Every wave on this bench is written the same way — y = A·sin(kx − ωt + φ). Learn to read the sign of each term and you never again guess which way a wave moves or which source leads. Flip the signs below and watch the trace obey.
Hold x fixed and let time run. If the wave is sin(kx − ωt), a point that was at phase θ must move to larger x to keep kx − ωt constant — so the whole profile marches in +x. Swap to sin(kx + ωt) and it runs the other way.
The phase constant φ just rotates the phasor to its starting angle. A wave with +φ reaches every value earlier — it leads the reference; −φ lags behind. Spin the dial and compare the violet trace against the dim reference.
Two points on the same wave, or two waves that travelled different distances, differ in phase by Δφ = (2π/λ)·Δx. One whole wavelength of extra path is exactly 2π — right back in step. Slide the second marker and read the phase gap.