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LECTURE # 2 & 3
SCALARS & VECTORS
1
SCALARS:
• A scalar is any positive or negative quantity that can be
completely specified by its magnitude for example length,
mass, time.
2
VECTORS:
• A vector is any physical quantity that requires both a magnitude and a direction
for its complete description for example force.
• It is graphically shown by an arrow, the length of the arrow represents the
magnitude of the vector and the angle between the vector and a fixed axis
defines the direction of its line of action.
3
MULTIPLICATION & DIVISION OF A VECTOR BY A
SCALAR
• If a vector is multiplied or divided by a positive scalar, its magnitude is increased
or decreased by that amount. If it is multiplied or divided by a negative scalar, it
will also change the direction sense of the vector.
4
VECTOR ADDITION USING PARALLELOGRAM RULE
• First join the tails of the vectors to make them concurrent.
• From the head of B draw a line parallel to vector A. Draw another line from the
head of vector A parallel to vector B. Where the two lines intersect is point P.
• The diagonal of this parallelogram that extends to point P is the resultant R.
• R = A + B
5
VECTOR ADDITION USING TRIANGLE RULE
• Vector addition is done using a triangle rule. Vector A is added to B using the
head to tail rule.
• Vector A is added to vector B by joining the head of vector A with the tail of
vector B.
• The resultant vector R extends from the tail of vector A to the head of vector B.
• R= A+B = B+ A
6
VECTOR SUBTRACTION
• R = A – B
• Reverse the direction of vector B and then using the triangle rule we add the two
vectors as R = A – B = A + (-B)
7
FORCES IN 2D – RESULTANT OF FORCES
• Finding Resultant of Forces:
• FR = F1 + F2 (Can be added using parallelogram rule (b) or triangular rule (c))
8
ADDITION OF MORE THAN TWO FORCES
• If more than two forces are to be added, successive applications of parallelogram
rule can be applied. For example FR = F1 +F2 + F3 = (F1+F2) + F3
9
COMPONENTS OF FORCES IN 2D
• Force F is to be resolved in two components along the axis u & v
• Using parallelogram, draw two lines from the tip of force F parallel to axis u and
axis v respectively.
• These parallel lines intersect with the axis u & v, and the components of forces
are established by joining the tail of the force F to these intersection points.
10
COSINE & SINE LAW11
PROPERTIES OF A PARALLELOGRAM
There are four important properties of parallelograms to
know:
• Opposite sides are congruent (AB = DC).
• Opposite angels are congruent (D = B).
• Consecutive angles are supplementary (A + D = 180°).
• If one angle is right, then all angles are right.
Note:
• Two line segments are congruent if they have the same
length.
• Two angles are congruent if they have the same measure.
12
NUMERICAL EXAMPLE
• The screw eye is subjected to two forces F1 & F2. Determine the magnitude and
direction of the resultant force
13
14
ADDITION OF A SYSTEM OF COPLANAR FORCES
SCALAR NOTATION
• F = Fx + Fy
• Fx = F cosø and Fy = F
sinø
•
𝐹𝑥
𝐹
=
𝑎
𝑐
and
•
𝐹𝑦
𝐹
=
𝑏
𝑐
15
CARTESIAN VECTOR NOTATIONS
• F = Fx i + Fy j
16
17
NUMERICAL
EXAMPLE
18
VECTORS IN 3D
• Right-Handed Coordinate System.
• Thumb point to the positive z axis, the fingers curl from positive x axis towards
positive y axis
19
VECTORS IN 3D
• Rectangular components of
vectors:
• A = Ax + Ay + Az
20
• Cartesian vector representation:
• A = Ax i + Ay j + Az k
MAGNITUDE & DIRECTION OF CARTESIAN VECTOR
IN 3D
• Magnitude
21
• Direction
UNIT VECTOR22
UA is a unit vector of A, in the direction of A.
Unit vector is the vector divided by its magnitude
POSITION VECTOR
• A position vector r is defined as a fixed vector which locates a point
in space relative to another point. For example if r extends from
origin to point P(x,y,z).
• r = xi + yj + zk
23
• In more general case. the position vector may be directed from point A to point B
in pace.
24 POSITION VECTOR
POSITION VECTOR (CONTINUED)25
• Force F has the same direction and sense as the
position vector r directed from point A towards B.
