Grade 12 Physics · Breaking the vector
The arrow and its shadows
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The arrow and its shadows

Grade 11 kept forces on one line: a push forward, a weight down. This year they point wherever they like, and the first skill of the course is taking one slanted arrow apart. A force is a vector: it has a magnitude FF in newtons — how hard — and a direction angle θ\theta in degrees, measured from the horizontal +x+x axis. Those two numbers say everything about it.

Take it apart and you get its two components, the shadows it casts on the axes: Fx=FcosθF_x = F\cos\theta — read aloud F-x equals F cos theta — is the part lying along the horizontal, and Fy=FsinθF_y = F\sin\thetaF-y equals F sin theta — is the part standing up the vertical. The subscript names the AXIS, not an order: xx is the horizontal shadow, yy the vertical one, and every symbol here is measured in newtons except θ\theta, which wears degrees.

Why cosine on xx? Draw the right triangle. The angle sits between the arrow and the x-axis, so the x-side TOUCHES the angle — it is the adjacent side, and cosθ=adjacenthypotenuse\cos\theta = \dfrac{\text{adjacent}}{\text{hypotenuse}}. The y-side sits across from the angle — opposite — and sinθ=oppositehypotenuse\sin\theta = \dfrac{\text{opposite}}{\text{hypotenuse}}. Learn it as touching-versus-across and it survives every rotated diagram the exam can print. The one caveat worth a mark: this holds when θ\theta is measured from the x-axis. Give a problem an angle from the VERTICAL and the two swap — read the diagram, not the habit.