MATH-283 (Calculus III) Curriculum

Session 02 - Vectors in 2D and 3D

Handout Worksheet
Fall Semester 2026
Session Objectives & Overview

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

  • Plot coordinates and calculate distances/equations of spheres in a 3D rectangular coordinate system.
  • Represent vectors in component form and unit-vector notation in 2D and 3D, and calculate their magnitudes and directions.
  • Perform vector operations (addition, subtraction, scalar multiplication, unit vectors) and apply them to model physical systems in static equilibrium.

Micro-Lecture

1. 3D Coordinates & Spatial Geometry

  • Mathematical Foundation: In the three-dimensional rectangular coordinate system, points are represented as ordered triples (x,y,z)(x, y, z)(x,y,z). The distance between two points P1(x1,y1,z1)P_1(x_1, y_1, z_1)P1​(x1​,y1​,z1​) and P2(x2,y2,z2)P_2(x_2, y_2, z_2)P2​(x2​,y2​,z2​) is d=(x2−x1)2+(y2−y1)2+(z2−z1)2d = \sqrt{(x_2-x_1)^2 + (y_2-y_1)^2 + (z_2-z_1)^2}d=(x2​−x1​)2+(y2​−y1​)2+(z2​−z1​)2​. A sphere centered at (h,k,l)(h, k, l)(h,k,l) with radius rrr is described by the equation (x−h)2+(y−k)2+(z−l)2=r2(x-h)^2 + (y-k)^2 + (z-l)^2 = r^2(x−h)2+(y−k)2+(z−l)2=r2.
  • Engineering Context: Necessary for mapping physical assets in 3D space, coordinate transformations in robotics, modeling spherical blast ranges, and structural piping designs.

2. Vectors and Unit Vector Notation

  • Mathematical Foundation: A vector v⃗\vec{v}v represents a directed line segment with component form ⟨vx,vy,vz⟩\langle v_x, v_y, v_z \rangle⟨vx​,vy​,vz​⟩ or standard unit vector form vxi^+vyj^+vzk^v_x\hat{i} + v_y\hat{j} + v_z\hat{k}vx​i^+vy​j^​+vz​k^. The magnitude is ∣v⃗∣=vx2+vy2+vz2|\vec{v}| = \sqrt{v_x^2 + v_y^2 + v_z^2}∣v∣=vx2​+vy2​+vz2​​. A unit vector in the direction of v⃗\vec{v}v is U^v=v⃗∣v⃗∣\hat{U}_v = \frac{\vec{v}}{|\vec{v}|}U^v​=∣v∣v​, which has a magnitude of 1.
  • Engineering Context: Used to define directional loads on joints in CAD modeling, velocity fields in aerodynamics, and electric fields in power systems.

3. Vector Arithmetic & Static Equilibrium

  • Mathematical Foundation: Vector addition u⃗+v⃗\vec{u} + \vec{v}u+v and scalar multiplication cv⃗c\vec{v}cv are performed component-wise. Under static equilibrium conditions, the net external force vector acting on a point-mass is zero: ∑F⃗=0⃗\sum \vec{F} = \vec{0}∑F=0, which requires the horizontal and vertical components to independently sum to zero.
  • Engineering Context: Crucial for calculating tension loads in support cables, resolving wind loads on structures, and structural analysis of crane supports.

Skill Block 1

Worked Example A: Distance in 3D

Calculate the distance between the two points P=(5,−2,−1)P = (5, -2, -1)P=(5,−2,−1) and Q=(−2,4,−6)Q = (-2, 4, -6)Q=(−2,4,−6).