This common direction is specified by unit vector u =
r/r
ADDITION OF CARTESIAN VECTORS IN 3D26
27
DOT PRODUCT28
Dot product is the product of two
magnitudes of vectors & the cosine angle
between them The result is a scalar
quantity
CARTESIAN VECTOR29
NUMERICAL EXAMPLE30
31

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Lecture basic mechanical engineering

  • 1. LECTURE # 2 & 3 SCALARS & VECTORS 1
  • 2. SCALARS: • A scalar is any positive or negative quantity that can be completely specified by its magnitude for example length, mass, time. 2
  • 3. VECTORS: • A vector is any physical quantity that requires both a magnitude and a direction for its complete description for example force. • It is graphically shown by an arrow, the length of the arrow represents the magnitude of the vector and the angle between the vector and a fixed axis defines the direction of its line of action. 3
  • 4. MULTIPLICATION & DIVISION OF A VECTOR BY A SCALAR • If a vector is multiplied or divided by a positive scalar, its magnitude is increased or decreased by that amount. If it is multiplied or divided by a negative scalar, it will also change the direction sense of the vector. 4
  • 5. VECTOR ADDITION USING PARALLELOGRAM RULE • First join the tails of the vectors to make them concurrent. • From the head of B draw a line parallel to vector A. Draw another line from the head of vector A parallel to vector B. Where the two lines intersect is point P. • The diagonal of this parallelogram that extends to point P is the resultant R. • R = A + B 5
  • 6. VECTOR ADDITION USING TRIANGLE RULE • Vector addition is done using a triangle rule. Vector A is added to B using the head to tail rule. • Vector A is added to vector B by joining the head of vector A with the tail of vector B. • The resultant vector R extends from the tail of vector A to the head of vector B. • R= A+B = B+ A 6
  • 7. VECTOR SUBTRACTION • R = A – B • Reverse the direction of vector B and then using the triangle rule we add the two vectors as R = A – B = A + (-B) 7
  • 8. FORCES IN 2D – RESULTANT OF FORCES • Finding Resultant of Forces: • FR = F1 + F2 (Can be added using parallelogram rule (b) or triangular rule (c)) 8
  • 9. ADDITION OF MORE THAN TWO FORCES • If more than two forces are to be added, successive applications of parallelogram rule can be applied. For example FR = F1 +F2 + F3 = (F1+F2) + F3 9
  • 10. COMPONENTS OF FORCES IN 2D • Force F is to be resolved in two components along the axis u & v • Using parallelogram, draw two lines from the tip of force F parallel to axis u and axis v respectively. • These parallel lines intersect with the axis u & v, and the components of forces are established by joining the tail of the force F to these intersection points. 10
  • 11. COSINE & SINE LAW11
  • 12. PROPERTIES OF A PARALLELOGRAM There are four important properties of parallelograms to know: • Opposite sides are congruent (AB = DC). • Opposite angels are congruent (D = B). • Consecutive angles are supplementary (A + D = 180°). • If one angle is right, then all angles are right. Note: • Two line segments are congruent if they have the same length. • Two angles are congruent if they have the same measure. 12
  • 13. NUMERICAL EXAMPLE • The screw eye is subjected to two forces F1 & F2. Determine the magnitude and direction of the resultant force 13
  • 14. 14
  • 15. ADDITION OF A SYSTEM OF COPLANAR FORCES SCALAR NOTATION • F = Fx + Fy • Fx = F cosø and Fy = F sinø • 𝐹𝑥 𝐹 = 𝑎 𝑐 and • 𝐹𝑦 𝐹 = 𝑏 𝑐 15
  • 16. CARTESIAN VECTOR NOTATIONS • F = Fx i + Fy j 16
  • 17. 17
  • 19. VECTORS IN 3D • Right-Handed Coordinate System. • Thumb point to the positive z axis, the fingers curl from positive x axis towards positive y axis 19
  • 20. VECTORS IN 3D • Rectangular components of vectors: • A = Ax + Ay + Az 20 • Cartesian vector representation: • A = Ax i + Ay j + Az k
  • 21. MAGNITUDE & DIRECTION OF CARTESIAN VECTOR IN 3D • Magnitude 21 • Direction
  • 22. UNIT VECTOR22 UA is a unit vector of A, in the direction of A. Unit vector is the vector divided by its magnitude
  • 23. POSITION VECTOR • A position vector r is defined as a fixed vector which locates a point in space relative to another point. For example if r extends from origin to point P(x,y,z). • r = xi + yj + zk 23
  • 24. • In more general case. the position vector may be directed from point A to point B in pace. 24 POSITION VECTOR
  • 25. POSITION VECTOR (CONTINUED)25 • Force F has the same direction and sense as the position vector r directed from point A towards B. This common direction is specified by unit vector u = r/r
  • 26. ADDITION OF CARTESIAN VECTORS IN 3D26
  • 27. 27
  • 28. DOT PRODUCT28 Dot product is the product of two magnitudes of vectors & the cosine angle between them The result is a scalar quantity
  • 31. 31