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Lect 1_TMT 20303.pptx
1. Mohd Arif Fahmi bin Rosli
Lecture 1: Introduction & Vector Function of One Variable
2. Scalar and Vector
If r = axi + ayj + azk, then modulus of |r| is…
Direction cosines [l, m, n] are the cosines of the angles between vector r and the
axes:
Let r = axi + ayj + azk, then
l = cos α =
ax
|r|
; m = cos β =
ay
|r|
; n = cos γ =
az
|r|
l2 + m2 + n2 = 1
Scalar product / dot product
A · B = AB cos θ = |A||B| cos θ = axbx + ayby + azbz = B · A
3. Vector product / cross product
|A x B| = AB sin θ
A x B = = (aybz – azby)i – (axbz – azbx)j + (axbz – azbx)k = -(B x A)
Angle between two vectors
cos θ = l1l2 + m1m2 + n1n2
Where l1, m1, n1 and l2, m2, n2 are the direction cosines of vector
r1 and r2 respectively.
4. If i, j, k are unit vectors in the directions OX, OY, OZ, respectively. Vector r is in
direction of OP and P is the point (3, 2, 6). Determines direction cosines of the
vector r, (i.e. l, m, n)
6. A · (B x C)
A · (B x C) = =
Properties of triple products
1. A · (B x C) = C · (A x B) = B · (C x A) CYCLIC ORDER
2. B · (A x C) ≠ A · (B x C) = -A · (B x C) NOT IN CYCLIC ORDER
3. A · (B x A) = B · (A x B) = C · (A x C) = 0 TWO VECS ARE IDENTICAL
7. Determination of Coplanar
The magnitude of scalar triple product |A · (B x C)| is equal to the volume of the
parallelepiped.
A · (B x C) = A · (BC sin θ n) = ABC sin θ cos ϕ, where θ is the angle between B
and C and ϕ is the angle between A and n.
Therefore, |A · (B x C)|= ABC |sin θ cos ϕ|
BC |sin θ| is the parallelogram area
A|cos ϕ| is the altitude/ height of the parallelepiped.
8. Consequently, if A · (B x C) = 0, then the volume of the parallelepiped is zero
and those vectors are coplanar
9. A x (B x C)
Then (B x C) is a vector perpendicular to the plane of B and C and A x (B x
C) is a vector perpendicular to the plane containing A and (B x C), i.e.
coplanar with B and C.
Thus,
10. Also,
Proof can be seen on Appendix K.A. Stroud, Dexter J. Booth.(2007). Advanced Engineering
Mathematics, 6th Edition.
11. If A is a vector and depends on the scalar variable t, time, then A can be
represented as A(t) and A is said to be a function of t.
Differentiating A(t) with respect to t, gives..
Not only with respect to t, differentiation also can be done with respect to other
such u.
12. Let’s visualise
If a position vector OP moves to OQ when u becomes u + δu,
then as δu → 0, the direction of the chord PQ becomes that of
the tangent to the curve at P
i.e. the direction of
d𝐀
d𝑢
is along the tangent to the locus of P.
Details can be found in K.A. Stroud, Dexter J. Booth (2013)
Engineering Mathematics, 7th Edition. Palgrave Macmillan. (page 322)
13. Let r(t) = (cos t, sint, t)
1. Sketch and describe the curve associated with r
2. If particle travels along this curve (with t representing time) then calculate r’(t)
and show that its speed is constant