Multivariable-Calculus Β· Unit 5 Β· Video 1 Β· Interactive Practice

A Line Is a Moving Point: Parametric Equations From Two Points in Space

IKey Formulas

FormulaNameWhat you need
Q0Q(t)β†’=t Q0Q1β†’\overrightarrow{Q_0Q(t)} = t\,\overrightarrow{Q_0Q_1}The one observationConstant speed, with Q(0)=Q0Q(0) = Q_0 and Q(1)=Q1Q(1) = Q_1
v=Q0Q1β†’=Q1βˆ’Q0\mathbf{v} = \overrightarrow{Q_0Q_1} = Q_1 - Q_0Velocity (direction) vectorTwo points: subtract the coordinates of Q0Q_0 from those of Q1Q_1, one component at a time
Q(t)=Q0+t vQ(t) = Q_0 + t\,\mathbf{v}Vector form of the lineOne point and one direction
x=x0+atx = x_0 + at
y=y0+bty = y_0 + bt
z=z0+ctz = z_0 + ct
Parametric equationsConstants: the position at t=0t = 0; coefficients: v=⟨a,b,c⟩\mathbf{v} = \langle a, b, c\rangle

Key Insight: A parametric line carries six numbers β€” the constants are the point at t=0t = 0, the coefficients of tt are the velocity β€” and finding a point on it means substituting one value of tt, never solving a system.

IIA Clock on the Line

At constant velocity the displacement from Q0Q_0 is exactly tt times Q0Q1β†’\overrightarrow{Q_0Q_1}, for every real tt.

IIIOne Vector Equation, Three Coordinate Formulas

Matching components turns Q0Q(t)β†’=t v\overrightarrow{Q_0Q(t)} = t\,\mathbf{v} into three formulas, each a constant plus a constant times tt.

Step 1 β€” Subtract the coordinates
v=Q0Q1β†’=⟨1βˆ’(βˆ’1),Β 3βˆ’2,Β βˆ’1βˆ’2⟩\mathbf{v} = \overrightarrow{Q_0Q_1} = \langle 1-(-1),\ 3-2,\ -1-2\rangle
v=⟨2,Β 1,Β βˆ’3⟩\mathbf{v} = \langle 2,\ 1,\ -3\rangle

IVReading the Six Numbers Backwards

The constants are the position at t=0t = 0; the coefficients of tt are the velocity along the line.

πŸ’‘ Challenge: change all six numbers and still describe the video's line.

VQuiz Questions

Problem 1 Β· Two Points, Three Formulas

Given: A=(2,βˆ’1,3)A = (2, -1, 3) and B=(5,1,2)B = (5, 1, 2) β€” find parametric equations of the line through them with Q(0)=AQ(0) = A and Q(1)=BQ(1) = B.

βœ… Correct! ABβ†’=⟨3,2,βˆ’1⟩\overrightarrow{AB} = \langle 3, 2, -1\rangle supplies the coefficients of tt and A=(2,βˆ’1,3)A = (2, -1, 3) supplies the constants.
❌ The roles are swapped. Here the constants are ⟨3,2,βˆ’1⟩\langle 3, 2, -1\rangle and the coefficients are the coordinates of AA. It does reach v+A=B\mathbf{v} + A = B at t=1t = 1, but at t=0t = 0 it sits at (3,2,βˆ’1)(3, 2, -1), not AA, and it moves along ⟨2,βˆ’1,3⟩\langle 2, -1, 3\rangle instead of ABβ†’\overrightarrow{AB}.
❌ Check the middle constant. yβˆ’(βˆ’1)=2ty - (-1) = 2t gives y=βˆ’1+2ty = -1 + 2t. With y=1+2ty = 1 + 2t the point sits at (2,1,3)β‰ A(2, 1, 3) \ne A when t=0t = 0 β€” a parallel line through neither point.
❌ That velocity is Aβˆ’BA - B. It traces the same line, but with the clock running backwards: it starts at AA and heads away from BB, reaching (βˆ’1,βˆ’3,4)(-1, -3, 4) at t=1t = 1 and passing BB only at t=βˆ’1t = -1. Subtract the coordinates of AA from those of BB.
❌ Not quite. The coefficients of tt come from Bβˆ’AB - A and the constants from AA.
Show solution

Subtract the coordinates of AA from those of BB, one component at a time:

v=ABβ†’=⟨5βˆ’2,Β 1βˆ’(βˆ’1),Β 2βˆ’3⟩=⟨3,Β 2,Β βˆ’1⟩\mathbf{v} = \overrightarrow{AB} = \langle 5-2,\ 1-(-1),\ 2-3\rangle = \langle 3,\ 2,\ -1\rangle

The arrow from AA to the moving point is tt times v\mathbf{v}:

⟨xβˆ’2,Β y+1,Β zβˆ’3⟩=⟨3t,Β 2t,Β βˆ’t⟩\langle x-2,\ y+1,\ z-3\rangle = \langle 3t,\ 2t,\ -t\rangle

Move each constant across:

x=2+3t,y=βˆ’1+2t,z=3βˆ’t\boxed{x = 2 + 3t,\quad y = -1 + 2t,\quad z = 3 - t}

Check: t=0t = 0 gives (2,βˆ’1,3)=A(2, -1, 3) = A, and t=1t = 1 gives (2+3,Β βˆ’1+2,Β 3βˆ’1)=(5,1,2)=BΒ βœ“(2+3,\ -1+2,\ 3-1) = (5, 1, 2) = B\ \checkmark

Problem 2 Β· Which Point Is on the Line?

