Coordinate Geometry, Quadrilateral Properties, and Conservation of Momentum

Coordinate Geometry: Polygon Area and Perimeter

  • Bounding Box Subtraction Method for Area:

    • To calculate the area of an irregular polygon plotted on a Cartesian coordinate plane, construct an enclosing bounding rectangle whose edges align with the maximum horizontal and vertical coordinates of the figure, then subtract the surplus exterior geometric shapes (triangles and rectangles).

    • Enclosing Bounding Rectangle Dimensions:

    • Length (LL) = 1111

    • Width (WW) = 1010

    • Total Area of Bounding Box (AtotalA_{\text{total}}) = L×W=11×10=110L \times W = 11 \times 10 = 110

    • Surrounding Boundary Regions Subtracted:

    • Region I (Right Triangle): AI=B×H2=4×72=14A_I = \frac{B \times H}{2} = \frac{4 \times 7}{2} = 14

    • Region II (Right Triangle): AII=B×H2=6×22=6A_{II} = \frac{B \times H}{2} = \frac{6 \times 2}{2} = 6

    • Region III (Right Triangle): AIII=B×H2=5×12=2.5A_{III} = \frac{B \times H}{2} = \frac{5 \times 1}{2} = 2.5

    • Region IV / VI (Right Triangle): AVI=B×H2=7×12=3.5A_{VI} = \frac{B \times H}{2} = \frac{7 \times 1}{2} = 3.5

    • Region V / VII (Right Triangle / Small Rectangle): AV=B×H2=2×22=2A_V = \frac{B \times H}{2} = \frac{2 \times 2}{2} = 2

    • Total Polygon Area Calculation:

    • A=Atotal−AI−AII−AIII−AVI−AVA = A_{\text{total}} - A_I - A_{II} - A_{III} - A_{VI} - A_V

    • A=110−14−6−2.5−3.5−2=82A = 110 - 14 - 6 - 2.5 - 3.5 - 2 = 82

  • Perimeter Calculation via Euclidean Distance Formula:

    • The perimeter of a polygon is the sum of the lengths of all bounding line segments. For each segment between coordinates (x1,y1)(x_1, y_1) and (x2,y2)(x_2, y_2), length is given by d=(Δx)2+(Δy)2d = \sqrt{(\Delta x)^2 + (\Delta y)^2}.

    • Individual Side Lengths:

    • Side 1: d1=62+32=36+9=45≈6.708d_1 = \sqrt{6^2 + 3^2} = \sqrt{36 + 9} = \sqrt{45} \approx 6.708

    • Side 2: d2=72+42=49+16=65≈8.062d_2 = \sqrt{7^2 + 4^2} = \sqrt{49 + 16} = \sqrt{65} \approx 8.062

    • Side 3: d3=62+22=36+4=40≈6.325d_3 = \sqrt{6^2 + 2^2} = \sqrt{36 + 4} = \sqrt{40} \approx 6.325

    • Side 4: d4=72+12=49+1=50≈7.071d_4 = \sqrt{7^2 + 1^2} = \sqrt{49 + 1} = \sqrt{50} \approx 7.071

    • Side 5: d5=52+12=25+1=26≈5.099d_5 = \sqrt{5^2 + 1^2} = \sqrt{25 + 1} = \sqrt{26} \approx 5.099

    • Total Perimeter Calculation:

    • Perimeter=45+65+40+50+26\text{Perimeter} = \sqrt{45} + \sqrt{65} + \sqrt{40} + \sqrt{50} + \sqrt{26}

    • Perimeter≈6.708+8.062+6.325+7.071+5.099=33.265\text{Perimeter} \approx 6.708 + 8.062 + 6.325 + 7.071 + 5.099 = 33.265

    • Rounded to the nearest hundredth: 33.2733.27

Polygon plotted on Cartesian coordinate grid with surrounding bounding box decomposition

Foundations of Euclidean Geometry: Lines, Angles, and Transformations

  • Transversal and Parallel Line Angle Relationships:

    • When two parallel lines are intersected by a transversal line:

    • Alternate interior angles are congruent: ∠alt int 1≅∠alt int 2\angle_{\text{alt int 1}} \cong \angle_{\text{alt int 2}}

    • Corresponding angles are congruent: ∠corr 1≅∠corr 2\angle_{\text{corr 1}} \cong \angle_{\text{corr 2}}

    • Consecutive interior angles are supplementary: m∠1+m∠2=180∘m\angle_1 + m\angle_2 = 180^\circ

    • Vertical angles are congruent across intersecting lines: x=116∘x = 116^\circ, y=116∘y = 116^\circ

  • Triangle Angle Sum and Exterior Angle Theorems:

    • The interior angles of any triangle in Euclidean space sum to 180∘180^\circ:

    • Equation: (4x+4)+79+65=180(4x + 4) + 79 + 65 = 180

    • Combine constants: 4x+148=1804x + 148 = 180

    • Subtract 148148: 4x=324x = 32

    • Solve for xx: x=8x = 8

    • Exterior Angle Theorem:

    • The measure of an exterior angle of a triangle equals the sum of the measures of its two remote interior angles:

    • Equation: 144=4x144 = 4x

    • Solve for xx: x=36x = 36

    • Algebraic Angle Systems:

    • Interior angle system: (3x−7)+(7x−8)+(2x−9)=180(3x - 7) + (7x - 8) + (2x - 9) = 180

    • Combine like terms: 12x−24=18012x - 24 = 180

    • Add 2424: 12x=20412x = 204

    • Solve for xx: x=17x = 17

  • The Triangle Inequality Theorem:

    • For any triangle with side lengths aa, bb, and cc, the sum of the lengths of any two sides must be strictly greater than the length of the remaining side (a+b>ca + b > c):

    • Candidate set {18,22,34}\{18, 22, 34\}: 18+22=40>3418 + 22 = 40 > 34 (Valid triangle)

    • Candidate set {8,22,30}\{8, 22, 30\}: 8+22=30≯308 + 22 = 30 \ngtr 30 (Invalid triangle)

  • Candidate set {7,12,20}\{7, 12, 20\}: 7+12=19≯207 + 12 = 19 \ngtr 20 (Invalid triangle)

  • Candidate set {6,9,15}\{6, 9, 15\}: 6+9=15≯156 + 9 = 15 \ngtr 15 (Invalid triangle)

  • Regular Polygons:

    • The sum of the exterior angles of any convex polygon is 360∘360^\circ.

    • Each exterior angle of an nn-sided regular polygon is given by E=360∘nE = \frac{360^\circ}{n}.

    • For a regular pentagon (n=5n = 5):

    • Exterior angle: E=360∘5=72∘E = \frac{360^\circ}{5} = 72^\circ

    • Interior angle: I=180∘−72∘=108∘I = 180^\circ - 72^\circ = 108^\circ

  • Geometric Transformations:

    • Translations:

    • A translation shifts every point of a geometric figure by the same displacement distance in a specified direction: (x,y)→(x+h,y+k)(x, y) \rightarrow (x + h, y + k).

    • Rotations:

    • A clockwise rotation of 90∘90^\circ about the origin follows the coordinate transformation mapping rule:

    • (x,y)→(y,−x)(x, y) \rightarrow (y, -x)

    • Composition of Transformations:

    • Applying sequential transformation mappings to coordinate pairs:

    • (1,7)→(7,0)→(6,10)(1, 7) \rightarrow (7, 0) \rightarrow (6, 10)

  • Coordinate Formulas: Midpoints, Distance, and Slopes:

    • Midpoint Formula:

    • The midpoint MM of a directed line segment connecting (x1,y1)(x_1, y_1) and (x2,y2)(x_2, y_2) is:

    • M=(x1+x22,y1+y22)M = \left(\frac{x_1 + x_2}{2}, \frac{y_1 + y_2}{2}\right)

    • Worked evaluation: for points (−1,5)(-1, 5) and (5,−11)(5, -11), M=(−1+52,5+(−11)2)=(2,−3)M = \left(\frac{-1 + 5}{2}, \frac{5 + (-11)}{2}\right) = (2, -3).