Worked Solution:
  1. Identify Coordinates: Let P=(x1,y1,z1)=(5,−2,−1)P = (x_1, y_1, z_1) = (5, -2, -1)P=(x1​,y1​,z1​)=(5,−2,−1) and Q=(x2,y2,z2)=(−2,4,−6)Q = (x_2, y_2, z_2) = (-2, 4, -6)Q=(x2​,y2​,z2​)=(−2,4,−6).
  2. Apply Distance Formula:
    d=(−2−5)2+(4−(−2))2+(−6−(−1))2d = \sqrt{(-2 - 5)^2 + (4 - (-2))^2 + (-6 - (-1))^2}d=(−2−5)2+(4−(−2))2+(−6−(−1))2​
  3. Simplify:
    d=(−7)2+62+(−5)2=49+36+25=110≈10.49d = \sqrt{(-7)^2 + 6^2 + (-5)^2} = \sqrt{49 + 36 + 25} = \sqrt{110} \approx 10.49d=(−7)2+62+(−5)2​=49+36+25​=110​≈10.49

Worked Example B: Equation of a Sphere

Find the standard equation of the sphere centered at (3,−4,2)(3, -4, 2)(3,−4,2) with a radius of 666.

Worked Solution:
  1. Identify the Center and Radius: (h,k,l)=(3,−4,2)(h, k, l) = (3, -4, 2)(h,k,l)=(3,−4,2) and r=6r = 6r=6.
  2. Substitute into standard form:
    (x−3)2+(y−(−4))2+(z−2)2=62(x - 3)^2 + (y - (-4))^2 + (z - 2)^2 = 6^2(x−3)2+(y−(−4))2+(z−2)2=62
  3. Simplify:
    (x−3)2+(y+4)2+(z−2)2=36(x - 3)^2 + (y + 4)^2 + (z - 2)^2 = 36(x−3)2+(y+4)2+(z−2)2=36

Worked Example C: Center and Radius of a Sphere

Find the center and radius of the sphere defined by the equation x2+y2+z2−6x+8y−2z−10=0x^2 + y^2 + z^2 - 6x + 8y - 2z - 10 = 0x2+y2+z2−6x+8y−2z−10=0.

Worked Solution:
  1. Group Variable Terms:
    (x2−6x)+(y2+8y)+(z2−2z)=10(x^2 - 6x) + (y^2 + 8y) + (z^2 - 2z) = 10(x2−6x)+(y2+8y)+(z2−2z)=10
  2. Complete the Square for Each Variable: (Note: Refer to Completing the Square for a detailed refresher on this algebraic technique.)
    • For xxx: add (−62)2=9\left(\frac{-6}{2}\right)^2 = 9(2−6​)2=9
    • For yyy: add (82)2=16\left(\frac{8}{2}\right)^2 = 16(28​)2=16
    • For zzz: add (−22)2=1\left(\frac{-2}{2}\right)^2 = 1(2−2​)2=1 Add these values to both sides of the equation:
      (x2−6x+9)+(y2+8y+16)+(z2−2z+1)=10+9+16+1(x^2 - 6x + 9) + (y^2 + 8y + 16) + (z^2 - 2z + 1) = 10 + 9 + 16 + 1(x2−6x+9)+(y2+8y+16)+(z2−2z+1)=10+9+16+1
  3. Write in Standard Form:
    (x−3)2+(y+4)2+(z−1)2=36(x - 3)^2 + (y + 4)^2 + (z - 1)^2 = 36(x−3)2+(y+4)2+(z−1)2=36
    The center is (3,−4,1)(3, -4, 1)(3,−4,1) and the radius is r=36=6r = \sqrt{36} = 6r=36​=6.

Practice Problem 1: Concept & Reading Check

Open this Skill Block on the Memex to locate the information needed to answer the following:

  • (a) Under the Conceptual Framework section, describe the Right-Hand Rule and how it determines the positive zzz-axis.
  • (b) Look at the Key Equations & Structural Rules section. What is the standard form equation of a sphere with center (h,k,l)(h, k, l)(h,k,l) and radius rrr?
  • (c) Trace Worked Example C. Why is the algebraic technique "Completing the Square" used to rewrite the sphere's equation? What values were added to both sides of the equation?
Solution Key:
  • (a) As outlined in the Conceptual Framework section, the Right-Hand Rule establishes the 3D coordinate orientation. Pointing your right index finger along positive xxx and curling your fingers to positive yyy leaves your thumb pointing along the positive zzz-axis.
  • (b) According to the Key Equations & Structural Rules section, the standard equation of a sphere is (x−h)2+(y−k)2+(z−l)2=r2(x-h)^2 + (y-k)^2 + (z-l)^2 = r^2(x−h)2+(y−k)2+(z−l)2=r2, where (h,k,l)(h, k, l)(h,k,l) is the center coordinate and rrr is the radius.
  • (c) Tracing Worked Example C, the given equation is x2+y2+z2−6x+8y−2z−10=0x^2 + y^2 + z^2 - 6x + 8y - 2z - 10 = 0x2+y2+z2−6x+8y−2z−10=0. Completing the square groups the quadratic and linear terms for each variable to rewrite them in standard squared form. To balance the equation, we add (−6/2)2=9(-6/2)^2 = 9(−6/2)2=9 for xxx, (8/2)2=16(8/2)^2 = 16(8/2)2=16 for yyy, and (−2/2)2=1(-2/2)^2 = 1(−2/2)2=1 for zzz to both sides, transforming the constants on the right side to 10+9+16+1=3610 + 9 + 16 + 1 = 3610+9+16+1=36.
Show your steps and calculations here.

