The double pendulum is already not that trivial!
I don't know, how complicated things must be, but already the "simple pendulum" would be a nice research project, which gives plenty of opportunities for both theoretical and experimental work. A rough project would be:
(a) derivation of the equation of motion: ##m L^2 \ddot{\phi}=-m g \sin \phi##, where ##\phi## is the angle with respect to the direction of ##\vec{g}##. The most simple case is where a mass is tight to a much lighter rope ("mathematical pendulum"). Then you can derive the equation of motion by analyzing the forces (gravitational field of the Earth + tension of the rope) on the body and writing down Newton's equation of motion, ##\vec{F}=m\vec{a}##.
More challenging is a rigid body fastened to rotate around a fixed axis, for which you need in addition the moment of inertia, center of mass, etc.
(b) Analyzing the solutions, which is tricky. The equation of motion cannot be solved with the standard elementary functions you are used to (it leads to socalled elliptic functions), but you can demonstrate energy conservation easily as an exact analytical result.
Next you can consider small excitations around the static solution ##\phi=0##, i.e., small amplitudes, where you can set ##\sin \phi \approx \phi##. Then you get "harmonic motion", and you can discuss the solutions of linear differential equations of 2nd order, finding the complete solutions (as superposition of two linearly independent solutions, ##\cos(\omega t)##, ##\sin (\omega t)##. In this approximation the frequency ##f=1/T=\omega/(2 pi)## is independent of the amplitude.
(c) Using the energy-conservation law next you can find the integral determining the exact period of the pendulum, which depends on the amplitude, but this integral is not solvable with elementary functions, but you can derive a series expansion in powers of the amplitude, calculating corrections to the amplitude-independent ##\omega##.
Alternatively you can also try perturbation theory with the amplitude as the expansion parameter. This is, however very amititious on the high-school level.
(d) Experimentally you can use the pendulum to determine the gravitational acceleration, ##g## at your place (using small-amplitude oscillations as a first approximation and discussing the systematical errors using this assumptions etc.). In addition you can also study the dependence of the period on the amplitude and compare it to the theoretical estimates of item (c).