Multivariable-Calculus Ā· Unit 17 Ā· Video 1 Ā· Interactive Practice
Vector Fields: Sketching Constant, Radial and Rotating Fields
I Key Formulas
Key Insight: ⨠x , y ā© ā
⨠ā y , x ā© = ā x y + y x = 0 \langle x, y\rangle \cdot \langle -y, x\rangle = -xy + yx = 0 ⨠x , y ā© ā
⨠ā y , x ā© = ā x y + y x = 0 , so the rotation field is perpendicular to the radius everywhere and its arrows circle the origin; ⨠y , ā x ā© \langle y, -x\rangle ⨠y , ā x ā© is the same rotation run clockwise.
II One Vector at Every Point
At each point P P P the field gives one vector ⨠M ( P ) , N ( P ) ⩠\langle M(P), N(P)\rangle ⨠M ( P ) , N ( P )⩠, drawn with its tail at P P P , not at the origin.
Field
F = 2i + j
F = x i
F = x i + y j
F = āy i + x j
G = y i ā x j
III Uniform Rotation
In the field ā y ā ı ^ + x ā Č· ^ -y\,\hat\imath + x\,\hat\jmath ā y ī± ^ + x ī· ^ ā a particle at distance r r r moves at speed r r r , so every particle turns one radian per unit time.
IV Quiz Questions
Problem 1 Ā· Evaluate the Field at a Point
Given: F ā = ā y ā ı ^ + x ā Č· ^ \vec F = -y\,\hat\imath + x\,\hat\jmath F = ā y ī± ^ + x ī· ^ ā ā find the vector the field attaches to the point ( 2 , ā 1 ) (2, -1) ( 2 , ā 1 ) .
a ⨠2 , ā 1 ā© \langle 2, -1\rangle ⨠2 , ā 1 ā©
b ⨠ā 1 , ā 2 ā© \langle -1, -2\rangle ⨠ā 1 , ā 2 ā©
c ⨠1 , 2 ā© \langle 1, 2\rangle ⨠1 , 2 ā©
d ⨠ā 1 , 2 ā© \langle -1, 2\rangle ⨠ā 1 , 2 ā©
ā
Correct! M = ā y = 1 M = -y = 1 M = ā y = 1 and
N = x = 2 N = x = 2 N = x = 2 ; the arrow
⨠1 , 2 ⩠\langle 1, 2\rangle ⨠1 , 2 ⩠is drawn with its tail at
( 2 , ā 1 ) (2, -1) ( 2 , ā 1 ) .
ā That is the position vector. The rotation field turns
⨠x , y ⩠\langle x, y\rangle ⨠x , y ⩠by
90 ° 90\degree 90° : its components are
ā y -y ā y and
x x x .
ā Wrong direction of rotation. ⨠ā 1 , ā 2 ā© \langle -1, -2\rangle ⨠ā 1 , ā 2 ā© is
⨠y , ā x ā© \langle y, -x\rangle ⨠y , ā x ā© , the clockwise field.
ā Check the sign of M M M . With
y = ā 1 y = -1 y = ā 1 ,
M = ā y = ā ( ā 1 ) = 1 M = -y = -(-1) = 1 M = ā y = ā ( ā 1 ) = 1 .
Show solution
Substitute x = 2 x = 2 x = 2 , y = ā 1 y = -1 y = ā 1 into each component:
M = ā y = ā ( ā 1 ) = 1 , N = x = 2 , F ā ( 2 , ā 1 ) = ⨠1 , 2 ā© . M = -y = -(-1) = 1, \qquad N = x = 2, \qquad \vec F(2, -1) = \langle 1, 2\rangle. M = ā y = ā ( ā 1 ) = 1 , N = x = 2 , F ( 2 , ā 1 ) = ⨠1 , 2 ā© .
Check: ⨠2 , ā 1 ā© ā
⨠1 , 2 ā© = 2 ā 2 = 0 \langle 2, -1\rangle \cdot \langle 1, 2\rangle = 2 - 2 = 0 ⨠2 , ā 1 ā© ā
⨠1 , 2 ā© = 2 ā 2 = 0 , so the arrow is perpendicular to the radius, as it must be for the rotation field.
Problem 2 Ā· Describe the Sketch
Given: F ā = y ā ı ^ \vec F = y\,\hat\imath F = y ī± ^ ā which description matches its sketch?
a Horizontal arrows, zero on the y y y -axis, longer farther to the left or right
b Vertical arrows, pointing up above the x x x -axis and down below it
c Horizontal arrows pointing right everywhere, longer farther from the x x x -axis
d Horizontal arrows, zero on the x x x -axis, pointing right above it and left below it
ā
Correct! N = 0 N = 0 N = 0 makes every arrow horizontal, and
M = y M = y M = y sets its signed length.
ā That is the sketch of x ā ı ^ x\,\hat\imath x ī± ^ . Here the length depends on
y y y , so it is zero on the line
y = 0 y = 0 y = 0 , the
x x x -axis.
ā Not quite. The vector is
y ā ı ^ = ⨠y , 0 ā© y\,\hat\imath = \langle y, 0\rangle y ī± ^ = ⨠y , 0 ā© : the
y y y sets the length, but
ı ^ \hat\imath ī± ^ points horizontally.
ā Check the sign below the axis. For
y < 0 y < 0 y < 0 ,
⨠y , 0 ⩠\langle y, 0\rangle ⨠y , 0 ⩠has a negative first component, so it points left.
