As in this post, I'm trying to understand why area of a sector of a circle $= \dfrac{\theta r^2}{2} $ WITHOUT relying on $\dfrac{\theta }{2\pi} \pi {r}^{2}$ or $\dfrac{\theta }{2\pi} 2 \pi {r}$ or integrals. To picture the emboldened phrase in Skeeter's reply, I edited this picture, but I can't picture why the orange curve is $r⋅dθ$?
to justify this formula w/o using the mentioned geometrical relationship requires the use of the calculus ...
consider a sector with a very small $θ=dθ$, and note the area of a small sector is close to the area of a triangle.
remembering the area of a triangle, $A=bh/2$ , the base is the small arclength equal to $r \cdot dθ$ and the height is equal to $r$ ...
a small sector of the large sector has area $dA=\dfrac{bh}2=\dfrac{r⋅dθ⋅r}2=\dfrac{r^2⋅dθ}2$
suffice it to say that summing all the small sectors that make up the larger sector results in $A=\dfrac{r^2⋅θ}2$