    • Determining an Endpoint from a Given Endpoint and Midpoint:

    • Let known endpoint be A(−8,5)A(-8, 5) and midpoint be M(−2,−3)M(-2, -3), solve for unknown endpoint B(x2,y2)B(x_2, y_2).

    • Horizontal: −8+x22=−2→−8+x2=−4→x2=4\frac{-8 + x_2}{2} = -2 \rightarrow -8 + x_2 = -4 \rightarrow x_2 = 4

    • Vertical: 5+y22=−3→5+y2=−6→y2=−11\frac{5 + y_2}{2} = -3 \rightarrow 5 + y_2 = -6 \rightarrow y_2 = -11

    • Unknown endpoint coordinates: B(4,−11)B(4, -11)

    • Slope Formula:

    • m=ΔyΔx=y2−y1x2−x1m = \frac{\Delta y}{\Delta x} = \frac{y_2 - y_1}{x_2 - x_1}

    • For points (9,5)(9, 5) and (21,−5)(21, -5): m=−5−521−9=−1012=−56m = \frac{-5 - 5}{21 - 9} = \frac{-10}{12} = -\frac{5}{6}

  • Equations of Lines and Perpendicular Bisectors:

    • Slope-Intercept Form: y=mx+by = mx + b

    • Point-Slope Form: y−y1=m(x−x1)y - y_1 = m(x - x_1)

    • For a line with slope m=−12m = -\frac{1}{2} passing through (11,1)(11, 1): y−1=−12(x−11)y - 1 = -\frac{1}{2}(x - 11)

    • For a line passing through (−6,−1)(-6, -1) with slope m=32m = \frac{3}{2}: y+1=32(x+6)y + 1 = \frac{3}{2}(x + 6)

    • Parallel and Perpendicular Lines:

    • Parallel lines have identical slopes: m∥=m1m_{\parallel} = m_1

    • Perpendicular lines have negative reciprocal slopes: m⊥=−1m1m_{\perp} = -\frac{1}{m_1}

    • Example: Line 3x−y=0→y=3x3x - y = 0 \rightarrow y = 3x. Parallel slope is 33; perpendicular slope is −13-\frac{1}{3}.

    • Equation of a Perpendicular Bisector:

    • 1. Calculate midpoint of segment: M=(x1+x22,y1+y22)=(−4,−1)M = \left(\frac{x_1 + x_2}{2}, \frac{y_1 + y_2}{2}\right) = (-4, -1)

    • 2. Calculate slope of original segment: m=ΔyΔx=6−(−4)−9−1=10−10=−1m = \frac{\Delta y}{\Delta x} = \frac{6 - (-4)}{-9 - 1} = \frac{10}{-10} = -1

    • 3. Determine perpendicular slope: m⊥=−(1−1)=1m_{\perp} = -\left(\frac{1}{-1}\right) = 1

    • 4. Construct point-slope equation: y+1=1(x+4)y + 1 = 1(x + 4)

Quadrilateral Properties: Parallelograms

  • Fundamental Properties of Parallelograms:

    • A parallelogram is a quadrilateral with both pairs of opposite sides parallel (AB∥CDAB \parallel CD and BC∥DABC \parallel DA).

    • Opposite sides are congruent (AB≅CDAB \cong CD and BC≅DABC \cong DA).

    • Opposite angles are congruent (∠A≅∠C\angle A \cong \angle C and ∠B≅∠D\angle B \cong \angle D).

    • Consecutive angles are supplementary (m∠A+m∠B=180∘m\angle A + m\angle B = 180^\circ, m∠B+m∠C=180∘m\angle B + m\angle C = 180^\circ, etc.).

    • Diagonals bisect each other.

  • Algebraic Applications to Parallelogram Sides and Slopes:

    • Parallel Slopes Property:

    • In parallelogram LMNOLMNO, if the slope of side LOLO is −13-\frac{1}{3}, the slope of opposite side MNMN is −13-\frac{1}{3}, because opposite sides are parallel.

    • Congruent Opposite Sides Property:

    • In quadrilateral LMNOLMNO, where ON=7x−5ON = 7x - 5, LM=6x+4LM = 6x + 4, and NM=x+6NM = x + 6:

    • Set opposite sides equal: 7x−5=6x+47x - 5 = 6x + 4

    • Subtract 6x6x: x−5=4x - 5 = 4

    • Add 55: x=9x = 9

  • Algebraic Applications to Parallelogram Angles:

    • Consecutive Supplementary Angles:

    • In parallelogram ABCDABCD, where m∠A=2x+10m\angle A = 2x + 10 and m∠B=3xm\angle B = 3x:

    • Set sum equal to 180∘180^\circ: (2x+10)+3x=180(2x + 10) + 3x = 180

    • Combine terms: 5x+10=1805x + 10 = 180

    • Subtract 1010: 5x=1705x = 170

    • Solve for xx: x=34x = 34

    • Evaluate angle measure: m∠B=3(34)=102circm\angle B = 3(34) = 102^circ

    • Congruent Opposite Angles:

    • In parallelogram ABCDABCD, where m∠A=3x+10m\angle A = 3x + 10 and m∠C=100∘m\angle C = 100^\circ:

    • Set opposite angles equal: 3x+10=1003x + 10 = 100

    • Subtract 1010: 3x=903x = 90

    • Solve for xx: x=30x = 30

  • Parallelogram Diagonals Bisecting Each Other:

    • In parallelogram ABCDABCD, diagonals ACAC and DBDB intersect at point EE. Segments along diagonal ACAC are given as AE=3x−4AE = 3x - 4 and EC=x+12EC = x + 12:

    • Set segments equal: 3x−4=x+123x - 4 = x + 12

    • Subtract xx: 2x−4=122x - 4 = 12

    • Add 44: 2x=162x = 16

    • Solve for xx: x=8x = 8

  • Comprehensive Parallelogram Geometry Problems:

    • Problem 1 (Parallelogram FRED):

    • Side EDED is extended to point AA, segment AFAF is drawn such that AF≅DFAF \cong DF, and m∠R=124∘m\angle R = 124^\circ.

    • Opposite angles are congruent: m∠D=m∠R=124∘m\angle D = m\angle R = 124^\circ (within the parallelogram interior).

    • Line segment ADEADE forms a linear pair: m∠ADF=180∘−124∘=56∘m\angle ADF = 180^\circ - 124^\circ = 56^\circ.

    • Since triangle △AFD\triangle AFD is isosceles with AF≅DFAF \cong DF, base angles are congruent: m∠FAD=m∠ADF=56∘m\angle FAD = m\angle ADF = 56^\circ.

    • Calculate vertex angle: m∠AFD=180∘−(56∘+56∘)=180∘−112∘=68∘m\angle AFD = 180^\circ - (56^\circ + 56^\circ) = 180^\circ - 112^\circ = 68^\circ.

    • Problem 2 (Parallelogram QRST):

    • Diagonal TRTR is drawn, points UU and VV lie on segments TSTS and QRQR respectively, and line segment UVUV intersects TRTR at point WW.

    • Given: m∠S=60∘m\angle S = 60^\circ, m∠SRT=83∘m\angle SRT = 83^\circ, and m∠TWU=35∘m\angle TWU = 35^\circ.

