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MATH-283 (Calculus III) Curriculum

Session 04 - Lines and Planes in Space

Handout Worksheet
Fall Semester 2026
Session Objectives & Overview

By the end of this session, you will be able to:

  • Review core multivariable mathematical concepts and engineering calculus prerequisites.

Micro-Lecture

Engineering Context: Designing in 3D

In this session, we investigate the mathematical principles of Lines and Planes in Space and explore how engineers apply these concepts to analyze real-world physical and structural systems.

Skill Block 1

Worked Example

Given a line with the points P=(βˆ’4,βˆ’6,βˆ’2)P=(-4,-6,-2)P=(βˆ’4,βˆ’6,βˆ’2) and Q=(10,2,1)Q=(10,2,1)Q=(10,2,1):

  • Find the vector equation of the line. Evaluate at a few values of ttt.
  • Find the parametric equation of the line.
  • Convert the parametric equation into a symmetric equation.
Worked Solution:

Here is the step-by-step solution to the problem presented in the image.

Given Data
  • Point PPP: (βˆ’4,βˆ’6,βˆ’2)(-4, -6, -2)(βˆ’4,βˆ’6,βˆ’2)

  • Point QQQ: (10,2,1)(10, 2, 1)(10,2,1)

1. Vector Equation of the Line

To find the vector equation, we first need a position vector rβƒ—0\vec{r}_0r0​ for a point on the line and a direction vector vβƒ—\vec{v}v that is parallel to the line.

  1. Find the direction vector v⃗\vec{v}v by finding the vector from PPP to QQQ:

vβƒ—=PQβƒ—=⟨10βˆ’(βˆ’4),2βˆ’(βˆ’6),1βˆ’(βˆ’2)⟩\vec{v} = \vec{PQ} = \langle 10 - (-4), 2 - (-6), 1 - (-2) \ranglev=PQ​=⟨10βˆ’(βˆ’4),2βˆ’(βˆ’6),1βˆ’(βˆ’2)⟩

vβƒ—=⟨14,8,3⟩\vec{v} = \langle 14, 8, 3 \ranglev=⟨14,8,3⟩

  1. Use point PPP as the initial position vector rβƒ—0\vec{r}_0r0​:

rβƒ—0=βŸ¨βˆ’4,βˆ’6,βˆ’2⟩\vec{r}_0 = \langle -4, -6, -2 \rangler0​=βŸ¨βˆ’4,βˆ’6,βˆ’2⟩

  1. Write the vector equation rβƒ—(t)=rβƒ—0+tvβƒ—\vec{r}(t) = \vec{r}_0 + t\vec{v}r(t)=r0​+tv:

rβƒ—(t)=βŸ¨βˆ’4,βˆ’6,βˆ’2⟩+t⟨14,8,3⟩\vec{r}(t) = \langle -4, -6, -2 \rangle + t\langle 14, 8, 3 \rangler(t)=βŸ¨βˆ’4,βˆ’6,βˆ’2⟩+t⟨14,8,3⟩

Evaluating at a few values of ttt:

  • For t=0t = 0t=0:

rβƒ—(0)=βŸ¨βˆ’4,βˆ’6,βˆ’2⟩(ThisΒ isΒ pointΒ P)\vec{r}(0) = \langle -4, -6, -2 \rangle \quad (\text{This is point } P)r(0)=βŸ¨βˆ’4,βˆ’6,βˆ’2⟩(ThisΒ isΒ pointΒ P)

  • For t=1t = 1t=1:

rβƒ—(1)=βŸ¨βˆ’4+14,βˆ’6+8,βˆ’2+3⟩=⟨10,2,1⟩(ThisΒ isΒ pointΒ Q)\vec{r}(1) = \langle -4+14, -6+8, -2+3 \rangle = \langle 10, 2, 1 \rangle \quad (\text{This is point } Q)r(1)=βŸ¨βˆ’4+14,βˆ’6+8,βˆ’2+3⟩=⟨10,2,1⟩(ThisΒ isΒ pointΒ Q)

  • For t=βˆ’1t = -1t=βˆ’1:

rβƒ—(βˆ’1)=βŸ¨βˆ’4βˆ’14,βˆ’6βˆ’8,βˆ’2βˆ’3⟩=βŸ¨βˆ’18,βˆ’14,βˆ’5⟩\vec{r}(-1) = \langle -4-14, -6-8, -2-3 \rangle = \langle -18, -14, -5 \rangler(βˆ’1)=βŸ¨βˆ’4βˆ’14,βˆ’6βˆ’8,βˆ’2βˆ’3⟩=βŸ¨βˆ’18,βˆ’14,βˆ’5⟩

2. Parametric Equations of the Line

The parametric equations break the vector equation down into separate components for xxx, yyy, and zzz using the format:

  • x=x0+atx = x_0 + atx=x0​+at

  • y=y0+bty = y_0 + bty=y0​+bt

  • z=z0+ctz = z_0 + ctz=z0​+ct

Substituting our point P(βˆ’4,βˆ’6,βˆ’2)P(-4, -6, -2)P(βˆ’4,βˆ’6,βˆ’2) and direction vector components ⟨14,8,3⟩\langle 14, 8, 3 \rangle⟨14,8,3⟩:

  • x=βˆ’4+14tx = -4 + 14tx=βˆ’4+14t

  • y=βˆ’6+8ty = -6 + 8ty=βˆ’6+8t

  • z=βˆ’2+3tz = -2 + 3tz=βˆ’2+3t

3. Symmetric Equation of the Line

To convert the parametric equations into a symmetric equation, we solve each individual equation for ttt and set them equal to each other:

  1. Solve for ttt in the xxx equation:

x=βˆ’4+14tβ€…β€ŠβŸΉβ€…β€Šx+4=14tβ€…β€ŠβŸΉβ€…β€Št=x+414x = -4 + 14t \implies x + 4 = 14t \implies t = \frac{x + 4}{14}x=βˆ’4+14t⟹x+4=14t⟹t=14x+4​

  1. Solve for ttt in the yyy equation:

y=βˆ’6+8tβ€…β€ŠβŸΉβ€…β€Šy+6=8tβ€…β€ŠβŸΉβ€…β€Št=y+68y = -6 + 8t \implies y + 6 = 8t \implies t = \frac{y + 6}{8}y=βˆ’6+8t⟹y+6=8t⟹t=8y+6​

  1. Solve for ttt in the zzz equation:

z=βˆ’2+3tβ€…β€ŠβŸΉβ€…β€Šz+2=3tβ€…β€ŠβŸΉβ€…β€Št=z+23z = -2 + 3t \implies z + 2 = 3t \implies t = \frac{z + 2}{3}z=βˆ’2+3t⟹z+2=3t⟹t=3z+2​

Equating all three expressions for ttt gives the symmetric equation:

x+414=y+68=z+23\frac{x + 4}{14} = \frac{y + 6}{8} = \frac{z + 2}{3}14x+4​=8y+6​=3z+2​

Active Practice Problem

Given a line with the points A=(1,4,βˆ’2)A=(1,4,-2)A=(1,4,βˆ’2) and B=(βˆ’3,5,0)B=(-3,5,0)B=(βˆ’3,5,0):

  • Find the vector equation of the line. Evaluate at a few values of ttt.
  • Find the Parametric equation of the line.
  • Convert the parametric equation into a symmetric equation.
Solution Key:

Here is the complete solution for Problem S1.1 from the activity:

Given Data
  • Point AAA: (1,4,βˆ’2)(1, 4, -2)(1,4,βˆ’2)

  • Point BBB: (βˆ’3,5,0)(-3, 5, 0)(βˆ’3,5,0)

1. Vector Equation of the Line

To construct the vector equation, we need an initial position vector rβƒ—0\vec{r}_0r0​ and a direction vector vβƒ—\vec{v}v.

  1. Find the direction vector v⃗\vec{v}v by finding the displacement vector from AAA to BBB:

vβƒ—=ABβƒ—=βŸ¨βˆ’3βˆ’1,Β 5βˆ’4,Β 0βˆ’(βˆ’2)⟩\vec{v} = \vec{AB} = \langle -3 - 1, \ 5 - 4, \ 0 - (-2) \ranglev=AB=βŸ¨βˆ’3βˆ’1,Β 5βˆ’4,Β 0βˆ’(βˆ’2)⟩

vβƒ—=βŸ¨βˆ’4,1,2⟩\vec{v} = \langle -4, 1, 2 \ranglev=βŸ¨βˆ’4,1,2⟩

  1. Set point AAA as your initial position vector rβƒ—0\vec{r}_0r0​:

rβƒ—0=⟨1,4,βˆ’2⟩\vec{r}_0 = \langle 1, 4, -2 \rangler0​=⟨1,4,βˆ’2⟩

  1. Assemble the vector equation rβƒ—(t)=rβƒ—0+tvβƒ—\vec{r}(t) = \vec{r}_0 + t\vec{v}r(t)=r0​+tv:

rβƒ—(t)=⟨1,4,βˆ’2⟩+tβŸ¨βˆ’4,1,2⟩\vec{r}(t) = \langle 1, 4, -2 \rangle + t\langle -4, 1, 2 \rangler(t)=⟨1,4,βˆ’2⟩+tβŸ¨βˆ’4,1,2⟩

Evaluating at a few values of ttt:

  • For t=0t = 0t=0:

rβƒ—(0)=⟨1,4,βˆ’2⟩(PointΒ A)\vec{r}(0) = \langle 1, 4, -2 \rangle \quad (\text{Point } A)r(0)=⟨1,4,βˆ’2⟩(PointΒ A)

  • For t=1t = 1t=1:

rβƒ—(1)=⟨1βˆ’4,Β 4+1,Β βˆ’2+2⟩=βŸ¨βˆ’3,5,0⟩(PointΒ B)\vec{r}(1) = \langle 1 - 4, \ 4 + 1, \ -2 + 2 \rangle = \langle -3, 5, 0 \rangle \quad (\text{Point } B)r(1)=⟨1βˆ’4,Β 4+1,Β βˆ’2+2⟩=βŸ¨βˆ’3,5,0⟩(PointΒ B)

  • For t=2t = 2t=2:

rβƒ—(2)=⟨1βˆ’8,Β 4+2,Β βˆ’2+4⟩=βŸ¨βˆ’7,6,2⟩\vec{r}(2) = \langle 1 - 8, \ 4 + 2, \ -2 + 4 \rangle = \langle -7, 6, 2 \rangler(2)=⟨1βˆ’8,Β 4+2,Β βˆ’2+4⟩=βŸ¨βˆ’7,6,2⟩

2. Parametric Equations of the Line

By breaking the vector equation down into its distinct scalar components (xxx, yyy, and zzz) using the format x=x0+atx = x_0 + atx=x0​+at, y=y0+bty = y_0 + bty=y0​+bt, and z=z0+ctz = z_0 + ctz=z0​+ct, we get:

  • x=1βˆ’4tx = 1 - 4tx=1βˆ’4t

  • y=4+ty = 4 + ty=4+t

  • z=βˆ’2+2tz = -2 + 2tz=βˆ’2+2t

3. Symmetric Equation of the Line

To find the symmetric equation, we isolate ttt in each parametric component and set them equal to one another:

  1. Solve for ttt in xxx:

x=1βˆ’4tβ€…β€ŠβŸΉβ€…β€Šxβˆ’1=βˆ’4tβ€…β€ŠβŸΉβ€…β€Št=xβˆ’1βˆ’4x = 1 - 4t \implies x - 1 = -4t \implies t = \frac{x - 1}{-4}x=1βˆ’4t⟹xβˆ’1=βˆ’4t⟹t=βˆ’4xβˆ’1​

  1. Solve for ttt in yyy:

y=4+tβ€…β€ŠβŸΉβ€…β€Št=yβˆ’41y = 4 + t \implies t = \frac{y - 4}{1}y=4+t⟹t=1yβˆ’4​

  1. Solve for ttt in zzz:

z=βˆ’2+2tβ€…β€ŠβŸΉβ€…β€Šz+2=2tβ€…β€ŠβŸΉβ€…β€Št=z+22z = -2 + 2t \implies z + 2 = 2t \implies t = \frac{z + 2}{2}z=βˆ’2+2t⟹z+2=2t⟹t=2z+2​

Equating these gives the symmetric equation:

xβˆ’1βˆ’4=yβˆ’4=z+22\frac{x - 1}{-4} = y - 4 = \frac{z + 2}{2}βˆ’4xβˆ’1​=yβˆ’4=2z+2​

Show your steps and calculations here.

Regroup 1

  • Review common misconceptions and clarify key notations.

Skill Block 2

Worked Example

Find the distance between the point M=(1,1,3)M=(1,1,3)M=(1,1,3) and the line:

xβˆ’34=y+12=zβˆ’3\frac{x-3}{4}=\frac{y+1}{2}=z-34xβˆ’3​=2y+1​=zβˆ’3

Worked Solution:

Here is the step-by-step solution for Skill 2 Demo using the distance formula provided in the activity.

Given Data
  • Point MMM (anywhere in space): (1,1,3)(1, 1, 3)(1,1,3)

  • Symmetric equation of the line: xβˆ’34=y+12=zβˆ’3\frac{x-3}{4} = \frac{y+1}{2} = z-34xβˆ’3​=2y+1​=zβˆ’3

1. Extract Information from the Line

From the symmetric equation form xβˆ’x0a=yβˆ’y0b=zβˆ’z0c\frac{x-x_0}{a} = \frac{y-y_0}{b} = \frac{z-z_0}{c}axβˆ’x0​​=byβˆ’y0​​=czβˆ’z0​​, we can extract:

  1. A point PPP on the line: (3,βˆ’1,3)(3, -1, 3)(3,βˆ’1,3)

  2. The direction vector vβƒ—\vec{v}v along the line: ⟨4,2,1⟩\langle 4, 2, 1 \rangle⟨4,2,1⟩ (note that zβˆ’3z-3zβˆ’3 is equivalent to zβˆ’31\frac{z-3}{1}1zβˆ’3​)