Practice Problem 2

Label the axes in the coordinate system below according to the right-hand rule, and plot the points A=(5,−4,0)A = (5, -4, 0)A=(5,−4,0), B=(0,3,0)B = (0, 3, 0)B=(0,3,0), and C=(1,3,2)C = (1, 3, 2)C=(1,3,2).

Empty 3D Plot.png
Solution Key:
  1. Establish the Axes: Following the standard convention for the right-hand rule:
    • The xxx-axis points diagonally forward and to the left.
    • The yyy-axis points horizontally to the right.
    • The zzz-axis points vertically upward.
  2. Plot Point A (5, -4, 0):
    • Move 555 units forward along the positive xxx-axis.
    • Move 444 units parallel to the negative yyy-axis (to the left).
    • Since the zzz-coordinate is 000, the point lies directly on the xyxyxy-plane.
  3. Plot Point B (0, 3, 0):
    • The xxx- and zzz-coordinates are 000.
    • Move 333 units to the right along the positive yyy-axis.
  4. Plot Point C (1, 3, 2):
    • Move 111 unit forward along the positive xxx-axis.
    • Move 333 units to the right parallel to the positive yyy-axis.
    • Move 222 units upward parallel to the positive zzz-axis.
Show your steps and calculations here.

Practice Problem 3

Determine if the equation x2+y2+z2+8x−4y+12z+47=0x^2 + y^2 + z^2 + 8x - 4y + 12z + 47 = 0x2+y2+z2+8x−4y+12z+47=0 represents a sphere. If it does, find its center and radius.

Solution Key:
  1. Group terms:
    (x2+8x)+(y2−4y)+(z2+12z)=−47(x^2 + 8x) + (y^2 - 4y) + (z^2 + 12z) = -47(x2+8x)+(y2−4y)+(z2+12z)=−47
  2. Complete the square: (Apply the Completing the Square technique to each variable):
    • For xxx: add (82)2=16\left(\frac{8}{2}\right)^2 = 16(28​)2=16
    • For yyy: add (−42)2=4\left(\frac{-4}{2}\right)^2 = 4(2−4​)2=4
    • For zzz: add (122)2=36\left(\frac{12}{2}\right)^2 = 36(212​)2=36 Add these to both sides:
      (x2+8x+16)+(y2−4y+4)+(z2+12z+36)=−47+16+4+36(x^2 + 8x + 16) + (y^2 - 4y + 4) + (z^2 + 12z + 36) = -47 + 16 + 4 + 36(x2+8x+16)+(y2−4y+4)+(z2+12z+36)=−47+16+4+36
  3. Simplify:
    (x+4)2+(y−2)2+(z+6)2=9(x + 4)^2 + (y - 2)^2 + (z + 6)^2 = 9(x+4)2+(y−2)2+(z+6)2=9
    Since the right side is positive (9>09 > 09>0), it is a sphere. Center: (−4,2,−6)(-4, 2, -6)(−4,2,−6) Radius: r=9=3r = \sqrt{9} = 3r=9​=3

Show your steps and calculations here.

Regroup 1

  • Review coordinate axes orientations and right-hand rule.
  • Address common errors in completing the square (e.g. sign errors and forgetting to add terms to both sides).