    • In triangle △RST\triangle RST, sum of interior angles is 180∘180^\circ:

      • m∠STR=180∘−(60∘+83∘)=180∘−143∘=37∘m\angle STR = 180^\circ - (60^\circ + 83^\circ) = 180^\circ - 143^\circ = 37^\circ

    • Since TS∥QRTS \parallel QR, alternate interior angles are congruent: m∠QRT=m∠STR=37∘m\angle QRT = m\angle STR = 37^\circ.

    • In triangle △TWU\triangle TWU, interior angle sum yields:

      • m∠TUW=180∘−(35∘+37∘)=180∘−72∘=108∘m\angle TUW = 180^\circ - (35^\circ + 37^\circ) = 180^\circ - 72^\circ = 108^\circ

    • By angle relationships across transversals and intersecting lines: m∠WVQ=72∘m\angle WVQ = 72^\circ.

    • Problem 3 (Parallelogram ABCD with Exterior Extension):

    • Side ABAB is extended through BB to point EE, and segment CECE is drawn such that CE≅BECE \cong BE. Given m∠D=112∘m\angle D = 112^\circ.

    • In parallelogram ABCDABCD, opposite angles are congruent (m∠B=112∘m\angle B = 112^\circ) and consecutive angles are supplementary (m∠A=180∘−112∘=68∘m\angle A = 180^\circ - 112^\circ = 68^\circ).

    • At vertex BB, the exterior angle to the line extension forms a linear pair: m∠CBE=180∘−112∘=68∘m\angle CBE = 180^\circ - 112^\circ = 68^\circ.

    • In triangle △CBE\triangle CBE, since CE≅BECE \cong BE, base angles are equal: m∠BCE=m∠CBE=68∘m\angle BCE = m\angle CBE = 68^\circ.

    • Interior angle sum of △CBE\triangle CBE: m∠E=180∘−(68∘+68∘)=180∘−136∘=44∘m\angle E = 180^\circ - (68^\circ + 68^\circ) = 180^\circ - 136^\circ = 44^\circ.

    • Problem 4 (Parallelogram ROCK):

    • Given m∠C=70∘m\angle C = 70^\circ and m∠ROS=65∘m\angle ROS = 65^\circ.

    • Consecutive angles are supplementary: m∠R=180∘−70∘=110∘m\angle R = 180^\circ - 70^\circ = 110^\circ.

    • In triangle △ROS\triangle ROS, angle sum yields: m∠RSO=180∘−(110∘+65∘)=180∘−175∘=5∘m\angle RSO = 180^\circ - (110^\circ + 65^\circ) = 180^\circ - 175^\circ = 5^\circ.

    • Triangle and line calculations at transversal intersection give: m∠KSO=135∘m\angle KSO = 135^\circ.

    • Problem 5 (Parallelogram LMNO with Diagonal LN):

    • Diagonal LNLN is drawn, m∠M=118∘m\angle M = 118^\circ, and m∠LNO=22∘m\angle LNO = 22^\circ.

    • Explanation for why m∠NLO=40∘m\angle NLO = 40^\circ:

      • Opposite angles of a parallelogram are congruent, so m∠O=m∠M=118∘m\angle O = m\angle M = 118^\circ.

      • In triangle △LNO\triangle LNO, the sum of interior angles is 180∘180^\circ: m∠NLO=180∘−(m∠O+m∠LNO)=180∘−(118∘+22∘)=180∘−140∘=40∘m\angle NLO = 180^\circ - (m\angle O + m\angle LNO) = 180^\circ - (118^\circ + 22^\circ) = 180^\circ - 140^\circ = 40^\circ.

      • Alternatively, consecutive angles are supplementary: m∠OLN+m∠MLN=180∘−118∘=62∘m\angle OLN + m\angle MLN = 180^\circ - 118^\circ = 62^\circ. By alternate interior angles, m∠MLN=m∠LNO=22∘m\angle MLN = m\angle LNO = 22^\circ, hence m∠NLO=62∘−22∘=40∘m\angle NLO = 62^\circ - 22^\circ = 40^\circ.

    • Problem 6 (Parallelogram ABCD Diagonals):

    • Diagonals ACAC and BDBD intersect. Given m∠1=45∘m\angle 1 = 45^\circ and m∠DCB=120∘m\angle DCB = 120^\circ.

    • By angle relationships and triangle decompositions: m∠2=180∘−120∘−45∘=15∘m\angle 2 = 180^\circ - 120^\circ - 45^\circ = 15^\circ.

Quadrilateral Properties: Trapezoids and Isosceles Trapezoids

  • Trapezoid Definition and Baseline Properties:

    • A trapezoid is a quadrilateral possessing exactly one pair of parallel sides (called bases).

    • The non-parallel sides are called legs.

    • Upper and lower base angles along each transversal leg are supplementary (m∠upper+m∠lower=180∘m\angle_{\text{upper}} + m\angle_{\text{lower}} = 180^\circ).

    • An altitude of a trapezoid is a perpendicular line segment dropped from one base to the opposite base.

  • Median (Midsegment) of a Trapezoid Theorem:

    • The median connects the midpoints of the two legs, is parallel to both bases, and its length equals the arithmetic average of the lengths of the two bases:

    • Median=Base1+Base22\text{Median} = \frac{\text{Base}_1 + \text{Base}_2}{2}

    • Problem 1 (Base Angle Evaluation):

    • In trapezoid ABCDABCD with bases ABAB and CDCD, if m∠B=123∘m\angle B = 123^\circ:

    • m∠C=180∘−123∘=57∘m\angle C = 180^\circ - 123^\circ = 57^\circ

    • Problem 2 (Base Length Evaluation):

    • In trapezoid RSTURSTU, RS∥TURS \parallel TU, XX is the midpoint of leg RURU, and VV is the midpoint of leg STST. Given base RS=30RS = 30 and median XV=44XV = 44:

    • 30+TU2=44\frac{30 + TU}{2} = 44

    • Multiply by 22: 30+TU=8830 + TU = 88

    • Subtract 3030: TU=58TU = 58

    • Problem 3 (Algebraic Midsegment Formulation):

    • In trapezoid ABCDABCD, median EF=2x+2EF = 2x + 2, base AB=5x−9AB = 5x - 9, and base DC=x+3DC = x + 3:

    • (x+3)+(5x−9)2=2x+2\frac{(x + 3) + (5x - 9)}{2} = 2x + 2

    • Simplify numerator: 6x−62=2x+2\frac{6x - 6}{2} = 2x + 2

    • Divide: 3x−3=2x+23x - 3 = 2x + 2

    • Subtract 2x2x and add 33: x=5x = 5

  • Isosceles Trapezoids:

    • Condition of Classification: Never assume a trapezoid is isosceles unless explicitly given or proven.

    • An isosceles trapezoid satisfies all baseline properties of a general trapezoid, plus:

    • Non-parallel legs are congruent (Leg1≅Leg2\text{Leg}_1 \cong \text{Leg}_2).

    • Diagonals are congruent (d1≅d2d_1 \cong d_2).

    • Both pairs of base angles are congruent (lower base angles congruent, upper base angles congruent).

    • Opposite angles are supplementary (m∠opp 1+m∠opp 2=180∘m\angle_{\text{opp 1}} + m\angle_{\text{opp 2}} = 180^\circ).