Given: the video's line x=βˆ’1+2tx = -1 + 2t, y=2+ty = 2 + t, z=2βˆ’3tz = 2 - 3t β€” which of these points lies on it?

βœ… Correct! All three coordinates give the same time: βˆ’1+2t=βˆ’3-1 + 2t = -3, 2+t=12 + t = 1 and 2βˆ’3t=52 - 3t = 5 each give t=βˆ’1t = -1, one unit of time before the point reaches Q0Q_0.
❌ That is the velocity, not a position. Treated as a point, x=2x = 2 needs t=32t = \tfrac{3}{2} while y=1y = 1 needs t=βˆ’1t = -1.
❌ Two coordinates out of three is not enough. xx and yy both give t=2t = 2, but at t=2t = 2 the third coordinate is 2βˆ’6=βˆ’42 - 6 = -4, not βˆ’3-3.
❌ That point is on the parallel line y=ty = t β€” the video's line with its constant 22 dropped, at t=1t = 1. On the actual line x=1x = 1 needs t=1t = 1 but y=1y = 1 needs t=βˆ’1t = -1.
❌ Not quite. Solve each coordinate equation for tt; the point is on the line only if all three give the same tt.
Show solution

A point is on the line exactly when one value of tt produces all three of its coordinates. Solve each coordinate equation for tt:

  • (2,1,βˆ’3)(2, 1, -3): xx gives t=32t = \tfrac{3}{2}, yy gives t=βˆ’1t = -1 β€” no.
  • (3,4,βˆ’3)(3, 4, -3): xx gives t=2t = 2, yy gives t=2t = 2, zz gives 2βˆ’3t=βˆ’32 - 3t = -3, so t=53t = \tfrac{5}{3} β€” no.
  • (1,1,βˆ’1)(1, 1, -1): xx gives t=1t = 1, yy gives t=βˆ’1t = -1 β€” no.
  • (βˆ’3,1,5)(-3, 1, 5): xx gives t=βˆ’1t = -1, yy gives t=βˆ’1t = -1, zz gives 2βˆ’3t=52 - 3t = 5, so t=βˆ’1t = -1 β€” yes.
Q(βˆ’1)=(βˆ’1βˆ’2,Β 2βˆ’1,Β 2+3)=(βˆ’3,Β 1,Β 5)=Q0βˆ’vQ(-1) = (-1 - 2,\ 2 - 1,\ 2 + 3) = (-3,\ 1,\ 5) = Q_0 - \mathbf{v}

Problem 3 Β· A Different Clock

Given: a point moves along a line at constant velocity; at t=0t = 0 it is at A=(2,βˆ’1,0)A = (2, -1, 0) and at t=3t = 3 it is at B=(8,5,βˆ’6)B = (8, 5, -6) β€” find its velocity and its position at t=1t = 1.

What is the velocity vector?

Where is the point one unit of time after leaving A?

βœ… Correct! The displacement ABβ†’=⟨6,6,βˆ’6⟩\overrightarrow{AB} = \langle 6, 6, -6\rangle takes 33 units of time, so v=⟨2,2,βˆ’2⟩\mathbf{v} = \langle 2, 2, -2\rangle and Q(1)=A+v=(4,1,βˆ’2)Q(1) = A + \mathbf{v} = (4, 1, -2).
❌ That is the whole displacement ABβ†’\overrightarrow{AB}. It is covered in 33 units of time, not one, so the velocity is a third of it.
❌ Only the coordinates of BB were divided by 33. The velocity is the displacement Bβˆ’AB - A divided by the elapsed time 33.
❌ That adds the coordinates of AA and BB. The displacement is the difference Bβˆ’A=⟨6,6,βˆ’6⟩B - A = \langle 6, 6, -6\rangle.
❌ Check the velocity. Velocity == displacement Γ·\div elapsed time =(Bβˆ’A)/3= (B - A) / 3.
❌ That is BB, where the point is at t=3t = 3. Arriving at the second point at t=1t = 1 was the clock chosen in the video; this clock reaches BB at t=3t = 3.
❌ That is the midpoint of ABAB. At constant velocity the point is halfway at t=32t = \tfrac{3}{2}, not at t=1t = 1.
❌ That is the velocity, not a position. The moving point starts from AA: Q(1)=A+vQ(1) = A + \mathbf{v}.
❌ Check the position. Start at AA and add one velocity: Q(1)=A+vQ(1) = A + \mathbf{v}.
Show solution