2. Find the Vector PM⃗\vec{PM}PM

Now, find the vector pointing from the line point PPP to the external point MMM:

PMβƒ—=⟨xMβˆ’xP,Β yMβˆ’yP,Β zMβˆ’zP⟩\vec{PM} = \langle x_M - x_P, \ y_M - y_P, \ z_M - z_P \ranglePM=⟨xMβ€‹βˆ’xP​,Β yMβ€‹βˆ’yP​,Β zMβ€‹βˆ’zPβ€‹βŸ©

PMβƒ—=⟨1βˆ’3,Β 1βˆ’(βˆ’1),Β 3βˆ’3⟩=βŸ¨βˆ’2,2,0⟩\vec{PM} = \langle 1 - 3, \ 1 - (-1), \ 3 - 3 \rangle = \langle -2, 2, 0 \ranglePM=⟨1βˆ’3,Β 1βˆ’(βˆ’1),Β 3βˆ’3⟩=βŸ¨βˆ’2,2,0⟩

3. Compute the Cross Product PM⃗×v⃗\vec{PM} \times \vec{v}PM×v

The formula requires the cross product of PM⃗\vec{PM}PM and the direction vector v⃗\vec{v}v:

PMβƒ—Γ—vβƒ—=∣i^j^k^βˆ’220421∣\vec{PM} \times \vec{v} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ -2 & 2 & 0 \\ 4 & 2 & 1 \end{vmatrix}PMΓ—v=​i^βˆ’24​j^​22​k^01​​

Expand the determinant by the top row:

PMβƒ—Γ—vβƒ—=i^(2(1)βˆ’0(2))βˆ’j^((βˆ’2)(1)βˆ’0(4))+k^((βˆ’2)(2)βˆ’2(4))\vec{PM} \times \vec{v} = \hat{i}(2(1) - 0(2)) - \hat{j}((-2)(1) - 0(4)) + \hat{k}((-2)(2) - 2(4))PMΓ—v=i^(2(1)βˆ’0(2))βˆ’j^​((βˆ’2)(1)βˆ’0(4))+k^((βˆ’2)(2)βˆ’2(4))

PMβƒ—Γ—vβƒ—=i^(2)βˆ’j^(βˆ’2)+k^(βˆ’4βˆ’8)\vec{PM} \times \vec{v} = \hat{i}(2) - \hat{j}(-2) + \hat{k}(-4 - 8)PMΓ—v=i^(2)βˆ’j^​(βˆ’2)+k^(βˆ’4βˆ’8)

PMβƒ—Γ—vβƒ—=⟨2,2,βˆ’12⟩\vec{PM} \times \vec{v} = \langle 2, 2, -12 \ranglePMΓ—v=⟨2,2,βˆ’12⟩

4. Calculate the Magnitudes

Now find the magnitudes (lengths) of both the cross product vector and the direction vector v⃗\vec{v}v:

  • Magnitude of PMβƒ—Γ—vβƒ—\vec{PM} \times \vec{v}PMΓ—v:

∣∣PMβƒ—Γ—vβƒ—βˆ£βˆ£=22+22+(βˆ’12)2=4+4+144=152||\vec{PM} \times \vec{v}|| = \sqrt{2^2 + 2^2 + (-12)^2} = \sqrt{4 + 4 + 144} = \sqrt{152}∣∣PMΓ—v∣∣=22+22+(βˆ’12)2​=4+4+144​=152​

152=4Γ—38=238\sqrt{152} = \sqrt{4 \times 38} = 2\sqrt{38}152​=4Γ—38​=238​

  • Magnitude of vβƒ—\vec{v}v:

∣∣vβƒ—βˆ£βˆ£=42+22+12=16+4+1=21||\vec{v}|| = \sqrt{4^2 + 2^2 + 1^2} = \sqrt{16 + 4 + 1} = \sqrt{21}∣∣v∣∣=42+22+12​=16+4+1​=21​

5. Calculate the Distance ddd

Substitute these magnitudes into the distance formula d=∣∣PMβƒ—Γ—vβƒ—βˆ£βˆ£βˆ£βˆ£vβƒ—βˆ£βˆ£d = \frac{||\vec{PM} \times \vec{v}||}{||\vec{v}||}d=∣∣v∣∣∣∣PMΓ—vβˆ£βˆ£β€‹:

d=23821d = \frac{2\sqrt{38}}{\sqrt{21}}d=21​238​​

To write it under a single radical or rationalize it:

d=23821=279821β‰ˆ2.69d = 2\sqrt{\frac{38}{21}} = \frac{2\sqrt{798}}{21} \approx 2.69d=22138​​=212798β€‹β€‹β‰ˆ2.69

The exact distance between the point and the line is 279821\frac{2\sqrt{798}}{21}212798​​ (or approximately 2.692.692.69 units).