    • Problem 4 (Congruent Legs):

    • In isosceles trapezoid DEFGDEFG, DE∥GFDE \parallel GF, leg DG=10x−7DG = 10x - 7, and leg EF=3+5xEF = 3 + 5x:

    • Set legs equal: 10x−7=3+5x10x - 7 = 3 + 5x

    • Subtract 5x5x: 5x−7=35x - 7 = 3

    • Add 77: 5x=105x = 10

    • Solve for xx: x=2x = 2

    • Problem 5 (Congruent Diagonals):

    • In isosceles trapezoid ABCDABCD, diagonals are AC=5x+13AC = 5x + 13 and BD=11x−5BD = 11x - 5:

    • Set diagonals equal: 5x+13=11x−55x + 13 = 11x - 5

    • Subtract 5x5x: 13=6x−513 = 6x - 5

    • Add 55: 18=6x18 = 6x

    • Solve for xx: x=3x = 3

    • Problem 6 (Congruent Base Angles):

    • In isosceles trapezoid QRSTQRST, bases are QRQR and TSTS. Given lower base angles m∠Q=5x+3m\angle Q = 5x + 3 and m∠R=7x−15m\angle R = 7x - 15:

    • Set angles equal: 5x+3=7x−155x + 3 = 7x - 15

    • Subtract 5x5x: 3=2x−153 = 2x - 15

    • Add 1515: 18=2x18 = 2x

    • Solve for xx: x=9x = 9

    • Evaluate m∠Qm\angle Q: m∠Q=5(9)+3=45+3=48∘m\angle Q = 5(9) + 3 = 45 + 3 = 48^\circ

    • Problem 7 (Supplementary Opposite Angles):

    • In trapezoid ABCDABCD, AB∥DCAB \parallel DC, AD≅BCAD \cong BC, m∠A=4x+20m\angle A = 4x + 20, and m∠C=3x−15m\angle C = 3x - 15:

    • Set sum equal to 180∘180^\circ: (4x+20)+(3x−15)=180(4x + 20) + (3x - 15) = 180

    • Combine terms: 7x+5=1807x + 5 = 180

    • Subtract 55: 7x=1757x = 175

    • Solve for xx: x=25x = 25

    • Evaluate m∠Dm\angle D: Since base angles are congruent, m∠D=m∠C=3(25)−15=75−15=60∘m\angle D = m\angle C = 3(25) - 15 = 75 - 15 = 60^\circ

  • Right Trapezoids:

    • A right trapezoid satisfies all general trapezoid properties plus the addition of exactly two adjacent right angles (90∘90^\circ).

Trapezoid family tree diagram illustrating hierarchy from general trapezoid to isosceles and right trapezoids
  • Trapezoid Altitude and Area Practice Problems:

    • Quadrilateral Diagonal Non-Bisection:

    • If the diagonals of a quadrilateral do not bisect each other, the figure cannot be a parallelogram, rectangle, rhombus, or square; it could be a trapezoid.

    • Equal Area Triangles in a Trapezoid:

    • In trapezoid RSTVRSTV with bases RSRS and VTVT, diagonals RTRT and SVSV intersect at point QQ.

    • Triangles △RSV\triangle RSV and △RST\triangle RST share the identical base RSRS and share identical perpendicular heights between the parallel bases; thus, Area(△RSV)=Area(△RST)\text{Area}(\triangle RSV) = \text{Area}(\triangle RST).

    • Subtracting shared area △RSQ\triangle RSQ yields equal areas for non-overlapping lateral triangles: Area(△RQV)=Area(△SQT)\text{Area}(\triangle RQV) = \text{Area}(\triangle SQT).

    • Altitude Calculation 1 (Trapezoid LATE):

    • Isosceles trapezoid LATELATE has bases LA=24LA = 24 and ET=40ET = 40, with leg AT=10AT = 10. Altitudes LFLF and AGAG are dropped to base ETET.

    • Horizontal projection on base: d=ET−LA2=40−242=162=8d = \frac{ET - LA}{2} = \frac{40 - 24}{2} = \frac{16}{2} = 8

    • Apply Pythagorean theorem to right triangle △AGT\triangle AGT: x2+82=102x^2 + 8^2 = 10^2

    • x2+64=100→x2=36→x=6x^2 + 64 = 100 \rightarrow x^2 = 36 \rightarrow x = 6

    • Length of altitude LF=6LF = 6

    • Altitude Calculation 2 (Trapezoid ABCD):

    • Isosceles trapezoid ABCDABCD has legs AB=CD=25AB = CD = 25, base BC=12BC = 12, and base AD=26AD = 26.

    • Horizontal projection on base: d=AD−BC2=26−122=142=7d = \frac{AD - BC}{2} = \frac{26 - 12}{2} = \frac{14}{2} = 7

    • Apply Pythagorean theorem: x2+72=252x^2 + 7^2 = 25^2

    • x2+49=625→x2=576→x=24x^2 + 49 = 625 \rightarrow x^2 = 576 \rightarrow x = 24

    • Length of altitude = 2424

    • Altitude Calculation 3 (Trapezoid ABCD):

    • Isosceles trapezoid ABCDABCD has legs AB=CD=17AB = CD = 17, base BC=20BC = 20, and base AD=36AD = 36.

    • Horizontal projection on base: d=AD−BC2=36−202=162=8d = \frac{AD - BC}{2} = \frac{36 - 20}{2} = \frac{16}{2} = 8

    • Apply Pythagorean theorem: x2+82=172x^2 + 8^2 = 17^2

    • x2+64=289→x2=225→x=15x^2 + 64 = 289 \rightarrow x^2 = 225 \rightarrow x = 15

    • Length of altitude = 1515

Quadrilateral Properties: Rhombuses and Squares

  • Properties of a Rhombus:

    • A rhombus is a parallelogram with four congruent sides.

    • Diagonals are perpendicular (AC⊥BDAC \perp BD).

    • Diagonals bisect the interior angles.

    • All general parallelogram properties apply (opposite angles congruent, consecutive angles supplementary, diagonals bisect each other).

  • Rhombus Problem Applications:

    • Problem 1 (Equilateral Sides and Perimeter):

    • In rhombus ABCDABCD, side AB=3x+2AB = 3x + 2 and side BC=x+12BC = x + 12:

    • Set sides equal: 3x+2=x+123x + 2 = x + 12

    • Subtract xx: 2x+2=122x + 2 = 12

    • Subtract 22: 2x=102x = 10

    • Solve for xx: x=5x = 5

    • Side length: s=3(5)+2=17s = 3(5) + 2 = 17

    • Total perimeter: P=4×s=4×17=68P = 4 \times s = 4 \times 17 = 68

    • Problem 2 (Diagonals Bisecting Angles):

    • In rhombus ABCDABCD, m∠C=100∘m\angle C = 100^\circ. Find m∠BDAm\angle BDA:

    • Consecutive angles are supplementary: m∠ADC=180∘−100∘=80∘m\angle ADC = 180^\circ - 100^\circ = 80^\circ

    • Diagonal BDBD bisects ∠ADC\angle ADC: m∠BDA=80∘2=40∘m\angle BDA = \frac{80^\circ}{2} = 40^\circ

    • Problem 3 (Perpendicular Diagonals and Pythagorean Theorem):

    • In rhombus ABCDABCD, diagonals ACAC and BDBD intersect perpendicularly at EE. Given half-diagonals AE=5AE = 5 and BE=12BE = 12. Find side length ABAB:

    • Apply Pythagorean theorem: AE2+BE2=AB2AE^2 + BE^2 = AB^2

    • 52+122=c2→25+144=c2→169=c2→c=135^2 + 12^2 = c^2 \rightarrow 25 + 144 = c^2 \rightarrow 169 = c^2 \rightarrow c = 13

    • Side length AB=13AB = 13

    • Problem 4 (Perimeter from Full Diagonals):

    • In rhombus PQRSPQRS, diagonals intersect at TT with full lengths PR=16PR = 16 and QS=30QS = 30.

    • Determine half-diagonal lengths: a=162=8a = \frac{16}{2} = 8, b=302=15b = \frac{30}{2} = 15

    • Calculate side length (ss): s=82+152=64+225=289=17s = \sqrt{8^2 + 15^2} = \sqrt{64 + 225} = \sqrt{289} = 17

    • Total perimeter: P=4×s=4×17=68P = 4 \times s = 4 \times 17 = 68

  • Properties of a Square:

    • A square is a regular quadrilateral that simultaneously satisfies all properties of a rectangle, a rhombus, and a parallelogram.