Skill Block 2

Worked Example A: Vector Components and Magnitude

Given the points P1=(2,3)P_1 = (2, 3)P1​=(2,3) and P2=(4,4)P_2 = (4, 4)P2​=(4,4), find the vector P⃗\vec{P}P starting at P1P_1P1​ and ending at P2P_2P2​ in component form and calculate its magnitude.

Worked Solution:
  1. Find components:
    Px=4−2=2P_x = 4 - 2 = 2Px​=4−2=2
    Py=4−3=1P_y = 4 - 3 = 1Py​=4−3=1
    Component form: P⃗=⟨2,1⟩\vec{P} = \langle 2, 1 \rangleP=⟨2,1⟩ (or unit vector form: P⃗=2i^+1j^\vec{P} = 2\hat{i} + 1\hat{j}P=2i^+1j^​).
  2. Calculate magnitude:
    ∣∣P⃗∣∣=Px2+Py2=22+12=5||\vec{P}|| = \sqrt{P_x^2 + P_y^2} = \sqrt{2^2 + 1^2} = \sqrt{5}∣∣P∣∣=Px2​+Py2​​=22+12​=5​

Worked Example B: 3D Vector Representation

A cable exerts a force of magnitude 580580580 N along a line pointing from the origin to the point (250,100,500)(250, 100, 500)(250,100,500) in millimeters. Write the force vector in component form.

Worked Solution:
  1. Find the direction vector: Let v⃗=⟨250,100,500⟩\vec{v} = \langle 250, 100, 500 \ranglev=⟨250,100,500⟩.
  2. Compute magnitude of direction vector:
    ∣v⃗∣=2502+1002+5002=62500+10000+250000=322500≈567.89|\vec{v}| = \sqrt{250^2 + 100^2 + 500^2} = \sqrt{62500 + 10000 + 250000} = \sqrt{322500} \approx 567.89∣v∣=2502+1002+5002​=62500+10000+250000​=322500​≈567.89
  3. Find the unit vector:
    U^v=v⃗∣v⃗∣≈⟨0.4402,0.1761,0.8805⟩\hat{U}_v = \frac{\vec{v}}{|\vec{v}|} \approx \langle 0.4402, 0.1761, 0.8805 \rangleU^v​=∣v∣v​≈⟨0.4402,0.1761,0.8805⟩
  4. Scale unit vector by force magnitude:
    F⃗=580⋅U^v≈⟨255.33,102.13,510.68⟩ N\vec{F} = 580 \cdot \hat{U}_v \approx \langle 255.33, 102.13, 510.68 \rangle\text{ N}F=580⋅U^v​≈⟨255.33,102.13,510.68⟩ N

Worked Example C: Components from Angle

A vector V⃗\vec{V}V has magnitude 777 and makes a 30∘30^\circ30∘ angle with the positive xxx-axis. Find its horizontal and vertical components.

Worked Solution:
  1. Apply trigonometric formulas:
    Vx=∣V⃗∣cos⁡(30∘)V_x = |\vec{V}|\cos(30^\circ)Vx​=∣V∣cos(30∘)
    Vy=∣V⃗∣sin⁡(30∘)V_y = |\vec{V}|\sin(30^\circ)Vy​=∣V∣sin(30∘)
  2. Evaluate components:
    Vx=7⋅32=732≈6.06V_x = 7 \cdot \frac{\sqrt{3}}{2} = \frac{7\sqrt{3}}{2} \approx 6.06Vx​=7⋅23​​=273​​≈6.06
    Vy=7⋅12=3.5V_y = 7 \cdot \frac{1}{2} = 3.5Vy​=7⋅21​=3.5
    Component form: V⃗=⟨732,72⟩\vec{V} = \langle \frac{7\sqrt{3}}{2}, \frac{7}{2} \rangleV=⟨273​​,27​⟩.