Show solution
F ā = ⨠y , 0 ā© \vec F = \langle y, 0\rangle F = ⨠y , 0 ā© . The second component is 0 0 0 , so every arrow is horizontal. On the x x x -axis y = 0 y = 0 y = 0 , giving the zero vector. At y = 1 y = 1 y = 1 the arrow is ı ^ \hat\imath ī± ^ , at y = 2 y = 2 y = 2 it is 2 ı ^ 2\hat\imath 2 ī± ^ ; at y = ā 1 y = -1 y = ā 1 it is ā ı ^ -\hat\imath ā ī± ^ , pointing left. Moving left or right changes nothing, because x x x does not appear.
Problem 3 Ā· Speed and Period in the Rotation Field
Given: fluid moves with velocity field F ā = ā y ā ı ^ + x ā Č· ^ \vec F = -y\,\hat\imath + x\,\hat\jmath F = ā y ī± ^ + x ī· ^ ā and a particle is at ( 3 , 4 ) (3, 4) ( 3 , 4 ) ā find its speed and the time it takes to go once around the origin.
What is the particle's speed?
How long does one full turn take?
a 10 Ļ 10\pi 10 Ļ
b 2 Ļ 2\pi 2 Ļ
c 2 Ļ 5 \tfrac{2\pi}{5} 5 2 Ļ ā
d Ļ \pi Ļ
ā
Correct! Speed
r = 5 r = 5 r = 5 on a circle of length
10 Ļ 10\pi 10 Ļ : one turn takes
10 Ļ / 5 = 2 Ļ 10\pi/5 = 2\pi 10 Ļ /5 = 2 Ļ , the same for every radius.
ā Check the speed. ⣠⨠ā 4 , 3 ⩠⣠= 16 + 9 |\langle -4, 3\rangle| = \sqrt{16 + 9} ⣠⨠ā 4 , 3 ⩠⣠= 16 + 9 ā ā the length of the vector, not the sum or the squared length of its components.
ā Check the period. Time is distance over speed: the circle through
( 3 , 4 ) (3,4) ( 3 , 4 ) has length
2 Ļ ā
5 2\pi \cdot 5 2 Ļ ā
5 , covered at speed
5 5 5 .
Show solution
At ( 3 , 4 ) (3, 4) ( 3 , 4 ) the field is ⨠ā 4 , 3 ā© \langle -4, 3\rangle ⨠ā 4 , 3 ā© , so the speed is
⣠F ā ⣠= ( ā 4 ) 2 + 3 2 = 5 = r . |\vec F| = \sqrt{(-4)^2 + 3^2} = 5 = r. ⣠F ⣠= ( ā 4 ) 2 + 3 2 ā = 5 = r .
The particle stays on the circle of radius r = 5 r = 5 r = 5 (the velocity is always perpendicular to the radius), whose length is 2 Ļ r = 10 Ļ 2\pi r = 10\pi 2 Ļ r = 10 Ļ . At speed 5 5 5 ,
time = 2 Ļ r r = 10 Ļ 5 = 2 Ļ . \text{time} = \frac{2\pi r}{r} = \frac{10\pi}{5} = 2\pi. time = r 2 Ļ r ā = 5 10 Ļ ā = 2 Ļ .
Problem 4 Ā· A Faster Rotation
Given: the velocity field F ā = ā 2 y ā ı ^ + 2 x ā Č· ^ \vec F = -2y\,\hat\imath + 2x\,\hat\jmath F = ā 2 y ī± ^ + 2 x ī· ^ ā ā find how long a particle takes to go once around the origin.
a 2 Ļ 2\pi 2 Ļ
b 4 Ļ 4\pi 4 Ļ
c Ļ \pi Ļ
d Ļ 2 \tfrac{\pi}{2} 2 Ļ ā
ā
Correct! The speed is
2 r 2r 2 r , so the angle grows at
2 2 2 radians per unit time and one turn takes
2 Ļ / 2 = Ļ 2\pi/2 = \pi 2 Ļ /2 = Ļ .
ā Not quite. 2 Ļ 2\pi 2 Ļ is the period of
⨠ā y , x ā© \langle -y, x\rangle ⨠ā y , x ā© ; doubling every arrow doubles the speed.
ā Wrong direction. A faster particle needs
less time: divide the circumference by the speed
2 r 2r 2 r , don't multiply.
ā Too fast. Speed
2 r 2r 2 r halves the period of
2 Ļ 2\pi 2 Ļ ; it does not quarter it.
Show solution
F ā = 2 ⨠ā y , x ā© \vec F = 2\langle -y, x\rangle F = 2 ⨠ā y , x ā© is perpendicular to the radius, so particles move on circles about the origin, with speed
⣠F ā ⣠= 2 x 2 + y 2 = 2 r . |\vec F| = 2\sqrt{x^2 + y^2} = 2r. ⣠F ⣠= 2 x 2 + y 2 ā = 2 r .
From s = r Īø s = r\theta s = r Īø , d s d t = r d Īø d t = 2 r \dfrac{ds}{dt} = r\dfrac{d\theta}{dt} = 2r d t d s ā = r d t d Īø ā = 2 r , so d Īø d t = 2 \dfrac{d\theta}{dt} = 2 d t d Īø ā = 2 for every radius. One turn is Īø = 2 Ļ \theta = 2\pi Īø = 2 Ļ , reached at t = Ļ t = \pi t = Ļ .
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