    • Four congruent sides.

    • Four congruent right angles (90∘90^\circ).

    • Diagonals are congruent, perpendicular bisectors of each other, and bisect interior angles at 45∘45^\circ.

  • Square Problem Applications:

    • Problem 1 (Diagonal Bisector Equivalence):

    • In square ABCDABCD, diagonals intersect at EE. Given segments DE=7y−10DE = 7y - 10 and CE=5y+10CE = 5y + 10:

    • Since diagonals of a square are congruent and bisect each other, half-diagonals are equal: 7y−10=5y+107y - 10 = 5y + 10

    • Subtract 5y5y: 2y−10=102y - 10 = 10

    • Add 1010: 2y=202y = 20

    • Solve for yy: y=10y = 10

    • Problem 2 (Diagonal Length from Known Side):

    • If side length s=4s = 4, find diagonal dd in simplest radical form:

    • Using Pythagorean theorem (s2+s2=d2s^2 + s^2 = d^2):

    • 42+42=d2→16+16=d2→d2=324^2 + 4^2 = d^2 \rightarrow 16 + 16 = d^2 \rightarrow d^2 = 32

    • d=32=16×2=42d = \sqrt{32} = \sqrt{16 \times 2} = 4\sqrt{2}

    • Problem 3 (Diagonal Length from Perimeter):

    • A square has a perimeter of 2828. Determine its diagonal in simplest radical form:

    • Calculate side length: s=284=7s = \frac{28}{4} = 7

    • Apply Pythagorean theorem: 72+72=d27^2 + 7^2 = d^2

    • 49+49=d2→d2=9849 + 49 = d^2 \rightarrow d^2 = 98

    • d=98=49×2=72d = \sqrt{98} = \sqrt{49 \times 2} = 7\sqrt{2}

    • Problem 4 (Side Length Expression from Polynomial Perimeter):

    • A square has a perimeter of 16x4+416x^4 + 4. Write an expression representing each side:

    • Since a square has four congruent sides, divide the total perimeter by 44:

    • Side=16x4+44=4x4+1\text{Side} = \frac{16x^4 + 4}{4} = 4x^4 + 1

Classical Mechanics: Principles of Momentum and Impulse

  • Core Definitions and Vector Formulations:

    • System:

    • A system is defined as the specific object or collection of interacting objects chosen for physical analysis.

    • Linear Momentum (pp):

    • Momentum is a vector quantity defined as the product of an object's mass (mm) and its velocity (vv):

    • p=mvp = mv

    • Standard SI unit: kg m/skg\,m/s

    • Sign Conventions:

    • Motion directed rightward or eastward is defined as positive (++).

    • Motion directed leftward or westward is defined as negative (−-).

    • Scalar Invariance of Mass:

    • Mass is an intrinsic scalar physical quantity and must strictly be positive (m>0m > 0).

    • A negative sign in momentum indicates vector direction (negative velocity), never negative mass.

  • The Law of Conservation of Momentum:

    • The total linear momentum of an isolated system remains constant over time unless acted upon by a net external force:

    • pbefore=pafterp_{\text{before}} = p_{\text{after}}

    • ∑pi=∑pf\sum p_i = \sum p_f

    • A net external force is the only mechanism that can change a system's total velocity and momentum (e.g., friction acting on a vehicle).

    • In any internal two-body interaction or collision, the momentum gained by one object is identical in magnitude and opposite in sign to the momentum lost by the second object:

    • Δp1=−Δp2\Delta p_1 = -\Delta p_2

  • Impulse (JJ) and Force-Time Integrals:

    • Impulse is defined as the product of the average net force acting on an object and the time duration (Δt\Delta t) over which it acts, which equals the object's change in linear momentum:

    • J=Δp=FnetΔtJ = \Delta p = F_{\text{net}} \Delta t

    • Standard SI units: N sN\,s or kg m/skg\,m/s

    • Graphical Impulse Determination:

    • The magnitude of impulse equals the geometric area beneath a force-time graph (F vs. tF \text{ vs. } t).

    • For a triangular force pulse rising from zero to peak force FpeakF_{\text{peak}} and returning to zero over duration Δt\Delta t:

    • J=12×Δt×FpeakJ = \frac{1}{2} \times \Delta t \times F_{\text{peak}}

Force magnitude versus time profile comparing rigid and flexible bumper impacts
  • Classification of Collision Typologies:

    • Elastic Collision:

    • Total linear momentum is conserved: pi=pfp_i = p_f

    • Total kinetic energy (KE=12mv2KE = \frac{1}{2}mv^2) is strictly conserved: KEi=KEfKE_i = KE_f

    • Inelastic Collision:

    • Total linear momentum is conserved: pi=pfp_i = p_f

    • Total kinetic energy is not conserved (KEf<KEiKE_f < KE_i); mechanical energy dissipates into internal thermal energy, acoustic energy, or structural deformation.

    • Perfectly Inelastic Collision:

    • Total linear momentum is conserved: pi=pfp_i = p_f

    • Colliding objects lock together upon impact and move with a unified, common final velocity (vfv_f).

    • This collision class exhibits the maximum possible kinetic energy loss consistent with conservation of momentum.

    • Explosions / Push-Aparts:

    • Internal stored energy (e.g., spring potential or chemical potential) converts into kinetic energy, propelling initially united or adjacent resting bodies into opposing directions while keeping total system momentum constant.

Collision Dynamics and Energy Classification

  • The Kinetic Sculpture Experiment (Two 3.0 kg3.0\,kg Steel Spheres):

    • Setup: Two identical 3.0 kg3.0\,kg spheres on a straight, horizontal track inside an enclosure with negligible external impulse.

    • Initial Conditions across all tests:

    • Sphere A: mA=3.0 kgm_A = 3.0\,kg, vAi=+2.0 m/sv_{Ai} = +2.0\,m/s

    • Sphere B: mB=3.0 kgm_B = 3.0\,kg, vBi=0 m/sv_{Bi} = 0\,m/s

    • Total initial system momentum:

      • pi=mAvAi+mBvBi=(3.0 kg)(+2.0 m/s)+(3.0 kg)(0 m/s)=+6.0 kg m/sp_i = m_A v_{Ai} + m_B v_{Bi} = (3.0\,kg)(+2.0\,m/s) + (3.0\,kg)(0\,m/s) = +6.0\,kg\,m/s

    • Total initial system kinetic energy:

      • KEi=12mAvAi2+12mBvBi2=12(3.0)(2.0)2+0=6.0 JKE_i = \frac{1}{2} m_A v_{Ai}^2 + \frac{1}{2} m_B v_{Bi}^2 = \frac{1}{2}(3.0)(2.0)^2 + 0 = 6.0\,J

    • Test A: Polished Steel Contact Surface:

    • Observed motion: Sphere A comes to a complete rest (vAf=0 m/sv_{Af} = 0\,m/s), and Sphere B moves right at vBf=+2.0 m/sv_{Bf} = +2.0\,m/s.

    • Final kinetic energy:

      • KEf=12(3.0 kg)(0 m/s)2+12(3.0 kg)(+2.0 m/s)2=0+6.0=6.0 JKE_f = \frac{1}{2}(3.0\,kg)(0\,m/s)^2 + \frac{1}{2}(3.0\,kg)(+2.0\,m/s)^2 = 0 + 6.0 = 6.0\,J

    • Collision Classification: Elastic (Kinetic energy is fully conserved: KEi=KEf=6.0 JKE_i = KE_f = 6.0\,J).