Practice Problem 4: Concept & Reading Check

Open this Skill Block on the Memex to locate the information needed to answer the following:

  • (a) Under the Conceptual Framework section, what is the difference between component form and unit-vector notation for representing a vector in 3D?
  • (b) According to the Key Equations & Structural Rules section, what is the formula for calculating a displacement vector PQ⃗\vec{PQ}PQ​ from points PPP and QQQ?
  • (c) Trace Worked Example B. Explain why we calculate a unit vector U^v\hat{U}_vU^v​ first before scaling it by the force magnitude of 580580580 N.
Solution Key:
  • (a) As explained in the Conceptual Framework section, a 3D vector can be written in two equivalent notations: component form using bracket notation ⟨vx,vy,vz⟩\langle v_x, v_y, v_z \rangle⟨vx​,vy​,vz​⟩, or unit-vector notation using the standard coordinate basis vectors vxi^+vyj^+vzk^v_x\hat{i} + v_y\hat{j} + v_z\hat{k}vx​i^+vy​j^​+vz​k^.
  • (b) According to the Key Equations & Structural Rules section, a displacement vector PQ⃗\vec{PQ}PQ​ representing the path from initial point PPP to terminal point QQQ is computed by subtracting the coordinates of PPP from QQQ: PQ⃗=⟨xQ−xP,yQ−yP,zQ−zP⟩\vec{PQ} = \langle x_Q - x_P, y_Q - y_P, z_Q - z_P \ranglePQ​=⟨xQ​−xP​,yQ​−yP​,zQ​−zP​⟩.
  • (c) In Worked Example B, the direction of the force is along the vector v⃗=⟨250,100,500⟩\vec{v} = \langle 250, 100, 500 \ranglev=⟨250,100,500⟩. Since this direction vector has a magnitude other than 1, we first convert it to a unit vector U^v=v⃗/∣v⃗∣\hat{U}_v = \vec{v}/|\vec{v}|U^v​=v/∣v∣ (which has magnitude 1). Multiplying this unit vector by the force magnitude of 580580580 N yields a vector that is collinear with v⃗\vec{v}v but scales the physical force magnitude correctly.
Show your steps and calculations here.

Practice Problem 5

Given the vector v⃗=⟨1,−3⟩\vec{v} = \langle 1, -3 \ranglev=⟨1,−3⟩:

  1. Draw the vector starting from the origin.
  2. Find the magnitude of the vector.
Solution Key:
  1. Draw the Vector:
    • Start at the origin (0,0)(0, 0)(0,0).
    • Move 111 unit to the right along the xxx-axis.
    • Move 333 units down along the yyy-axis.
    • Draw an arrow from (0,0)(0, 0)(0,0) to the point (1,−3)(1, -3)(1,−3).
  2. Compute the Magnitude:
    ∣v⃗∣=12+(−3)2=1+9=10≈3.16|\vec{v}| = \sqrt{1^2 + (-3)^2} = \sqrt{1 + 9} = \sqrt{10} \approx 3.16∣v∣=12+(−3)2​=1+9​=10​≈3.16
Show your steps and calculations here.

Practice Problem 6

A directional antenna points along a line from P(1,−2,3)P(1, -2, 3)P(1,−2,3) to Q(3,4,0)Q(3, 4, 0)Q(3,4,0). Write the direction vector d⃗=PQ⃗\vec{d} = \vec{PQ}d=PQ​ in unit-vector notation, and find a unit vector in the same direction.

Solution Key:
  1. Calculate displacement vector:
    d⃗=⟨3−1,4−(−2),0−3⟩=⟨2,6,−3⟩\vec{d} = \langle 3 - 1, 4 - (-2), 0 - 3 \rangle = \langle 2, 6, -3 \rangled=⟨3−1,4−(−2),0−3⟩=⟨2,6,−3⟩
    In unit-vector notation: d⃗=2i^+6j^−3k^\vec{d} = 2\hat{i} + 6\hat{j} - 3\hat{k}d=2i^+6j^​−3k^.
  2. Compute magnitude:
    ∣d⃗∣=22+62+(−3)2=4+36+9=49=7|\vec{d}| = \sqrt{2^2 + 6^2 + (-3)^2} = \sqrt{4 + 36 + 9} = \sqrt{49} = 7∣d∣=22+62+(−3)2​=4+36+9​=49​=7
  3. Compute unit vector:
    U^d=d⃗∣d⃗∣=2i^+6j^−3k^7=27i^+67j^−37k^\hat{U}_d = \frac{\vec{d}}{|\vec{d}|} = \frac{2\hat{i} + 6\hat{j} - 3\hat{k}}{7} = \frac{2}{7}\hat{i} + \frac{6}{7}\hat{j} - \frac{3}{7}\hat{k}U^d​=∣d∣d​=72i^+6j^​−3k^​=72​i^+76​j^​−73​k^

Show your steps and calculations here.

