between them and solve problems related to work done, equilibrium, and distance calculations.
  • The cross product of two vectors helps in finding the moment of a force, volume of a parallelepiped, and moment of a force about an axis.
  • Both scalar and vector triple products have applications in physics.
  • Vectors have widespread applications in various branches of physics and are crucial for understanding and solving problems in the subject.