Multiplication of vector...p u vr uZ v B B u() W E upE W B uMB LAMI ’S THEOREM Contact :...
Transcript of Multiplication of vector...p u vr uZ v B B u() W E upE W B uMB LAMI ’S THEOREM Contact :...
Multiplication of vector
MULTIPLICATION OF VECTORS
Two types of multiplication:
1. Scalar (or dot) product of two vectors.
2. Vector (or cross) product of two vectors.
1. Scalar Product of Two Vectors
(1) Definition : The scalar product (or dot product) of two
vectors is defined as the product of the magnitude of two
vectors with cosine of angle between them.
Thus, if there are two vectors and having angle q
between them, then their scalar product written as is
defined as
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A B.A B
cosAB q.A B
(2) Properties : (i) It is always a scalar which is positive
if angle between the vectors is acute (i.e., < 90°) and
negative if angle between them is obtuse (i.e. 90°< q <
180°).
(ii) It is commutative, i.e.
(iii) It is distributive, i.e.
(iv) As by definitionwww.gangwarinstitue.com Contact : 8400-582-582, 8604-582-582
q
A
B
Fig. 0.10
. .A B B A
CABACBA ..)(.
qcos. ABBA
The angle between the vectors
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In
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In
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2. Geometrical interpretation of scalar product
Let OA & OB represent vectors a & b respectively.
Then,
a = |a| = |OA| = OA
b = |b| = |OB| = OB
Let, M, N be the feet of the
perpendiculars from A, B on OB, OA respectively.
Then, magnitude of projection of a on b
= OM = OA cosq ( cosq = OM/OA in DOMA)
= a cosq
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b
A N a O
M B
a.b = ab cosq = a(a cosq) = b. (projection of a on
b)
similarly magnitude of projection of b on a.
= ON = OB cosq ( cosq = ON/OB in DONB)
= b cosq
a.b = ab cosq = a(b cosq) = a. projection of b on a.
Thus a.b can be defined as the product of the
modulus of one vector and the projection of the
other vector upon it.
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(3) Example : (i) Work W : In physics for constant
force work is defined as,
…(i)
But by definition of scalar product of two vectors,
…(ii)
So from eqn (i) and (ii) i.e. work is the scalar
product of force with displacement.
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cosW Fs q
. cosF s Fs q
.W F s
In
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Magnetic flux through an area is given by
…(i)
But by definition of scalar product
...(ii)
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cosd Bds q
. cosB d s Bds q
q
sd
B
O
Fig. 0.11
(iv) Potential energy of a dipole U : If an electric
dipole of moment is situated in an electric field
or a magnetic dipole of moment in a field of
induction the potential energy of the dipole is
given by :
and
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p
E M
B
.EU p E .BU M B
VECTOR PRODUCT OF TWO VECTORS
(1) Definition : The vector product or cross product
of two vectors is defined as a vector having a
magnitude equal to the product of the magnitudes
of hand screw rule.
Thus, if and are two vectors, then their vector
product written as is a vector defined by
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C A B
A B
A B C
ˆsinC A B AB nq
The direction of i.e. is perpendicular to the plane containing
vectors and and in the sense of advance of a right handed screw
rotated from (first vector) to (second vector) through the
smaller angle between them. Thus, if a right handed screw whose
axis is perpendicular to the plane framed by and is rotated
from to through the smaller angle between them, then the
direction of advancement of the screw gives the direction of
i.e.
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Fig. 0.12
A B C
A B
A B
BA
BA
A B C
(2) Properties :
(i) Vector product of any two vectors is always a vector
perpendicular to the plane containing these two vectors,
i.e., orthogonal to both the vectors and though the
vectors and may or may not be orthogonal.
(ii) Vector product of two vectors is not commutative,
i.e., [but
Here it is worthy to note that
i.e. in case of vector and magnitudes are equal
but directions are opposite.www.gangwarinstitue.com Contact : 8400-582-582, 8604-582-582
A B
A B
A B B A ]B A
| | | | sinA B B A AB q
A B B A
(iii) The vector product is distributive when the order
of the vectors is strictly maintained, i.e.