Active Practice Problem

Find the distance between the point (0,3,6)(0, 3, 6)(0,3,6) and the line with parametric equations:

x=1βˆ’t,y=1+2t,z=5+3tx=1-t, \quad y=1+2t, \quad z=5+3tx=1βˆ’t,y=1+2t,z=5+3t

Solution Key:
Given Data
  • Point MMM (external point): (0,3,6)(0, 3, 6)(0,3,6)

  • Parametric equations of the line: x=1βˆ’tx = 1 - tx=1βˆ’t, y=1+2ty = 1 + 2ty=1+2t, z=5+3tz = 5 + 3tz=5+3t

1. Extract Information from the Line

From the parametric equations form x=x0+atx = x_0 + atx=x0​+at, y=y0+bty = y_0 + bty=y0​+bt, and z=z0+ctz = z_0 + ctz=z0​+ct , we can easily read off a point on the line and its direction vector:

  1. A point PPP on the line (by looking at the constant terms where t=0t = 0t=0):

P=(1,1,5)P = (1, 1, 5)P=(1,1,5)

  1. The direction vector v⃗\vec{v}v along the line (the coefficients of ttt):

vβƒ—=βŸ¨βˆ’1,2,3⟩\vec{v} = \langle -1, 2, 3 \ranglev=βŸ¨βˆ’1,2,3⟩

2. Find the Vector PM⃗\vec{PM}PM

Now, find the vector pointing from the line's point PPP to the external point MMM:

PMβƒ—=⟨xMβˆ’xP,Β yMβˆ’yP,Β zMβˆ’zP⟩\vec{PM} = \langle x_M - x_P, \ y_M - y_P, \ z_M - z_P \ranglePM=⟨xMβ€‹βˆ’xP​,Β yMβ€‹βˆ’yP​,Β zMβ€‹βˆ’zPβ€‹βŸ©

PMβƒ—=⟨0βˆ’1,Β 3βˆ’1,Β 6βˆ’5⟩=βŸ¨βˆ’1,2,1⟩\vec{PM} = \langle 0 - 1, \ 3 - 1, \ 6 - 5 \rangle = \langle -1, 2, 1 \ranglePM=⟨0βˆ’1,Β 3βˆ’1,Β 6βˆ’5⟩=βŸ¨βˆ’1,2,1⟩

3. Compute the Cross Product PM⃗×v⃗\vec{PM} \times \vec{v}PM×v

Next, find the cross product required by the formula:

PMβƒ—Γ—vβƒ—=∣i^j^k^βˆ’121βˆ’123∣\vec{PM} \times \vec{v} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ -1 & 2 & 1 \\ -1 & 2 & 3 \end{vmatrix}PMΓ—v=​i^βˆ’1βˆ’1​j^​22​k^13​​

Expand the determinant along the top row:

PMβƒ—Γ—vβƒ—=i^(2(3)βˆ’1(2))βˆ’j^((βˆ’1)(3)βˆ’1(βˆ’1))+k^((βˆ’1)(2)βˆ’2(βˆ’1))\vec{PM} \times \vec{v} = \hat{i}(2(3) - 1(2)) - \hat{j}((-1)(3) - 1(-1)) + \hat{k}((-1)(2) - 2(-1))PMΓ—v=i^(2(3)βˆ’1(2))βˆ’j^​((βˆ’1)(3)βˆ’1(βˆ’1))+k^((βˆ’1)(2)βˆ’2(βˆ’1))

PMβƒ—Γ—vβƒ—=i^(6βˆ’2)βˆ’j^(βˆ’3+1)+k^(βˆ’2+2)\vec{PM} \times \vec{v} = \hat{i}(6 - 2) - \hat{j}(-3 + 1) + \hat{k}(-2 + 2)PMΓ—v=i^(6βˆ’2)βˆ’j^​(βˆ’3+1)+k^(βˆ’2+2)

PMβƒ—Γ—vβƒ—=i^(4)βˆ’j^(βˆ’2)+k^(0)\vec{PM} \times \vec{v} = \hat{i}(4) - \hat{j}(-2) + \hat{k}(0)PMΓ—v=i^(4)βˆ’j^​(βˆ’2)+k^(0)

PMβƒ—Γ—vβƒ—=⟨4,2,0⟩\vec{PM} \times \vec{v} = \langle 4, 2, 0 \ranglePMΓ—v=⟨4,2,0⟩

4. Calculate the Magnitudes

Now compute the magnitudes (lengths) of our cross product vector and the line's direction vector v⃗\vec{v}v:

  • Magnitude of PMβƒ—Γ—vβƒ—\vec{PM} \times \vec{v}PMΓ—v:

∣∣PMβƒ—Γ—vβƒ—βˆ£βˆ£=42+22+02=16+4+0=20=25||\vec{PM} \times \vec{v}|| = \sqrt{4^2 + 2^2 + 0^2} = \sqrt{16 + 4 + 0} = \sqrt{20} = 2\sqrt{5}∣∣PMΓ—v∣∣=42+22+02​=16+4+0​=20​=25​

  • Magnitude of vβƒ—\vec{v}v:

∣∣vβƒ—βˆ£βˆ£=(βˆ’1)2+22+32=1+4+9=14||\vec{v}|| = \sqrt{(-1)^2 + 2^2 + 3^2} = \sqrt{1 + 4 + 9} = \sqrt{14}∣∣v∣∣=(βˆ’1)2+22+32​=1+4+9​=14​

5. Calculate the Distance ddd

Substitute these values into the distance formula d=∣∣PMβƒ—Γ—vβƒ—βˆ£βˆ£βˆ£βˆ£vβƒ—βˆ£βˆ£d = \frac{||\vec{PM} \times \vec{v}||}{||\vec{v}||}d=∣∣v∣∣∣∣PMΓ—vβˆ£βˆ£β€‹:

d=2014=2014=107d = \frac{\sqrt{20}}{\sqrt{14}} = \sqrt{\frac{20}{14}} = \sqrt{\frac{10}{7}}d=14​20​​=1420​​=710​​

To rationalize the denominator:

d=107β‹…77=707β‰ˆ1.20d = \frac{\sqrt{10}}{\sqrt{7}} \cdot \frac{\sqrt{7}}{\sqrt{7}} = \frac{\sqrt{70}}{7} \approx 1.20d=7​10​​⋅7​7​​=770β€‹β€‹β‰ˆ1.20

The exact distance between the point and the line is 707\frac{\sqrt{70}}{7}770​​ (or approximately 1.201.201.20 units).

Show your steps and calculations here.

Regroup 2

  • Reflect on the physical modeling applications and mathematical setups.

Skill Block 3

Worked Example

Determine whether the lines L1L_{1}L1​ and L2L_{2}L2​ are equal, parallel but not skew, skew, or intersecting.

L1:x=5t,y=βˆ’13βˆ’6t,z=19βˆ’tL_{1}:x=5t, \quad y=-13-6t, \quad z=19-tL1​:x=5t,y=βˆ’13βˆ’6t,z=19βˆ’t
L2:x=βˆ’1βˆ’6s,y=βˆ’12βˆ’12s,z=19βˆ’18sL_{2}:x=-1-6s, \quad y=-12-12s, \quad z=19-18sL2​:x=βˆ’1βˆ’6s,y=βˆ’12βˆ’12s,z=19βˆ’18s

  • Equal
  • Parallel
  • Skew
  • Intersecting
Worked Solution:
Given Data
  • Line 1 (L1L_1L1​): x=5t,y=βˆ’13βˆ’6t,z=19βˆ’tx = 5t, \quad y = -13 - 6t, \quad z = 19 - tx=5t,y=βˆ’13βˆ’6t,z=19βˆ’t

  • Line 2 (L2L_2L2​): x=βˆ’1βˆ’6s,y=βˆ’12βˆ’12s,z=19βˆ’18sx = -1 - 6s, \quad y = -12 - 12s, \quad z = 19 - 18sx=βˆ’1βˆ’6s,y=βˆ’12βˆ’12s,z=19βˆ’18s

Step 1: Extract and Compare Direction Vectors

First, we extract the direction vectors (u⃗\vec{u}u and v⃗\vec{v}v) from the coefficients of the parameters ttt and sss:

  • Direction vector of L1L_1L1​ (uβƒ—\vec{u}u): ⟨5,βˆ’6,βˆ’1⟩\langle 5, -6, -1 \rangle⟨5,βˆ’6,βˆ’1⟩

  • Direction vector of L2L_2L2​ (vβƒ—\vec{v}v): βŸ¨βˆ’6,βˆ’12,βˆ’18⟩\langle -6, -12, -18 \rangleβŸ¨βˆ’6,βˆ’12,βˆ’18⟩

To check if the lines are parallel, we see if one vector is a scalar multiple of the other (u⃗=av⃗\vec{u} = a\vec{v}u=av):

βˆ’65β‰ βˆ’12βˆ’6\frac{-6}{5} \neq \frac{-12}{-6}5βˆ’6​=βˆ’6βˆ’12​

Because the components do not scale proportionally, the direction vectors are not parallel. Looking at our relationship table, this leaves two possibilities: Intersecting or Skew.