    • Test B: Soft Polymer Contact Surface:

    • The polymer coating briefly compresses during impact. Sphere A rebounds with a recorded final velocity of vAf=+0.50 m/sv_{Af} = +0.50\,m/s.

    • Determine missing final velocity of Sphere B (vBfv_{Bf}) using conservation of momentum:

      • pbefore=pafterp_{\text{before}} = p_{\text{after}}

      • mAvAi+mBvBi=mAvAf+mBvBfm_A v_{Ai} + m_B v_{Bi} = m_A v_{Af} + m_B v_{Bf}

      • +6.0 kg m/s=(3.0 kg)(+0.50 m/s)+(3.0 kg)(vBf)+6.0\,kg\,m/s = (3.0\,kg)(+0.50\,m/s) + (3.0\,kg)(v_{Bf})

      • 6.0=1.5+3.0vBf6.0 = 1.5 + 3.0 v_{Bf}

      • 4.5=3.0vBf→vBf=+1.5 m/s4.5 = 3.0 v_{Bf} \rightarrow v_{Bf} = +1.5\,m/s

    • Final kinetic energy calculation:

      • KEf=12(3.0)(0.50)2+12(3.0)(1.5)2=12(3.0)(0.25)+12(3.0)(2.25)KE_f = \frac{1}{2}(3.0)(0.50)^2 + \frac{1}{2}(3.0)(1.5)^2 = \frac{1}{2}(3.0)(0.25) + \frac{1}{2}(3.0)(2.25)

      • KEf=0.375 J+3.375 J=3.75 JKE_f = 0.375\,J + 3.375\,J = 3.75\,J

    • Energy loss: ΔKE=6.0 J−3.75 J=2.25 J\Delta KE = 6.0\,J - 3.75\,J = 2.25\,J

    • Collision Classification: Inelastic (Kinetic energy decreased by 2.25 J2.25\,J, and the spheres did not lock together).

    • Test C: Magnetic Connectors:

    • Spheres connect and latch together upon impact, moving as a single combined mass.

    • Determine shared final velocity (vfv_f):

      • pi=(mA+mB)vfp_i = (m_A + m_B) v_f

      • +6.0 kg m/s=(3.0 kg+3.0 kg)vf+6.0\,kg\,m/s = (3.0\,kg + 3.0\,kg) v_f

      • 6.0=6.0vf→vf=+1.0 m/s6.0 = 6.0 v_f \rightarrow v_f = +1.0\,m/s

    • Collision Classification: Perfectly Inelastic.

    • Fundamental Conservation Rationale:

    • Total linear momentum is conserved across all three simulations because the spheres exert internal forces on one another, while the net external impulse on the two-sphere system is negligible.

  • Floating Solar Panels Protective Bumper Experiment:

    • System model: Module A (mA=150 kgm_A = 150\,kg) drifts east at vAi=+1.2 m/sv_{Ai} = +1.2\,m/s. Module B (unknown mass mBm_B) drifts west at vBi=−0.40 m/sv_{Bi} = -0.40\,m/s.

    • Following a flexible bumper collision: Module A moves west at vAf=−0.40 m/sv_{Af} = -0.40\,m/s, and Module B moves east at vBf=+0.56 m/sv_{Bf} = +0.56\,m/s.

    • Derivation of Module B Mass:

    • mAvAi+mBvBi=mAvAf+mBvBfm_A v_{Ai} + m_B v_{Bi} = m_A v_{Af} + m_B v_{Bf}

    • (150)(+1.2)+mB(−0.40)=(150)(−0.40)+mB(+0.56)(150)(+1.2) + m_B(-0.40) = (150)(-0.40) + m_B(+0.56)

    • 180−0.40mB=−60+0.56mB180 - 0.40 m_B = -60 + 0.56 m_B

    • Add 6060 and add 0.40mB0.40 m_B: 240=0.96mB240 = 0.96 m_B

    • Solve for mass: mB=2400.96=250 kgm_B = \frac{240}{0.96} = 250\,kg

    • Module Momentum Inventory:

    • Initial momentum of Module A: pAi=(150 kg)(+1.2 m/s)=+180 kg m/sp_{Ai} = (150\,kg)(+1.2\,m/s) = +180\,kg\,m/s

    • Initial momentum of Module B: pBi=(250 kg)(−0.40 m/s)=−100 kg m/sp_{Bi} = (250\,kg)(-0.40\,m/s) = -100\,kg\,m/s

    • Total initial system momentum: pi=180+(−100)=+80 kg m/sp_i = 180 + (-100) = +80\,kg\,m/s

    • Final momentum of Module A: pAf=(150 kg)(−0.40 m/s)=−60 kg m/sp_{Af} = (150\,kg)(-0.40\,m/s) = -60\,kg\,m/s

    • Final momentum of Module B: pBf=(250 kg)(+0.56 m/s)=+140 kg m/sp_{Bf} = (250\,kg)(+0.56\,m/s) = +140\,kg\,m/s

    • Total final system momentum: pf=−60+140=+80 kg m/sp_f = -60 + 140 = +80\,kg\,m/s

    • Momentum change of Module A: ΔpA=−60−180=−240 kg m/s\Delta p_A = -60 - 180 = -240\,kg\,m/s (decreases by 240 kg m/s240\,kg\,m/s)

    • Momentum change of Module B: ΔpB=140−(−100)=+240 kg m/s\Delta p_B = 140 - (-100) = +240\,kg\,m/s (increases by 240 kg m/s240\,kg\,m/s)

    • Absolute exchange: ΔpA=−ΔpB\Delta p_A = -\Delta p_B

    • Protective Systems Comparison and Energy Dissipation:

    • Initial Total Kinetic Energy: KEi=12(150)(1.2)2+12(250)(−0.40)2=108+20=128 JKE_i = \frac{1}{2}(150)(1.2)^2 + \frac{1}{2}(250)(-0.40)^2 = 108 + 20 = 128\,J

    • Rigid Bumper Test:

      • Final velocities: Module A rebounds at −0.80 m/s-0.80\,m/s, Module B moves at +0.80 m/s+0.80\,m/s.

      • Final KE: KEf=12(150)(−0.80)2+12(250)(0.80)2=48+80=128 JKE_f = \frac{1}{2}(150)(-0.80)^2 + \frac{1}{2}(250)(0.80)^2 = 48 + 80 = 128\,J

      • Classification: Elastic (KEi=KEf=128 JKE_i = KE_f = 128\,J).

    • Flexible Bumper Test:

      • Final velocities: Module A rebounds at −0.40 m/s-0.40\,m/s, Module B moves at +0.56 m/s+0.56\,m/s.

      • Final KE: KEf=12(150)(−0.40)2+12(250)(0.56)2=12+39.2=51.2 JKE_f = \frac{1}{2}(150)(-0.40)^2 + \frac{1}{2}(250)(0.56)^2 = 12 + 39.2 = 51.2\,J

      • Classification: Inelastic (76.8 J76.8\,J converted into deformation and thermal energy).

    • Locking Connector Test:

      • The modules link and move with common velocity vfv_f:

      • pi=(mA+mB)vf→+80 kg m/s=(150 kg+250 kg)vfp_i = (m_A + m_B) v_f \rightarrow +80\,kg\,m/s = (150\,kg + 250\,kg) v_f

      • 80=400vf→vf=+0.2 m/s80 = 400 v_f \rightarrow v_f = +0.2\,m/s

      • Classification: Perfectly Inelastic.

