Displacement, velocity, acceleration and force all have a size and a direction: they are vectors. In two dimensions the easiest way to handle a vector is to split it into an $x$-part and a $y$-part, using the Sine, Cosine and Tangent you know from geometry.
🔑 Key idea
A vector of magnitude $A$ at angle $\theta$ from the $+x$ axis has components $A_x = A\cos\theta$ and $A_y = A\sin\theta$. In general: the component along the side adjacent to the angle uses cosine; the one opposite uses sine.
💡 Why it works
Draw the vector as the hypotenuse of a right triangle whose legs lie along the axes. The legs are the components. Cosine is adjacent over hypotenuse, so the adjacent leg is $A\cos\theta$; sine is opposite over hypotenuse, so the opposite leg is $A\sin\theta$. Which leg is "adjacent" depends on which axis the angle is measured from, not on whether it is $x$ or $y$.
A 50 N force at 30°: Fx = 50 cos 30° = 43.3 N and Fy = 50 sin 30° = 25 N.
Worked examples
✏️ Worked example: Angle from the horizontal
A rope pulls a sled with $80\ \text{N}$ at $25^\circ$ above the horizontal. Find the components.
The angle is measured from $x$, so $x$ is adjacent: $F_x = 80\cos 25^\circ \approx 72.5\ \text{N}$.
Using sine for the $x$-component every time (or cosine every time). It depends on where the angle is measured from. Quick checks: as $\theta \to 0$ from an axis, the component along that axis should approach the whole vector (cosine does that). And the two components must satisfy $A_x^2 + A_y^2 = A^2$.
Practice
Pass with 3 right answers, the last 2 in a row. Each right answer earns 2 XP.