Step 2: Check for an Intersection Point

To find out if they share a common point, we set the corresponding coordinate components equal to each other (x1=x2x_1 = x_2x1​=x2​, y1=y2y_1 = y_2y1​=y2​, z1=z2z_1 = z_2z1​=z2​):

  1. 5t=βˆ’1βˆ’6s5t = -1-6s5t=βˆ’1βˆ’6s

  2. βˆ’13βˆ’6t=βˆ’12βˆ’12s-13-6t = -12-12sβˆ’13βˆ’6t=βˆ’12βˆ’12s

  3. 19βˆ’t=19βˆ’18s19-t = 19-18s19βˆ’t=19βˆ’18s

Solve the system using equations (1) and (3):

From equation (3), we can simplify by subtracting 19 from both sides:

βˆ’t=βˆ’18sβ€…β€ŠβŸΉβ€…β€Št=18s-t = -18s \implies t = 18sβˆ’t=βˆ’18s⟹t=18s

Substitute t=18st = 18st=18s into equation (1):

5(18s)=βˆ’1βˆ’6s5(18s) = -1 - 6s5(18s)=βˆ’1βˆ’6s

90s=βˆ’1βˆ’6s90s = -1 - 6s90s=βˆ’1βˆ’6s

96s=βˆ’1β€…β€ŠβŸΉβ€…β€Šs=βˆ’19696s = -1 \implies s = -\frac{1}{96}96s=βˆ’1⟹s=βˆ’961​

Now find ttt:

t=18(βˆ’196)=βˆ’316t = 18\left(-\frac{1}{96}\right) = -\frac{3}{16}t=18(βˆ’961​)=βˆ’163​

Test the values in the remaining equation (2):

We must check if these values for ttt and sss satisfy equation (2) to see if the lines actually cross:

LeftΒ SideΒ (LS):Β βˆ’13βˆ’6(βˆ’316)=βˆ’13+98=βˆ’1048+98=βˆ’958=βˆ’11.875\text{Left Side (LS): } -13 - 6\left(-\frac{3}{16}\right) = -13 + \frac{9}{8} = -\frac{104}{8} + \frac{9}{8} = -\frac{95}{8} = -11.875LeftΒ SideΒ (LS):Β βˆ’13βˆ’6(βˆ’163​)=βˆ’13+89​=βˆ’8104​+89​=βˆ’895​=βˆ’11.875

RightΒ SideΒ (RS):Β βˆ’12βˆ’12(βˆ’196)=βˆ’12+18=βˆ’968+18=βˆ’958=βˆ’11.875\text{Right Side (RS): } -12 - 12\left(-\frac{1}{96}\right) = -12 + \frac{1}{8} = -\frac{96}{8} + \frac{1}{8} = -\frac{95}{8} = -11.875RightΒ SideΒ (RS):Β βˆ’12βˆ’12(βˆ’961​)=βˆ’12+81​=βˆ’896​+81​=βˆ’895​=βˆ’11.875

Since LS=RS\text{LS} = \text{RS}LS=RS, the system is consistent! The lines share a common intersection point.

Conclusion

Because the direction vectors are not parallel and the lines share a common point, the lines are Intersecting.

  • Equal

  • Parallel

  • Skew (Incorrect option)

  • Intersecting (Correct Answer)

Active Practice Problem

Given line A running through the points A1=(2,0,3)A_{1}=(2,0,3)A1​=(2,0,3) and A2=(4,7,8)A_{2}=(4,7,8)A2​=(4,7,8) as well as line B running through the points B1=(βˆ’3,βˆ’1,4)B_{1}=(-3,-1,4)B1​=(βˆ’3,βˆ’1,4) and B2=(βˆ’1,5,9)B_{2}=(-1,5,9)B2​=(βˆ’1,5,9), determine if the lines A and B are equal, parallel but not skew, skew, or intersecting.

  • Equal
  • Parallel
  • Skew
  • Intersecting
Solution Key:

Here is the step-by-step solution for Problem S3.1 to determine the relationship between line A and line B.