    • Impulse Pulse Structure and Engineering Implications:

    • Rigid Bumper Pulse:

      • Duration: Δt=0.1 s\Delta t = 0.1\,s

      • Peak force: Fpeak=6000 NF_{\text{peak}} = 6000\,N

      • Jrigid=12(0.1 s)(6000 N)=300 N sJ_{\text{rigid}} = \frac{1}{2}(0.1\,s)(6000\,N) = 300\,N\,s

    • Flexible Bumper Pulse:

      • Duration: Δt=0.2 s\Delta t = 0.2\,s

      • Peak force: Fpeak=2400 NF_{\text{peak}} = 2400\,N

      • Jflex=12(0.2 s)(2400 N)=240 N sJ_{\text{flex}} = \frac{1}{2}(0.2\,s)(2400\,N) = 240\,N\,s

    • Engineering Analysis:

      • The impulses differ between the designs because the final velocity changes of Module A differ: ∣ΔvA∣rigid=∣−0.80−1.2∣=2.0 m/s|\Delta v_A|_{\text{rigid}} = |-0.80 - 1.2| = 2.0\,m/s (J=150×2.0=300 N sJ = 150 \times 2.0 = 300\,N\,s), whereas ∣ΔvA∣flex=∣−0.40−1.2∣=1.6 m/s|\Delta v_A|_{\text{flex}} = |-0.40 - 1.2| = 1.6\,m/s (J=150×1.6=240 N sJ = 150 \times 1.6 = 240\,N\,s).

      • The flexible bumper extends impact contact duration (0.2 s0.2\,s vs. 0.1 s0.1\,s), spreading momentum transfer over double the time, thereby reducing peak impact force from 6000 N6000\,N to 2400 N2400\,N (a 60%60\% reduction) to protect platform hardware.

Applied Conservation of Momentum: Problem Archive

  • Laboratory Cart Collision Scenarios:

    • Scenario 1 (Elastic / Disjoint Collision):

    • Cart A (mA=5 kgm_A = 5\,kg) moves east at vAi=5 m/sv_{Ai} = 5\,m/s and collides with Cart B (mB=2.5 kgm_B = 2.5\,kg) at rest (vBi=0 m/sv_{Bi} = 0\,m/s). After collision, Cart A continues east at vAf=1 m/sv_{Af} = 1\,m/s.

    • mAvAi+mBvBi=mAvAf+mBvBfm_A v_{Ai} + m_B v_{Bi} = m_A v_{Af} + m_B v_{Bf}

    • (5)(5)+(2.5)(0)=(5)(1)+(2.5)vBf(5)(5) + (2.5)(0) = (5)(1) + (2.5) v_{Bf}

    • 25=5+2.5vBf→20=2.5vBf→vBf=8 m/s25 = 5 + 2.5 v_{Bf} \rightarrow 20 = 2.5 v_{Bf} \rightarrow v_{Bf} = 8\,m/s

    • Scenario 2 (Carts Sticking Together):

    • Same carts, but they lock together upon impact:

    • (mA+mB)vf=mAvAi+mBvBi(m_A + m_B) v_f = m_A v_{Ai} + m_B v_{Bi}

    • (5+2.5)vf=(5)(5)→7.5vf=25(5 + 2.5) v_f = (5)(5) \rightarrow 7.5 v_f = 25

    • vf=257.5=3.33 m/sv_f = \frac{25}{7.5} = 3.33\,m/s

    • Scenario 3 (Explosion / Separation from Rest):

    • Both carts start united at rest (pi=0p_i = 0). An internal mechanism pushes them apart, causing Cart A to move left at 10 m/s10\,m/s (vAf=−10 m/sv_{Af} = -10\,m/s):

    • 0=mAvAf+mBvBf0 = m_A v_{Af} + m_B v_{Bf}

    • 0=(5 kg)(−10 m/s)+(2.5 kg)vBf0 = (5\,kg)(-10\,m/s) + (2.5\,kg) v_{Bf}

    • 0=−50+2.5vBf→50=2.5vBf→vBf=20 m/s0 = -50 + 2.5 v_{Bf} \rightarrow 50 = 2.5 v_{Bf} \rightarrow v_{Bf} = 20\,m/s (to the right)

  • Single-Object Momentum and Velocity Calculations:

    • Challenge 1 (Equipment Crate on Studio Floor):

    • A heavy equipment crate slides left at v=−2.5 m/sv = -2.5\,m/s, having momentum p=−150 kg m/sp = -150\,kg\,m/s.

    • Rearrange formula for mass: m=pvm = \frac{p}{v}

    • Calculate mass: m=−150 kg m/s−2.5 m/s=60 kgm = \frac{-150\,kg\,m/s}{-2.5\,m/s} = 60\,kg

    • Physical reasoning: Mass must be positive because it is a scalar magnitude; the negative sign belongs exclusively to the velocity vector indicating leftward movement.

    • Challenge 2 (Autonomous Underwater Inspection Robot):

    • A robot of mass m=80 kgm = 80\,kg has a recorded momentum of p=−240 kg m/sp = -240\,kg\,m/s.

    • Rearrange for velocity: v=pm=−240 kg m/s80 kg=−3 m/sv = \frac{p}{m} = \frac{-240\,kg\,m/s}{80\,kg} = -3\,m/s

    • Velocity Magnitude = 3 m/s3\,m/s

    • Direction = Left

  • Push-Apart and Docking Investigations:

    • Challenge 3 (Curling Stones Collision):

    • Stone A (mA=20 kgm_A = 20\,kg) slides right at vAi=+2.0 m/sv_{Ai} = +2.0\,m/s and strikes stationary Stone B (mB=20 kgm_B = 20\,kg, vBi=0 m/sv_{Bi} = 0\,m/s). Stone A deflects forward at vAf=+0.60 m/sv_{Af} = +0.60\,m/s.

    • mAvAi+mBvBi=mAvAf+mBvBfm_A v_{Ai} + m_B v_{Bi} = m_A v_{Af} + m_B v_{Bf}

    • (20)(2.0)+(20)(0)=(20)(0.60)+(20)vBf(20)(2.0) + (20)(0) = (20)(0.60) + (20) v_{Bf}

    • 40=12+20vBf→28=20vBf→vBf=1.4 m/s40 = 12 + 20 v_{Bf} \rightarrow 28 = 20 v_{Bf} \rightarrow v_{Bf} = 1.4\,m/s

    • Total momentum before and after is conserved at +40 kg m/s+40\,kg\,m/s.

    • Challenge 4 (Research Barges Docking):

    • Barge A (mA=400 kgm_A = 400\,kg) travels east at vAi=+2.0 m/sv_{Ai} = +2.0\,m/s. Barge B travels west at vBi=−0.50 m/sv_{Bi} = -0.50\,m/s. They collide, lock together, and continue east at vf=+0.50 m/sv_f = +0.50\,m/s.

    • mAvAi+mBvBi=(mA+mB)vfm_A v_{Ai} + m_B v_{Bi} = (m_A + m_B) v_f

    • (400)(2.0)+mB(−0.50)=(400+mB)(0.50)(400)(2.0) + m_B(-0.50) = (400 + m_B)(0.50)

    • 800−0.50mB=200+0.50mB800 - 0.50 m_B = 200 + 0.50 m_B

    • Subtract 200200 and add 0.50mB0.50 m_B: 600=1.0mB→mB=600 kg600 = 1.0 m_B \rightarrow m_B = 600\,kg

    • Evaluation of claim: An observer claims that because the barges moved toward each other, combined motion must be west. This claim is refuted; total initial system momentum (pi=800−300=+500 kg m/sp_i = 800 - 300 = +500\,kg\,m/s) is net eastward (positive), which dictates post-docking motion to the east.

    • Challenge 5 (Ocean Research Floats Push-Apart):

    • Two floats start at rest (pi=0p_i = 0) in calm water. An internal spring expands, propelling Instrument A (mA=24 kgm_A = 24\,kg) west at vAf=−1.5 m/sv_{Af} = -1.5\,m/s, and Instrument B east at vBf=+0.90 m/sv_{Bf} = +0.90\,m/s.