The displacement from AA to BB:

ABβ†’=⟨8βˆ’2,Β 5βˆ’(βˆ’1),Β βˆ’6βˆ’0⟩=⟨6,Β 6,Β βˆ’6⟩\overrightarrow{AB} = \langle 8-2,\ 5-(-1),\ -6-0\rangle = \langle 6,\ 6,\ -6\rangle

It is covered between t=0t = 0 and t=3t = 3, so each unit of time covers a third of it:

v=13⟨6,Β 6,Β βˆ’6⟩=⟨2,Β 2,Β βˆ’2⟩\mathbf{v} = \tfrac{1}{3}\langle 6,\ 6,\ -6\rangle = \langle 2,\ 2,\ -2\rangle

With AA as the constants and v\mathbf{v} as the coefficients (the zz-constant is 00 because AA lies in the xyxy-plane):

x=2+2t,y=βˆ’1+2t,z=βˆ’2tx = 2 + 2t,\quad y = -1 + 2t,\quad z = -2t Q(1)=(2+2,Β βˆ’1+2,Β βˆ’2)=(4,Β 1,Β βˆ’2)Q(1) = (2 + 2,\ -1 + 2,\ -2) = (4,\ 1,\ -2)

Check: Q(3)=(2+6,Β βˆ’1+6,Β βˆ’6)=(8,5,βˆ’6)=BΒ βœ“Q(3) = (2 + 6,\ -1 + 6,\ -6) = (8, 5, -6) = B\ \checkmark

Problem 4 Β· Same Line, Different Numbers

Given: the video's line x=βˆ’1+2tx = -1 + 2t, y=2+ty = 2 + t, z=2βˆ’3tz = 2 - 3t β€” which of these describes the same line?

βœ… Correct! Its constants (1,3,βˆ’1)(1, 3, -1) are Q1Q_1, a point of the line, and its coefficients ⟨4,2,βˆ’6⟩=2v\langle 4, 2, -6\rangle = 2\mathbf{v} point along it: the same line, travelled twice as fast with the clock started at Q1Q_1.
❌ The constant of yy is missing. The direction is right, but at t=0t = 0 this line is at (βˆ’1,0,2)(-1, 0, 2) β€” two units from Q0Q_0 in the βˆ’y-y direction, on a parallel line through neither Q0Q_0 nor Q1Q_1.
❌ Constants and coefficients have traded places. This line starts at (2,1,βˆ’3)(2, 1, -3) and moves along βŸ¨βˆ’1,2,2⟩\langle -1, 2, 2\rangle, which is not a multiple of ⟨2,1,βˆ’3⟩\langle 2, 1, -3\rangle.
❌ One coefficient changed sign. It starts at Q0Q_0 but moves along ⟨2,1,3⟩\langle 2, 1, 3\rangle, not a multiple of ⟨2,1,βˆ’3⟩\langle 2, 1, -3\rangle, so the two lines meet at Q0Q_0 and nowhere else.
❌ Not quite. Same line means a parallel velocity AND a starting point that lies on the video's line.
Show solution

Read each candidate backwards: the constants are its point at t=0t = 0, the coefficients its velocity. It is the video's line exactly when (1) the velocity is a multiple of v=⟨2,1,βˆ’3⟩\mathbf{v} = \langle 2, 1, -3\rangle and (2) the starting point lies on the video's line.

  • (a) velocity ⟨2,1,βˆ’3⟩\langle 2, 1, -3\rangle βœ“\checkmark, but (βˆ’1,0,2)(-1, 0, 2): xx gives t=0t = 0, yy gives t=βˆ’2t = -2 β€” not on the line. Parallel, different.
  • (b) velocity ⟨4,2,βˆ’6⟩=2⟨2,1,βˆ’3⟩\langle 4, 2, -6\rangle = 2\langle 2, 1, -3\rangle βœ“\checkmark, and (1,3,βˆ’1)(1, 3, -1) gives t=1t = 1 in all three coordinates β€” it is Q1Q_1. Same line.
  • (c) velocity βŸ¨βˆ’1,2,2⟩\langle -1, 2, 2\rangle β€” not a multiple of ⟨2,1,βˆ’3⟩\langle 2, 1, -3\rangle.
  • (d) velocity ⟨2,1,3⟩\langle 2, 1, 3\rangle β€” not a multiple of ⟨2,1,βˆ’3⟩\langle 2, 1, -3\rangle.

For (b), the point it reaches at time ss is the video's point at time t=1+2st = 1 + 2s:

(βˆ’1+2(1+2s),Β 2+(1+2s),Β 2βˆ’3(1+2s))=(1+4s,Β 3+2s,Β βˆ’1βˆ’6s)\big(-1 + 2(1+2s),\ 2 + (1+2s),\ 2 - 3(1+2s)\big) = (1 + 4s,\ 3 + 2s,\ -1 - 6s)

Solved: 0 / 4