Given Data
  • Line A passes through: A1=(2,0,3)A_1 = (2, 0, 3)A1​=(2,0,3) and A2=(4,7,8)A_2 = (4, 7, 8)A2​=(4,7,8)

  • Line B passes through: B1=(βˆ’3,βˆ’1,4)B_1 = (-3, -1, 4)B1​=(βˆ’3,βˆ’1,4) and B2=(βˆ’1,5,9)B_2 = (-1, 5, 9)B2​=(βˆ’1,5,9)

Step 1: Find and Compare Direction Vectors

First, we calculate the direction vectors (u⃗\vec{u}u and v⃗\vec{v}v) for both lines by subtracting their given coordinates:

  • Direction vector for Line A (uβƒ—\vec{u}u):

uβƒ—=A1A2βƒ—=⟨4βˆ’2,Β 7βˆ’0,Β 8βˆ’3⟩=⟨2,7,5⟩\vec{u} = \vec{A_1A_2} = \langle 4 - 2, \ 7 - 0, \ 8 - 3 \rangle = \langle 2, 7, 5 \rangleu=A1​A2​​=⟨4βˆ’2,Β 7βˆ’0,Β 8βˆ’3⟩=⟨2,7,5⟩

  • Direction vector for Line B (vβƒ—\vec{v}v):

vβƒ—=B1B2βƒ—=βŸ¨βˆ’1βˆ’(βˆ’3),Β 5βˆ’(βˆ’1),Β 9βˆ’4⟩=⟨2,6,5⟩\vec{v} = \vec{B_1B_2} = \langle -1 - (-3), \ 5 - (-1), \ 9 - 4 \rangle = \langle 2, 6, 5 \ranglev=B1​B2​​=βŸ¨βˆ’1βˆ’(βˆ’3),Β 5βˆ’(βˆ’1),Β 9βˆ’4⟩=⟨2,6,5⟩

Now we check if the direction vectors are parallel (u⃗=av⃗\vec{u} = a\vec{v}u=av): Comparing the components:

  • xxx-component ratio: 22=1\frac{2}{2} = 122​=1

  • yyy-component ratio: 76\frac{7}{6}67​

Since 22β‰ 76\frac{2}{2} \neq \frac{7}{6}22​=67​, the direction vectors are not parallel. Based on the classification table, the lines must be either Intersecting or Skew.

Step 2: Write Parametric Equations for Both Lines

To check if they share a common point, we first write out their parametric forms using A1A_1A1​ and B1B_1B1​ as our initial points:

  • Line A (using parameter ttt):

x=2+2tx = 2 + 2tx=2+2t

y=0+7t=7ty = 0 + 7t = 7ty=0+7t=7t

z=3+5tz = 3 + 5tz=3+5t

  • Line B (using parameter sss):

x=βˆ’3+2sx = -3 + 2sx=βˆ’3+2s

y=βˆ’1+6sy = -1 + 6sy=βˆ’1+6s

z=4+5sz = 4 + 5sz=4+5s

Step 3: Check for an Intersection Point

We set the corresponding coordinate equations equal to one another (xA=xBx_A = x_BxA​=xB​, yA=yBy_A = y_ByA​=yB​, zA=zBz_A = z_BzA​=zB​):

  1. 2+2t=βˆ’3+2s2 + 2t = -3 + 2s2+2t=βˆ’3+2s

  2. 7t=βˆ’1+6s7t = -1 + 6s7t=βˆ’1+6s

  3. 3+5t=4+5s3 + 5t = 4 + 5s3+5t=4+5s

Solve the system using equations (1) and (3):

From equation (3), subtract 5s5s5s and 3 from both sides:

5tβˆ’5s=1β€…β€ŠβŸΉβ€…β€Š5(tβˆ’s)=1β€…β€ŠβŸΉβ€…β€Štβˆ’s=155t - 5s = 1 \implies 5(t - s) = 1 \implies t - s = \frac{1}{5}5tβˆ’5s=1⟹5(tβˆ’s)=1⟹tβˆ’s=51​

From equation (1), rearrange to group ttt and sss:

2tβˆ’2s=βˆ’5β€…β€ŠβŸΉβ€…β€Š2(tβˆ’s)=βˆ’5β€…β€ŠβŸΉβ€…β€Štβˆ’s=βˆ’522t - 2s = -5 \implies 2(t - s) = -5 \implies t - s = -\frac{5}{2}2tβˆ’2s=βˆ’5⟹2(tβˆ’s)=βˆ’5⟹tβˆ’s=βˆ’25​

Notice the contradiction:

From equation (3) we get tβˆ’s=0.2t - s = 0.2tβˆ’s=0.2, but from equation (1) we get tβˆ’s=βˆ’2.5t - s = -2.5tβˆ’s=βˆ’2.5. Because 0.2β‰ βˆ’2.50.2 \neq -2.50.2ξ€ =βˆ’2.5, it is mathematically impossible to find values for ttt and sss that satisfy this system. The system is inconsistent, meaning the lines do not share a common point.

Conclusion

Since the direction vectors are not parallel and the lines do not share a common point, the lines are Skew.

  • Equal

  • Parallel

  • Skew (Correct Answer)

  • Intersecting

Show your steps and calculations here.

Regroup 3

  • Verify calculations and mathematical reasoning.

Synthesis Wrap-up

  • Core takeaways from Session 04 and overview of homework homework assignment: Equations of Lines and Planes in Space.