(iv) The vector product of two vectors will be maximum
when i.e.,
i.e. vector product is maximum if the vectors are
orthogonal.
(v) The vector product of two non- zero vectors will be
minimum when minimum = 0, i.e.,
or 180°www.gangwarinstitue.com Contact : 8400-582-582, 8604-582-582
( )A B C A B A C
sin max 1,q 90oq
maxˆ[ ]A B AB n
| sin |q 0oq
min[ ] 0A B
i.e. if the vector product of two non-zero vectors
vanishes, the vectors are collinear.
(vi) The self cross product, i.e., product of a vector by
itself vanishes, i.e., is null vector
(vii) In case of unit vector so that
(viii) In case of orthogonal unit vectors, in
accordance with right hand screw rule :
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ˆsin0 0oA A AA n
ˆ ˆ 0n n ˆ ˆˆ ˆ ˆ ˆ 0i i j j k k
ˆˆ ˆ, ,i j k
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i
j
k
i
j
k
Fig. 0.13
(x) In terms of components
(3) Example : Since vector product of two vectors is a
vector, vector physical quantities (particularly
representing rotational effects) like torque, angular
momentum, velocity and force on a moving charge in a
magnetic field and can be expressed as the vector
product of two vectors. It is well – established in physics
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ˆˆ ˆ
x y z
x y z
i j k
A B A A A
B B B
ˆ( )y z z yi A B A B ˆˆ( ) ( )z x x z x y y xj A B A B k A B A B
(i) Torque
(ii) Angular momentum
(iii) Velocity
(iv) Force on a charged particle q moving with
velocity in a magnetic field is given by
(v) Torque on a dipole in a field
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r F
L r p
v r
v B ( )F q v B
E p E
B M B
LAMI’S THEOREM
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i.e. for any triangle the ratio of the sine of the angle
containing the side to the length of the side is a constant.
For a triangle whose three sides are in the same order
we establish the Lami's theorem in the following
manner. For the triangle shown
[All three sides are taken in order]
…(i)
…(ii)
Pre-multiplying both sides by
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0a b c
a b c
a
If
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If
Dividing through out by abc, we have
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sin sin sin
a b c
If a vector is perpendicular to the
vector Then the value of is;
(A) –1 (B) 1/2
(C) –1/2 (D) 1.
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ˆˆ ˆ2 3 8i j k
ˆˆ ˆ4 4 .j i k
01
A particle acted upon by constant forces
and is displaced from the point
to point . The total work done by the
forces in SI unit is;
(A) 20 (B) 24
(C) 50 (D) 30.
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ˆˆ ˆ4 3i j k ˆˆ ˆ3i j k
ˆˆ ˆ5 4i j k
02
ˆˆ ˆ2 3i j k
A body, constrained to move in the Y-direction is
subjected to a force given What
is the work done by this force in moving the body
a distance 10 m along the Y-axis;
(A) 20 J (B) 150 J
(C) 160 J (D) 190 J.
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ˆˆ ˆ( 2 15 15 ) .F i j k N
03
Vector which is perpendicular to is
(A) (B)
(C) (D) All of these.
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ˆ ˆ( cos sin )a i b jq q
ˆ ˆsin cosb i a jq q1 1ˆ ˆsin cosi ja b
q q
ˆ5k
04
If vector & are
functions of time, then the value to t at which they
are orthogonal to each other is;
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ˆ ˆcos sinA ti tj ˆ ˆcos sin2 2
t tB i j
05
A vector points vertically upward and points
towards north. The vector product is
(A) Zero
(B) Along west
(C) Along east
(D) Vertically downward
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A B
A B
06
If , then the value of is;
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| | 3( . )A B A B | |A B
07
The moment of the force, at (2, 0, –3)
about the point (2, –2, –2) is given;
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ˆˆ ˆ4 5 6F i j k
08
A angle between the vectors and is q. The
value of the triple product is
(A) A2B (b) Zero
(C) A2B sinq (d) A2B cosq
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A B
.( )A B A
09
What is the unit vector perpendicular to the
following vectors and
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ˆˆ ˆ2 2i j k ˆˆ ˆ6 3 2i j k
10
Which
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