Vector Physics and Relative Velocity

Vector Fundamentals and Graphical Representation

  • Definition of a Vector:

    • A vector quantity is completely defined by two fundamental properties: its magnitude (مقداره\text{مقداره}) and its direction (اتجاهه\text{اتجاهه}).

    • Vectors are represented graphically using a directed line segment (an arrow).

  • Graphical Rules for Vector Representation (التمثيل البياني للمتجهات\text{التمثيل البياني للمتجهات}):

    • The magnitude of the vector is directly proportional to the length of the arrow (مقدار المتجه يعبر عنه طول السهم\text{مقدار المتجه يعبر عنه طول السهم}).

    • The orientation and arrowhead define the vector's direction in space.

    • Scale Mapping Examples:

    • A speed vector V=3m/sV = 3\,\text{m/s} pointing East can be represented graphically by a line of length 3cm3\,\text{cm} using a scale of 1cm=1m/s1\,\text{cm} = 1\,\text{m/s}.

    • A force vector F=5NF = 5\,\text{N} pointing North (5نيوتن شمالاً5\,\text{نيوتن شمالاً}) is represented by an arrow of proportional length pointing vertically upwards.

    • A velocity vector V=3m/sV = 3\,\text{m/s} pointing East (3م/ث شرقاً3\,\text{م/ث شرقاً}) is drawn horizontally to the right.

  • Vector Shift/Translation Property (ملاحظة نقل المتجه\text{ملاحظة نقل المتجه}):

    • Any vector can be freely shifted or translated in space provided that its magnitude (length of the arrow) and its direction are strictly preserved.

Resultant Vectors and Vector Addition Methods

  • Concept of the Resultant Vector (المحصلة\text{المحصلة}):

    • The resultant vector (Mres\vec{M}_{res} or Vres\vec{V}_{res}) represents the single combined vector that produces the same effect as two or more individual vectors acting together.

    • Vector addition formula: Mres=A+B\vec{M}_{res} = \vec{A} + \vec{B} or Vres=vA+vB\vec{V}_{res} = \vec{v}_A + \vec{v}_B.

    • Head-to-Tail Method (طريقة الرأس والذيل\text{طريقة الرأس والذيل}):

    • To add vectors graphically, place the tail (الذيل\text{الذيل}) of the second vector at the head (الرأس\text{الرأس}) of the first vector.

    • The angle θ\theta of the resultant with the horizontal axis is determined by tan(θ)=vBvA\tan(\theta) = \frac{v_B}{v_A}.

  • Rules for Calculating Resultant Force Magnitude (إيجاد مقدار محصلة القوى\text{إيجاد مقدار محصلة القوى}):

    • Vectors in the Same Direction (Parallel):

    • Perform simple algebraic addition: f=f1+f2f = f_1 + f_2.

    • Vectors in Opposite Directions (Anti-parallel):

    • Perform simple algebraic subtraction: f=f1f2f = f_1 - f_2 (or f=f2f1f = f_2 - f_1).

    • Mutually Perpendicular Vectors (Orthogonal, 9090^\circ angle):

    • Apply the Pythagorean theorem: f=f12+f22f = \sqrt{f_1^2 + f_2^2}.

Vector Resolution and Component Analysis

  • Concept of Vector Resolution (تحليل المتجهات\text{تحليل المتجهات}):

    • Vector resolution is the inverse operation of finding the resultant vector. It decomposes a single vector into two perpendicular components along the horizontal (xx) and vertical (yy) axes.

  • General Equations for Vector Components:

    • Horizontal Component (المركبة الأفقية\text{المركبة الأفقية} / المسقط الأفقي\text{المسقط الأفقي}):

    • For force: Fx=Fcos(α)F_x = F \cos(\alpha)

    • For velocity: Vx=Vcos(α)V_x = V \cos(\alpha)

    • Vertical Component (المركبة الرأسية\text{المركبة الرأسية} / المسقط الرأسي\text{المسقط الرأسي}):

    • For force: Fy=Fsin(α)F_y = F \sin(\alpha)

    • For velocity: Vy=Vsin(α)V_y = V \sin(\alpha)

  • Concrete Examples and Case Studies:

    • Case Study 1: Calculating Displacement Magnitude and Direction

    • Given horizontal displacement x=3mx = 3\,\text{m} East (شرقاً\text{شرقاً}) and vertical displacement y=4my = 4\,\text{m} North (شمالاً\text{شمالاً}).