    • 0=mAvAf+mBvBf0 = m_A v_{Af} + m_B v_{Bf}

    • 0=(24)(−1.5)+mB(0.90)0 = (24)(-1.5) + m_B(0.90)

    • 0=−36+0.90mB→36=0.90mB→mB=40 kg0 = -36 + 0.90 m_B \rightarrow 36 = 0.90 m_B \rightarrow m_B = 40\,kg

    • Physical reasoning: Total momentum remains zero because the objects possess equal and opposite signed momenta (−36 kg m/s-36\,kg\,m/s and +36 kg m/s+36\,kg\,m/s) which sum to zero.

    • Challenge 6 (Film Studio Motorized Platforms Rebound):

    • Platform A (mA=40 kgm_A = 40\,kg) moves right at vAi=+3.0 m/sv_{Ai} = +3.0\,m/s. Platform B moves left at vBi=−1.0 m/sv_{Bi} = -1.0\,m/s. Motors are unpowered during collision. Platform A rebounds left at vAf=−2.0 m/sv_{Af} = -2.0\,m/s, and Platform B moves right at vBf=+1.0 m/sv_{Bf} = +1.0\,m/s.

    • mAvAi+mBvBi=mAvAf+mBvBfm_A v_{Ai} + m_B v_{Bi} = m_A v_{Af} + m_B v_{Bf}

    • (40)(3.0)+mB(−1.0)=(40)(−2.0)+mB(1.0)(40)(3.0) + m_B(-1.0) = (40)(-2.0) + m_B(1.0)

    • 120−1.0mB=−80+1.0mB120 - 1.0 m_B = -80 + 1.0 m_B

    • Add 8080 and add 1.0mB1.0 m_B: 200=2.0mB→mB=100 kg200 = 2.0 m_B \rightarrow m_B = 100\,kg

    • Physical reasoning: Simple scalar addition of momentum magnitudes cannot determine total momentum because momentum is a directional vector requiring signed arithmetic.

    • Challenge 7 (Automated Baggage Carriers):

    • Carrier A (mA=10 kgm_A = 10\,kg) moves right at vAi=+3.0 m/sv_{Ai} = +3.0\,m/s. Carrier B (mB=20 kgm_B = 20\,kg) moves left at vBi=−1.5 m/sv_{Bi} = -1.5\,m/s. They collide and lock together.

    • pi=(10)(+3.0)+(20)(−1.5)=30−30=0 kg m/sp_i = (10)(+3.0) + (20)(-1.5) = 30 - 30 = 0\,kg\,m/s

    • (mA+mB)vf=0→(10+20)vf=0→30vf=0→vf=0 m/s(m_A + m_B) v_f = 0 \rightarrow (10 + 20) v_f = 0 \rightarrow 30 v_f = 0 \rightarrow v_f = 0\,m/s

    • Technician claim: A technician claims the carriers will remain completely stationary post-collision because their initial momenta cancel. This claim is supported (pA=+30 kg m/sp_A = +30\,kg\,m/s and pB=−30 kg m/sp_B = -30\,kg\,m/s sum to zero).

    • Challenge 8 (Magnetic-Levitation Pod Separation):

    • Pod A (mA=12 kgm_A = 12\,kg) and Pod B (mB=18 kgm_B = 18\,kg) travel rightward together at vi=+1.0 m/sv_i = +1.0\,m/s via a compressed spring latch. Upon release, Pod A reverses left at vAf=−2.0 m/sv_{Af} = -2.0\,m/s.

    • (mA+mB)vi=mAvAf+mBvBf(m_A + m_B) v_i = m_A v_{Af} + m_B v_{Bf}

    • (12+18)(1.0)=(12)(−2.0)+(18)vBf(12 + 18)(1.0) = (12)(-2.0) + (18) v_{Bf}

    • 30=−24+18vBf30 = -24 + 18 v_{Bf}

    • Add 2424: 54=18vBf→vBf=+3.0 m/s54 = 18 v_{Bf} \rightarrow v_{Bf} = +3.0\,m/s

    • Direction of Pod B: Rightward

    • Total momentum before (+30 kg m/s+30\,kg\,m/s) equals total momentum after (−24+54=+30 kg m/s-24 + 54 = +30\,kg\,m/s).

  • Spacewalk Equipment Push Investigation:

    • An astronaut pushes a cargo container of mass mC=30 kgm_C = 30\,kg in space under zero external impulse conditions. The combined mass of the astronaut and spacesuit is mAm_A.

    • Trial 1 (Determining Unknown Mass from Rest):

    • Initial state: vAi=0 m/sv_{Ai} = 0\,m/s, vCi=0 m/sv_{Ci} = 0\,m/s

    • Final state: vAf=−0.60 m/sv_{Af} = -0.60\,m/s, vCf=+2.40 m/sv_{Cf} = +2.40\,m/s

    • Conservation equation: 0=mAvAf+mCvCf0 = m_A v_{Af} + m_C v_{Cf}

    • 0=mA(−0.60)+(30)(+2.40)0 = m_A(-0.60) + (30)(+2.40)

    • 0=−0.60mA+72→0.60mA=72→mA=120 kg0 = -0.60 m_A + 72 \rightarrow 0.60 m_A = 72 \rightarrow m_A = 120\,kg

    • Trial 2 (Predicting Velocity from Initial Motion):

    • Initial state: vAi=+0.50 m/sv_{Ai} = +0.50\,m/s, vCi=+0.50 m/sv_{Ci} = +0.50\,m/s

    • Final state: vAf=+0.20 m/sv_{Af} = +0.20\,m/s, vCfv_{Cf} is unknown.

    • Using mass mA=120 kgm_A = 120\,kg:

    • mAvAi+mCvCi=mAvAf+mCvCfm_A v_{Ai} + m_C v_{Ci} = m_A v_{Af} + m_C v_{Cf}

    • (120)(0.50)+(30)(0.50)=(120)(0.20)+(30)vCf(120)(0.50) + (30)(0.50) = (120)(0.20) + (30) v_{Cf}

    • 60+15=24+30vCf60 + 15 = 24 + 30 v_{Cf}

    • 75=24+30vCf→51=30vCf→vCf=+1.7 m/s75 = 24 + 30 v_{Cf} \rightarrow 51 = 30 v_{Cf} \rightarrow v_{Cf} = +1.7\,m/s

    • Final velocity of container: 1.7 m/s1.7\,m/s directed to the right.

    • Trial 3 (Full Momentum Balance Evaluation):

    • Initial state: vAi=0 m/sv_{Ai} = 0\,m/s, vCi=0 m/sv_{Ci} = 0\,m/s

    • Final state: vAf=−0.50 m/sv_{Af} = -0.50\,m/s, vCf=+2.00 m/sv_{Cf} = +2.00\,m/s

    • Total momentum before push: pi=(120)(0)+(30)(0)=0 kg m/sp_i = (120)(0) + (30)(0) = 0\,kg\,m/s

    • Total momentum after push:

      • pf=(120 kg)(−0.50 m/s)+(30 kg)(+2.00 m/s)=−60 kg m/s+60 kg m/s=0 kg m/sp_f = (120\,kg)(-0.50\,m/s) + (30\,kg)(+2.00\,m/s) = -60\,kg\,m/s + 60\,kg\,m/s = 0\,kg\,m/s

    • Scientific Argument and Invariance Summary:

    • System momentum is strictly conserved across all trials: Trial 1 has 0 kg m/s0\,kg\,m/s before and after; Trial 2 has 75 kg m/s75\,kg\,m/s before and after; Trial 3 has 0 kg m/s0\,kg\,m/s before and after.

    • For the momentum of a system to change, a net external force must act on the system.