Regroup 2

  • Differentiate between coordinates of a point (x,y,z)(x,y,z)(x,y,z) and components of a vector ⟨vx,vy,vz⟩\langle v_x, v_y, v_z \rangle⟨vx​,vy​,vz​⟩.
  • Review notation conventions (bold letters v\mathbf{v}v vs. arrows v⃗\vec{v}v, and unit vectors i^,j^,k^\hat{i}, \hat{j}, \hat{k}i^,j^​,k^).

Skill Block 3

Worked Example A: Vector Combinations

Given the vectors v⃗=3i^+4j^\vec{v} = 3\hat{i} + 4\hat{j}v=3i^+4j^​ and u⃗=2i^−2j^\vec{u} = 2\hat{i} - 2\hat{j}u=2i^−2j^​, calculate the vector sum u⃗+v⃗\vec{u} + \vec{v}u+v and find the vector w⃗=3(u⃗+v⃗)\vec{w} = 3(\vec{u} + \vec{v})w=3(u+v).

Worked Solution:
  1. Calculate u⃗+v⃗\vec{u} + \vec{v}u+v:
    u⃗+v⃗=(3+2)i^+(4−2)j^=5i^+2j^\vec{u} + \vec{v} = (3 + 2)\hat{i} + (4 - 2)\hat{j} = 5\hat{i} + 2\hat{j}u+v=(3+2)i^+(4−2)j^​=5i^+2j^​
  2. Calculate w⃗=3(u⃗+v⃗)\vec{w} = 3(\vec{u} + \vec{v})w=3(u+v):
    w⃗=3(5i^+2j^)=15i^+6j^=⟨15,6⟩\vec{w} = 3(5\hat{i} + 2\hat{j}) = 15\hat{i} + 6\hat{j} = \langle 15, 6 \ranglew=3(5i^+2j^​)=15i^+6j^​=⟨15,6⟩

Worked Example B: Resultant Force from Wind and Current

A boat in a river experiences two forces: a river current force c=⟨2,0⟩\mathbf{c} = \langle 2, 0 \ranglec=⟨2,0⟩ kN and a wind thrust force t=⟨0,3⟩\mathbf{t} = \langle 0, 3 \ranglet=⟨0,3⟩ kN. Add the forces to find the resultant force v=c+t\mathbf{v} = \mathbf{c} + \mathbf{t}v=c+t acting on the boat and calculate its magnitude.

Worked Solution:
  1. Add components: (Refer to Combining Forces and Force Components for a review of how to represent and add force vectors component-wise to find their equivalent single resultant force.)
    v=⟨2+0,0+3⟩=⟨2,3⟩ kN\mathbf{v} = \langle 2 + 0, 0 + 3 \rangle = \langle 2, 3 \rangle\text{ kN}v=⟨2+0,0+3⟩=⟨2,3⟩ kN
  2. Calculate magnitude:
    ∣v∣=22+32=4+9=13≈3.61 kN|\mathbf{v}| = \sqrt{2^2 + 3^2} = \sqrt{4 + 9} = \sqrt{13} \approx 3.61\text{ kN}∣v∣=22+32​=4+9​=13​≈3.61 kN

Worked Example C: Vector Equations

Consider the vector F=⟨−3,4,0⟩\mathbf{F} = \langle -3, 4, 0 \rangleF=⟨−3,4,0⟩. Compute the vectors 3F3\mathbf{F}3F, −2F-2\mathbf{F}−2F, and find the unit vector U^F\hat{U}_FU^F​.

