CLASSICAL-MECHANICS Β· Interactive Practice

From Components to Coordinates: Vectors

IKey Formulas

Formula Name Description
Aβƒ—=Ax i^+Ay j^+Az k^\vec{A} = A_x\,\hat{i} + A_y\,\hat{j} + A_z\,\hat{k} Components Vector by its components
∣Aβƒ—βˆ£=Ax2+Ay2+Az2\lvert\vec{A}\rvert = \sqrt{A_x^2 + A_y^2 + A_z^2} Magnitude Square, add, square root
A⃗±B⃗=(Ax±Bx, Ay±By, Az±Bz)\vec{A}\pm\vec{B} = (A_x\pm B_x,\ A_y\pm B_y,\ A_z\pm B_z) Add / Subtract Component by component
A^=Aβƒ—βˆ£Aβƒ—βˆ£\hat{A} = \dfrac{\vec{A}}{\lvert\vec{A}\rvert} Unit vector Direction, length 1
(x,y)=(rcos⁑θ, rsin⁑θ)(x, y) = (r\cos\theta,\ r\sin\theta) Polar form Angle θ\theta from +x+x axis

IIVisualization 1 β€” Components, Magnitude & Direction

Two perpendicular components fix both how long a vector is and which way it points.

IIIVisualization 2 β€” Bearings to Standard Angles

Why must a compass bearing become a standard angle from +x+x before it goes into rcos⁑θr\cos\theta and rsin⁑θr\sin\theta?

πŸ’‘ Plug the raw bearing straight into cos⁑\cos and sin⁑\sin and you land in the wrong quadrant β€” convert to ΞΈ\theta from +x+x first.

IVVisualization 3 β€” Point on a Segment

As a point slides from P1P_1 to P2P_2, its position vector is a weighted average of the two endpoints.

VQuiz Questions

Question 1

Given the vector Aβƒ—=2 i^βˆ’3 j^+7 k^\vec{A} = 2\,\hat{i} - 3\,\hat{j} + 7\,\hat{k}, what is its magnitude ∣Aβƒ—βˆ£\lvert\vec{A}\rvert?

βœ… Correct! 4+9+49=62\sqrt{4+9+49} = \sqrt{62}.

❌ Not quite. Remember to square each component (including the negative one) before adding.

Show solution

Solution:

Square each component, add, then take the square root: ∣Aβƒ—βˆ£=22+(βˆ’3)2+72=4+9+49=62β‰ˆ7.87\lvert\vec{A}\rvert = \sqrt{2^2 + (-3)^2 + 7^2} = \sqrt{4 + 9 + 49} = \sqrt{62} \approx 7.87

The negative component squares to a positive value β€” magnitudes are never negative.

Question 2

A vector points 18° south of east at a distance of 24 km from the origin (east is +x+x, north is +y+y). What standard angle θ\theta, measured from the positive x-axis, should you use in rcos⁑θr\cos\theta and rsin⁑θr\sin\theta?

βœ… Correct! South of east is below the +x axis, so ΞΈ = -18Β°.

❌ Not quite. 'South of east' rotates below the positive x-axis β€” that is a negative angle.

Show solution

Solution:

"South of east" means start on the positive x-axis (east) and rotate downward (toward south) by 18Β°. Measuring from the positive x-axis, a downward rotation is negative: ΞΈ=βˆ’18Β°\theta = -18Β°

A common mistake is to plug the compass number +18Β°+18Β° straight in, which would point above the x-axis instead of below it.

Question 3

A Coast Guard ship is at position r1βƒ—=βˆ’21.5 i^+27.6 j^\vec{r_1} = -21.5\,\hat{i} + 27.6\,\hat{j} km and a sailboat is at r2βƒ—=22.8 i^βˆ’7.4 j^\vec{r_2} = 22.8\,\hat{i} - 7.4\,\hat{j} km. What is the displacement vector r2βƒ—βˆ’r1βƒ—\vec{r_2} - \vec{r_1} the ship must travel?

βœ… Correct! Subtracting components gives 44.3 i - 35.0 j km.

❌ Not quite. Subtract component by component: be careful with the double negative in x (22.8 βˆ’ (βˆ’21.5)).

Show solution

Solution:

Subtract component by component, r2βƒ—βˆ’r1βƒ—\vec{r_2} - \vec{r_1}:

x:22.8βˆ’(βˆ’21.5)=44.3Β kmx:\quad 22.8 - (-21.5) = 44.3 \text{ km} y:βˆ’7.4βˆ’27.6=βˆ’35.0Β kmy:\quad -7.4 - 27.6 = -35.0 \text{ km}

So r2βƒ—βˆ’r1βƒ—=44.3 i^βˆ’35.0 j^\vec{r_2} - \vec{r_1} = 44.3\,\hat{i} - 35.0\,\hat{j} km.

The magnitude is 44.32+35.02β‰ˆ56.5\sqrt{44.3^2 + 35.0^2} \approx 56.5 km, and the heading is tanβ‘βˆ’1(βˆ’35.0/44.3)β‰ˆβˆ’38.3Β°\tan^{-1}(-35.0/44.3) \approx -38.3Β°, i.e. 38.3Β° south of east.

Question 4

The position vector of a point on the segment from P1P_1 to P2P_2 is Aβƒ—=(1βˆ’ad)r1βƒ—+ad r2βƒ—\vec{A} = \left(1 - \tfrac{a}{d}\right)\vec{r_1} + \tfrac{a}{d}\,\vec{r_2} where aa is the distance from P1P_1 and dd is the segment length.

True or False: When a=da = d, the formula gives A⃗=r2⃗\vec{A} = \vec{r_2} (the point sits exactly at P2P_2).

βœ… Correct! With a/d = 1 the first term vanishes, leaving A = rβ‚‚.

❌ Not quite. Plug in a/d = 1: the coefficient of r₁ becomes 0 and rβ‚‚'s becomes 1.

Show solution

Solution:

Substitute a=da = d, so a/d=1a/d = 1: Aβƒ—=(1βˆ’1) r1βƒ—+(1) r2βƒ—=r2βƒ—\vec{A} = (1 - 1)\,\vec{r_1} + (1)\,\vec{r_2} = \vec{r_2}

The point sits exactly at P2P_2. (Similarly, a=0a = 0 gives A⃗=r1⃗\vec{A} = \vec{r_1}.) This confirms the formula is a weighted average that slides smoothly between the two endpoints — so the statement is True.

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