    • Displacement magnitude (dd):       d=x2+y2=32+42=9+16=25=5md = \sqrt{x^2 + y^2} = \sqrt{3^2 + 4^2} = \sqrt{9 + 16} = \sqrt{25} = 5\,\text{m}

    • Direction angle θ\theta relative to horizontal:       tan(θ)=yx=43    θ=tan1(43)36.89\tan(\theta) = \frac{y}{x} = \frac{4}{3} \implies \theta = \tan^{-1}\left(\frac{4}{3}\right) \approx 36.89^\circ

    • Complete displacement statement: 5m5\,\text{m} North of East making an angle of 36.8936.89^\circ with the horizontal (5m  شمال شرقه وتصنع زاوبة  36.89  مع الأفقي5\,\text{m \text{ شمال شرقه وتصنع زاوبة } 36.89 \text{ مع الأفقي}}).

    • Case Study 2: Component Reconstruction from Hypotenuse

    • Given a hypotenuse h=5mh = 5\,\text{m} at an angle θ=53.13\theta = 53.13^\circ with the horizontal.

    • Horizontal side (XX):       cos(53.13)=X5    X=5cos(53.13)=3m\cos(53.13^\circ) = \frac{X}{5} \implies X = 5 \cos(53.13^\circ) = 3\,\text{m}

    • Vertical side (YY):       sin(53.13)=Y5    Y=5sin(53.13)=4m\sin(53.13^\circ) = \frac{Y}{5} \implies Y = 5 \sin(53.13^\circ) = 4\,\text{m}

    • Angle verification:       tan(θ)=43    θ=53.13010235\tan(\theta) = \frac{4}{3} \implies \theta = 53.13010235^\circ

    • Case Study 3: Velocity Components at 3030^\circ

    • Given velocity magnitude V=5m/sV = 5\,\text{m/s} at an angle α=30\alpha = 30^\circ to the horizontal.

    • Horizontal velocity component (VxV_x):       Vx=Vcos(30)=5cos(30)=2.53m/s4.33m/sV_x = V \cos(30^\circ) = 5 \cos(30^\circ) = 2.5\sqrt{3}\,\text{m/s} \approx 4.33\,\text{m/s}

    • Vertical velocity component (VyV_y):       Vy=Vsin(30)=5sin(30)=2.5m/sV_y = V \sin(30^\circ) = 5 \sin(30^\circ) = 2.5\,\text{m/s}

    • Case Study 4: Vertical Component Determination via Tangent

    • Given opposite horizontal leg 5m/s5\,\text{m/s} and angle 3030^\circ:       tan(30)=5Vy    5=Vytan(30)    Vy=5tan(30)=53m/s\tan(30^\circ) = \frac{5}{V_y} \implies 5 = V_y \tan(30^\circ) \implies V_y = \frac{5}{\tan(30^\circ)} = 5\sqrt{3}\,\text{m/s}

Vector Subtraction and Directional Conventions

  • Principles of Vector Subtraction:

    • True mathematical vector subtraction does not exist as a separate operation in vector physics; subtraction is defined as the addition of a vector pointing in the opposite direction.

    • The negative sign (-) strictly indicates an opposite directional sense relative to a chosen positive reference axis.

  • Directional Sign Conventions:

    • East direction (الشرق\text{الشرق}) is defined as positive (++).

    • West direction (الغرب\text{الغرب}) is defined as negative (---).

  • Illustrative Examples:

    • An object moving with speed 3m/s3\,\text{m/s} East is denoted as V=+3m/sV = +3\,\text{m/s}.