Worked Solution:
  1. Compute 3F3\mathbf{F}3F:
    3F=3⟨−3,4,0⟩=⟨−9,12,0⟩3\mathbf{F} = 3\langle -3, 4, 0 \rangle = \langle -9, 12, 0 \rangle3F=3⟨−3,4,0⟩=⟨−9,12,0⟩
  2. Compute −2F-2\mathbf{F}−2F:
    −2F=−2⟨−3,4,0⟩=⟨6,−8,0⟩-2\mathbf{F} = -2\langle -3, 4, 0 \rangle = \langle 6, -8, 0 \rangle−2F=−2⟨−3,4,0⟩=⟨6,−8,0⟩
  3. Compute the unit vector U^F\hat{U}_FU^F​: First, calculate magnitude:
    ∣F∣=(−3)2+42+02=9+16=5|\mathbf{F}| = \sqrt{(-3)^2 + 4^2 + 0^2} = \sqrt{9 + 16} = 5∣F∣=(−3)2+42+02​=9+16​=5
    Divide vector by magnitude:
    U^F=F5=⟨−0.6,0.8,0⟩\hat{U}_F = \frac{\mathbf{F}}{5} = \langle -0.6, 0.8, 0 \rangleU^F​=5F​=⟨−0.6,0.8,0⟩

Practice Problem 7: Concept & Reading Check

Open this Skill Block on the Memex to locate the information needed to answer the following:

  • (a) Under the Conceptual Framework section, what mathematical condition must be satisfied for a physical system of vectors to be in static equilibrium?
  • (b) Look at the Key Equations & Structural Rules section. Write down the equations that represent static equilibrium in component-wise form for 3D space.
  • (c) Trace the linked Engineering Application under the Engineering Applications section. How does the concept of static equilibrium apply to the stage lighting system described?
Solution Key:
  • (a) According to the Conceptual Framework section, static equilibrium requires that a system is in a state of zero net force. Mathematically, the vector sum of all external forces acting on the body must equal the zero vector: ∑F⃗=0⃗\sum \vec{F} = \vec{0}∑F=0.
  • (b) As stated in the Key Equations & Structural Rules section, in three-dimensional space, the vector equilibrium condition translates to three independent scalar equations: the sum of the horizontal, vertical, and depth force components must each equal zero (∑Fx=0\sum F_x = 0∑Fx​=0, ∑Fy=0\sum F_y = 0∑Fy​=0, ∑Fz=0\sum F_z = 0∑Fz​=0).
  • (c) In the linked Engineering Application under "Suspended Stage Lighting", the stage lights represent a stationary mass. By applying static equilibrium, entertainment engineers can calculate the exact tension forces in the supporting cables to ensure they do not exceed safety limits and that the structure remains completely stable.
Show your steps and calculations here.

Practice Problem 8

An offshore oil platform structural support ring is subjected to three cable force vectors: F⃗1=⟨10,−5,8⟩\vec{F}_1 = \langle 10, -5, 8 \rangleF1​=⟨10,−5,8⟩ kN, F⃗2=⟨−4,12,−3⟩\vec{F}_2 = \langle -4, 12, -3 \rangleF2​=⟨−4,12,−3⟩ kN, and F⃗3=⟨−6,−7,−5⟩\vec{F}_3 = \langle -6, -7, -5 \rangleF3​=⟨−6,−7,−5⟩ kN. Find the resultant force vector F⃗R=F⃗1+F⃗2+F⃗3\vec{F}_R = \vec{F}_1 + \vec{F}_2 + \vec{F}_3FR​=F1​+F2​+F3​. Is the ring in static equilibrium?

Solution Key:
  1. Sum the xxx-components:
    FRx=10+(−4)+(−6)=0 kNF_{Rx} = 10 + (-4) + (-6) = 0\text{ kN}FRx​=10+(−4)+(−6)=0 kN
  2. Sum the yyy-components:
    FRy=−5+12+(−7)=0 kNF_{Ry} = -5 + 12 + (-7) = 0\text{ kN}FRy​=−5+12+(−7)=0 kN
  3. Sum the zzz-components:
    FRz=8+(−3)+(−5)=0 kNF_{Rz} = 8 + (-3) + (-5) = 0\text{ kN}FRz​=8+(−3)+(−5)=0 kN
    The resultant force vector is:
    F⃗R=⟨0,0,0⟩ kN\vec{F}_R = \langle 0, 0, 0 \rangle\text{ kN}FR​=⟨0,0,0⟩ kN
    Since F⃗R=0⃗\vec{F}_R = \vec{0}FR​=0, the support ring is in static equilibrium.
Show your steps and calculations here.

