A common confusion here: reading Hertz's and Lenard's experiments as measurements of electron energy. They were not. Neither wrote an energy equation. They established that light of high enough frequency liberates negative charge from a metal, and which surface it leaves.
Hertz, 1887. While studying the spark discharge that produced his electromagnetic waves, Hertz noticed the discharge across the gap occurred more readily — at lower applied voltage — when ultraviolet light fell on the negative electrode. UV was helping electrons escape the metal, so a smaller field sufficed. The finding was incidental: he was building a radio-wave experiment.
Hallwachs, 1888. A clean zinc plate joined to a gold-leaf electroscope, lit with UV. A negatively charged plate lost its charge; a neutral plate acquired positive charge; an already-positive plate became more positive. All three point one way: the plate loses negative particles.
Lenard, 1900. Two electrodes in an evacuated tube with a potential difference across them. Shine UV on the emitter plate and current flows in the external circuit; stop the light and the current stops at once. Charged particles crossing the vacuum complete the circuit — emitted by the illuminated plate, gathered by the other. Illuminating the collector instead does nothing.
The particles were identified as electrons when their charge-to-mass ratio matched Thomson's cathode-ray value, and the effect was named photoelectric. Hallwachs and Lenard also recorded a frequency selectivity: alkali metals — lithium, sodium, potassium, caesium — respond to visible light, while zinc, cadmium and magnesium need ultraviolet (NCERT Class 12 Physics, Chapter 11, page 275).
In NEET, this topic is tested as whose observation was what and which plate was illuminated. The energy bookkeeping — work function, threshold, stopping potential — belongs to the Einstein-equation topics.