Multivariable-Calculus Ā· Unit 17 Ā· Video 1 Ā· Interactive Practice

Vector Fields: Sketching Constant, Radial and Rotating Fields

IKey Formulas

FieldNameWhat it does
Fāƒ—=M(x,y) ı^+N(x,y) ȷ^\vec F = M(x,y)\,\hat\imath + N(x,y)\,\hat\jmathVector fieldOne vector at every point, drawn with its tail at that point
Fāƒ—=2ı^+Č·^\vec F = 2\hat\imath + \hat\jmathConstant fieldThe same arrow ⟨2,1⟩\langle 2, 1\rangle everywhere
Fāƒ—=x ı^+y ȷ^\vec F = x\,\hat\imath + y\,\hat\jmathRadial fieldPoints away from the origin, ∣Fāƒ—āˆ£=x2+y2=r|\vec F| = \sqrt{x^2+y^2} = r
Fāƒ—=āˆ’y ı^+x ȷ^\vec F = -y\,\hat\imath + x\,\hat\jmathRotation fieldPosition vector turned 90°90\degree counterclockwise, ∣Fāƒ—āˆ£=r|\vec F| = r

Key Insight: ⟨x,yāŸ©ā‹…āŸØāˆ’y,x⟩=āˆ’xy+yx=0\langle x, y\rangle \cdot \langle -y, x\rangle = -xy + yx = 0, so the rotation field is perpendicular to the radius everywhere and its arrows circle the origin; ⟨y,āˆ’x⟩\langle y, -x\rangle is the same rotation run clockwise.

IIOne Vector at Every Point

At each point PP the field gives one vector ⟨M(P),N(P)⟩\langle M(P), N(P)\rangle, drawn with its tail at PP, not at the origin.

IIIUniform Rotation

In the field āˆ’y ı^+x ȷ^-y\,\hat\imath + x\,\hat\jmath a particle at distance rr moves at speed rr, so every particle turns one radian per unit time.

IVQuiz Questions

Problem 1 Ā· Evaluate the Field at a Point

Given: Fāƒ—=āˆ’y ı^+x ȷ^\vec F = -y\,\hat\imath + x\,\hat\jmath — find the vector the field attaches to the point (2,āˆ’1)(2, -1).

āœ… Correct! M=āˆ’y=1M = -y = 1 and N=x=2N = x = 2; the arrow ⟨1,2⟩\langle 1, 2\rangle is drawn with its tail at (2,āˆ’1)(2, -1).
āŒ That is the position vector. The rotation field turns ⟨x,y⟩\langle x, y\rangle by 90°90\degree: its components are āˆ’y-y and xx.
āŒ Wrong direction of rotation. āŸØāˆ’1,āˆ’2⟩\langle -1, -2\rangle is ⟨y,āˆ’x⟩\langle y, -x\rangle, the clockwise field.
āŒ Check the sign of MM. With y=āˆ’1y = -1, M=āˆ’y=āˆ’(āˆ’1)=1M = -y = -(-1) = 1.
Show solution

Substitute x=2x = 2, y=āˆ’1y = -1 into each component:

M=āˆ’y=āˆ’(āˆ’1)=1,N=x=2,Fāƒ—(2,āˆ’1)=⟨1,2⟩.M = -y = -(-1) = 1, \qquad N = x = 2, \qquad \vec F(2, -1) = \langle 1, 2\rangle.

Check: ⟨2,āˆ’1āŸ©ā‹…āŸØ1,2⟩=2āˆ’2=0\langle 2, -1\rangle \cdot \langle 1, 2\rangle = 2 - 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: Fāƒ—=y ı^\vec F = y\,\hat\imath — which description matches its sketch?

āœ… Correct! N=0N = 0 makes every arrow horizontal, and M=yM = y sets its signed length.
āŒ That is the sketch of x ı^x\,\hat\imath. Here the length depends on yy, so it is zero on the line y=0y = 0, the xx-axis.
āŒ Not quite. The vector is y ı^=⟨y,0⟩y\,\hat\imath = \langle y, 0\rangle: the yy sets the length, but ı^\hat\imath points horizontally.
āŒ Check the sign below the axis. For y<0y < 0, ⟨y,0⟩\langle y, 0\rangle has a negative first component, so it points left.
Show solution

Fāƒ—=⟨y,0⟩\vec F = \langle y, 0\rangle. The second component is 00, so every arrow is horizontal. On the xx-axis y=0y = 0, giving the zero vector. At y=1y = 1 the arrow is ı^\hat\imath, at y=2y = 2 it is 2ı^2\hat\imath; at y=āˆ’1y = -1 it is āˆ’Ä±^-\hat\imath, pointing left. Moving left or right changes nothing, because xx does not appear.

Problem 3 Ā· Speed and Period in the Rotation Field

Given: fluid moves with velocity field Fāƒ—=āˆ’y ı^+x ȷ^\vec F = -y\,\hat\imath + x\,\hat\jmath and a particle is at (3,4)(3, 4) — 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?

āœ… Correct! Speed r=5r = 5 on a circle of length 10Ļ€10\pi: one turn takes 10Ļ€/5=2Ļ€10\pi/5 = 2\pi, the same for every radius.
āŒ Check the speed. āˆ£āŸØāˆ’4,3⟩∣=16+9|\langle -4, 3\rangle| = \sqrt{16 + 9} — the length of the vector, not the sum or the squared length of its components.
āŒ Check the period. Time is distance over speed: the circle through (3,4)(3,4) has length 2π⋅52\pi \cdot 5, covered at speed 55.
Show solution

At (3,4)(3, 4) the field is āŸØāˆ’4,3⟩\langle -4, 3\rangle, so the speed is

∣Fāƒ—āˆ£=(āˆ’4)2+32=5=r.|\vec F| = \sqrt{(-4)^2 + 3^2} = 5 = r.

The particle stays on the circle of radius r=5r = 5 (the velocity is always perpendicular to the radius), whose length is 2Ļ€r=10Ļ€2\pi r = 10\pi. At speed 55,

time=2Ļ€rr=10Ļ€5=2Ļ€.\text{time} = \frac{2\pi r}{r} = \frac{10\pi}{5} = 2\pi.

Problem 4 Ā· A Faster Rotation

Given: the velocity field Fāƒ—=āˆ’2y ı^+2x ȷ^\vec F = -2y\,\hat\imath + 2x\,\hat\jmath — find how long a particle takes to go once around the origin.

āœ… Correct! The speed is 2r2r, so the angle grows at 22 radians per unit time and one turn takes 2Ļ€/2=Ļ€2\pi/2 = \pi.
āŒ Not quite. 2Ļ€2\pi is the period of āŸØāˆ’y,x⟩\langle -y, x\rangle; doubling every arrow doubles the speed.
āŒ Wrong direction. A faster particle needs less time: divide the circumference by the speed 2r2r, don't multiply.
āŒ Too fast. Speed 2r2r halves the period of 2Ļ€2\pi; it does not quarter it.
Show solution

Fāƒ—=2āŸØāˆ’y,x⟩\vec F = 2\langle -y, x\rangle is perpendicular to the radius, so particles move on circles about the origin, with speed

∣Fāƒ—āˆ£=2x2+y2=2r.|\vec F| = 2\sqrt{x^2 + y^2} = 2r.

From s=rĪøs = r\theta, dsdt=rdĪødt=2r\dfrac{ds}{dt} = r\dfrac{d\theta}{dt} = 2r, so dĪødt=2\dfrac{d\theta}{dt} = 2 for every radius. One turn is Īø=2Ļ€\theta = 2\pi, reached at t=Ļ€t = \pi.

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