Practice Problem 9

A weight of 350350350 N is suspended by two cables. Cable A makes an angle of 20∘20^\circ20∘ with the horizontal ceiling (pulling up and left), and Cable B makes an angle of 40∘40^\circ40∘ with the horizontal ceiling (pulling up and right). Calculate the tension magnitudes TAT_ATA​ and TBT_BTB​ in each cable. (Round to 2 decimal places).

Solution Key:
  1. Decompose the forces into components: (Use the methods outlined in Force Components to resolve the angled tension vectors into xxx- and yyy-components):
    • Cable A: T⃗A=⟨−TAcos⁡(20∘),TAsin⁡(20∘)⟩\vec{T}_A = \langle -T_A\cos(20^\circ), T_A\sin(20^\circ) \rangleTA​=⟨−TA​cos(20∘),TA​sin(20∘)⟩
    • Cable B: T⃗B=⟨TBcos⁡(40∘),TBsin⁡(40∘)⟩\vec{T}_B = \langle T_B\cos(40^\circ), T_B\sin(40^\circ) \rangleTB​=⟨TB​cos(40∘),TB​sin(40∘)⟩
    • Weight: F⃗g=⟨0,−350⟩\vec{F}_g = \langle 0, -350 \rangleFg​=⟨0,−350⟩
  2. Apply horizontal equilibrium (∑Fx=0\sum F_x = 0∑Fx​=0):
    −TAcos⁡(20∘)+TBcos⁡(40∘)=0  ⟹  TB=TAcos⁡(20∘)cos⁡(40∘)≈1.22668 TA-T_A \cos(20^\circ) + T_B \cos(40^\circ) = 0 \implies T_B = T_A \frac{\cos(20^\circ)}{\cos(40^\circ)} \approx 1.22668 \, T_A−TA​cos(20∘)+TB​cos(40∘)=0⟹TB​=TA​cos(40∘)cos(20∘)​≈1.22668TA​
  3. Apply vertical equilibrium (∑Fy=0\sum F_y = 0∑Fy​=0):
    TAsin⁡(20∘)+TBsin⁡(40∘)−350=0  ⟹  TAsin⁡(20∘)+TBsin⁡(40∘)=350T_A \sin(20^\circ) + T_B \sin(40^\circ) - 350 = 0 \implies T_A \sin(20^\circ) + T_B \sin(40^\circ) = 350TA​sin(20∘)+TB​sin(40∘)−350=0⟹TA​sin(20∘)+TB​sin(40∘)=350
  4. Substitute TBT_BTB​ into vertical equation:
    TAsin⁡(20∘)+(1.22668 TA)sin⁡(40∘)=350T_A \sin(20^\circ) + (1.22668 \, T_A) \sin(40^\circ) = 350TA​sin(20∘)+(1.22668TA​)sin(40∘)=350
    TA(0.34202+1.22668×0.64279)=350T_A (0.34202 + 1.22668 \times 0.64279) = 350TA​(0.34202+1.22668×0.64279)=350
    TA(0.34202+0.78849)=350T_A (0.34202 + 0.78849) = 350TA​(0.34202+0.78849)=350
    1.13051 TA=350  ⟹  TA≈309.59 N1.13051 \, T_A = 350 \implies T_A \approx 309.59\text{ N}1.13051TA​=350⟹TA​≈309.59 N
  5. Solve for TBT_BTB​:
    TB≈1.22668×309.5935≈379.77 NT_B \approx 1.22668 \times 309.5935 \approx 379.77\text{ N}TB​≈1.22668×309.5935≈379.77 N

Show your steps and calculations here.

Regroup 3

  • Review standard free-body diagrams and drawing force vectors head-to-tail.
  • Emphasize component-wise decoupling in static equilibrium equations.

Synthesis Wrap-up

  • Core takeaways from Session 02 and overview of homework assignment: Vectors in the Plane Vectors in Three Dimensions.