    • An object moving with speed 5m/s5\,\text{m/s} West is denoted as V=5m/sV = -5\,\text{m/s}.

    • Combining a positive force/velocity of +10+10 with an opposing vector of 2-2:     Vres=(+10)+(2)=+8V_{res} = (+10) + (-2) = +8     The positive result (+8+8) signifies a net vector directed East (8شرقاً8\,\text{شرقاً}).

Relative Velocity Calculations

  • Definition of Relative Velocity (السرعة النسبية\text{السرعة النسبية}):

    • Relative velocity is the velocity of a body (e.g., BB) as observed from the reference frame of another moving body (e.g., AA).

  • General Relative Velocity Formulas:

    • Velocity of BB relative to AA:     vAB=vBvAv_{AB} = v_B - v_A

    • Velocity of AA relative to BB:     vBA=vAvBv_{BA} = v_A - v_B

    • Oppositional Identity:     vAB=vBAv_{AB} = -v_{BA}

  • Quantitative Scenarios:

    • Scenario A: Objects Moving in the Same Direction (East)

    • Object AA moves at vA=+3m/sv_A = +3\,\text{m/s} East (3شرقاً3\,\text{شرقاً}).

    • Object BB moves at vB=+4m/sv_B = +4\,\text{m/s} East (4شرقاً4\,\text{شرقاً}).

    • Relative position difference from coordinates A(1,1)A(1,1) and B(4,5)B(4,5) gives vector (41,51)=(3,4)(4-1, 5-1) = (3,4).

    • Relative velocity of BB relative to AA (vABv_{AB}):       vAB=vBvA=+4(+3)=+1m/sv_{AB} = v_B - v_A = +4 - (+3) = +1\,\text{m/s}

    • Relative velocity of AA relative to BB (vBAv_{BA}):       vBA=vAvB=+3(+4)=1m/sv_{BA} = v_A - v_B = +3 - (+4) = -1\,\text{m/s}

    • Scenario B: Objects Moving in Opposite Directions

    • Object AA moves at vA=+4m/sv_A = +4\,\text{m/s} East (4شرقاً4\,\text{شرقاً}).

    • Object BB moves at vB=5m/sv_B = -5\,\text{m/s} West (5غرباً5\,\text{غرباً}).

    • Relative velocity of BB relative to AA (vABv_{AB}):       vAB=vBvA=5(+4)=9m/sv_{AB} = v_B - v_A = -5 - (+4) = -9\,\text{m/s}

    • Relative velocity of AA relative to BB (vBAv_{BA}):       vBA=vAvB=+4(5)=+9m/sv_{BA} = v_A - v_B = +4 - (-5) = +9\,\text{m/s}

River Crossing Dynamics and Boat Kinetics

  • Kinematic System Setup (حركة القارب وضفة النهر\text{حركة القارب وضفة النهر}):

    • A boat crosses a river of width d=60md = 60\,\text{m} at an angle of 6060^\circ with the riverbank (ضفة النهر\text{ضفة النهر}).

    • Parallel component / adjacent speed along bank = 3m/s3\,\text{m/s}.

    • Total boat velocity along the angled trajectory = 6m/s6\,\text{m/s}.

  • Trigonometric Verification and Kinetic Solutions:

    • Verification of bank angle cosine:     cos(60)=36=12\cos(60^\circ) = \frac{3}{6} = \frac{1}{2}

    • Perpendicular velocity component across the river (VV):     sin(60)=V6    V=6sin(60)=6×32=33m/s\sin(60^\circ) = \frac{V}{6} \implies V = 6 \sin(60^\circ) = 6 \times \frac{\sqrt{3}}{2} = 3\sqrt{3}\,\text{m/s}

    • Time required to cross the river (tt):     Using the distance-speed-time relationship d=v×td = v \times t:     t=dV=6033=20311.55sect = \frac{d}{V} = \frac{60}{3\sqrt{3}} = \frac{20}{\sqrt{3}} \approx 11.55\,\text{sec}