Classical-Mechanics ¡ Unit 8 ¡ Video 3 ¡ Interactive Practice

The Free-Body Diagram: Deciding Which Forces Matter

IKey Formulas

FormulaNameWhat it says
F⃗=F⃗1+F⃗2+⋯\vec{F} = \vec{F}_1 + \vec{F}_2 + \cdotsTotal forceVector sum of every force on the system
F⃗=Fx ı^+Fy ȷ^+Fz k^\vec{F} = F_x\,\hat{\imath} + F_y\,\hat{\jmath} + F_z\,\hat{k}Cartesian componentsResolve the total force onto the axes
Fx=F1,x+F2,x+⋯F_x = F_{1,x} + F_{2,x} + \cdotsComponent-wise sumEach component adds independently

Key Insight: A free-body diagram counts only the forces acting on the system — never the forces the system exerts on everything else.

IINet Force as a Vector Sum

Two forces on a system combine tip-to-tail into one net force — and the magnitudes generally don't add.

💡 Challenge: arrange the two forces so the net force is zero — the system is then in equilibrium.

IIIResolving a Force into Components

Every force casts perpendicular shadows on the axes: F⃗=Fx ı^+Fy ȷ^\vec{F} = F_x\,\hat{\imath} + F_y\,\hat{\jmath}, with Fx=∣F⃗∣cos⁡θF_x = |\vec{F}|\cos\theta and Fy=∣F⃗∣sin⁡θF_y = |\vec{F}|\sin\theta.

💡 Each component is itself a sum: Fx=F1,x+F2,x+⋯F_x = F_{1,x} + F_{2,x} + \cdots — the diagram does the bookkeeping, one axis at a time.

IVWhich Forces Belong in the Model

The model is a choice — include the forces that matter, drop those both small and hard to compute.

💡 Whenever objects move, some friction is always present; the only question is whether the model can afford to ignore it.

VQuiz Questions

Problem 1 ¡ Add the Forces

Given: two forces act on a system, F⃗1=(3, −2)\vec{F}_1 = (3,\,-2) N and F⃗2=(−1, 5)\vec{F}_2 = (-1,\,5) N — find the net force F⃗\vec{F}.

✅ Correct! Add components with their signs: 3+(−1)=23 + (-1) = 2 and −2+5=3-2 + 5 = 3.
❌ Watch the signs. You added magnitudes; the components are signed, so 3+(−1)=23 + (-1) = 2, not 44.
❌ Not quite. Add the two vectors component by component, keeping every sign.
Show solution

Vectors add component by component:

F⃗=F⃗1+F⃗2=(3+(−1), −2+5)=(2, 3) N\vec{F} = \vec{F}_1 + \vec{F}_2 = (3 + (-1),\ -2 + 5) = (2,\,3)\text{ N}

The net force is (2, 3)(2,\,3) N — the xx-components combine to 22 and the yy-components to 33.

Problem 2 ¡ Magnitudes Don't Add

Given: F⃗1\vec{F}_1 points east with magnitude 33 N and F⃗2\vec{F}_2 points north with magnitude 44 N — find the magnitude of the net force ∣F⃗∣|\vec{F}|. ⚠️ Direction matters!

✅ Correct! Perpendicular forces combine by the Pythagorean theorem: 32+42=5\sqrt{3^2 + 4^2} = 5 N.
❌ Close, but that's 3+43 + 4. Magnitudes only add when the forces are parallel; here they are perpendicular.
❌ Not quite. The forces are at right angles — use ∣F⃗∣=Fx2+Fy2|\vec{F}| = \sqrt{F_x^2 + F_y^2}.
Show solution

East and north are perpendicular, so the components are Fx=3F_x = 3 N and Fy=4F_y = 4 N:

∣F⃗∣=Fx2+Fy2=32+42=9+16=25=5 N|\vec{F}| = \sqrt{F_x^2 + F_y^2} = \sqrt{3^2 + 4^2} = \sqrt{9 + 16} = \sqrt{25} = 5\text{ N}

Adding magnitudes (3+4=73 + 4 = 7) would only be right if both forces pointed the same way.

Problem 3 ¡ Resolve into Components

Given: a force of magnitude ∣F⃗∣=10|\vec{F}| = 10 N acts at θ=30°\theta = 30\degree above the +x+x axis — find FxF_x and FyF_y.

What is FxF_x?

What is FyF_y?

✅ Correct! Fx=10cos⁡30°≈8.66F_x = 10\cos 30\degree \approx 8.66 N and Fy=10sin⁡30°=5F_y = 10\sin 30\degree = 5 N.
❌ Check the horizontal leg. The xx-component uses cosine: Fx=∣F⃗∣cos⁡θF_x = |\vec{F}|\cos\theta.
❌ Check the vertical leg. The yy-component uses sine: Fy=∣F⃗∣sin⁡θF_y = |\vec{F}|\sin\theta.
Show solution

Drop perpendiculars from the tip of F⃗\vec{F} onto each axis:

Fx=∣F⃗∣cos⁡θ=10cos⁡30°=10⋅32≈8.66 NF_x = |\vec{F}|\cos\theta = 10\cos 30\degree = 10 \cdot \tfrac{\sqrt{3}}{2} \approx 8.66\text{ N} Fy=∣F⃗∣sin⁡θ=10sin⁡30°=10⋅12=5 NF_y = |\vec{F}|\sin\theta = 10\sin 30\degree = 10 \cdot \tfrac{1}{2} = 5\text{ N}

Swapping sine and cosine is the classic slip — cosine goes with the axis the angle is measured from.

Problem 4 ¡ Build the Model

Given: a metal block is pushed by hand across a rough table. Which set of forces gives the best working model?

✅ Correct! The essentials plus surface friction — simple enough to keep, small hard effects left out.
❌ Too few. Surface friction is usually significant here and its formula is simple, so dropping it makes the prediction wrong.
❌ Too many. Nothing is magnetic, and air resistance is small yet messy — including them makes the math intractable for no gain.
❌ Not quite. Gravity and the normal force are essential — leaving either out breaks the model.
Show solution

Keep the essentials: gravity, the normal force from the table, and the applied push all clearly act and all matter.

Keep surface friction: on a rough table it is significant, and its formula is simple — so include it.

Drop the small-and-hard: air resistance is often negligible here and its mathematics is messy; the magnetic force isn't acting at all.

Best model: gravity, normal, applied push, and surface friction. Include too few and the prediction is wrong; include too many and the math becomes impossible.

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