 Light hits a metal plate, ejecting electrons  Once ejected, electrons are attracted to a positively charged electrode.  Electrode is connected to a sensitive meter.  When light shines on the metal plate, meter deflects (gets a current reading)  When light is turned off, meter reads zero.

Put a negatively charged screen in the way. Ejected electrons will be repelled back down to the metal. No current will be read on the meter.

Brighter light does not result in more energetic electrons punching through the screen.

Electrons make it through the screen

 Planck deduced that the energy of a wave of light is tied to its frequency. E = hf where h = 6.6x J s  UV light = high frequency = high energy.  Red light = low frequency = low energy.  Red light cannot give the electrons enough energy to get through the screen, but UV can.

 Light is a wave, but it is sent in packets  Each packet has a small quantity of energy given by its frequency (E = hf)  One packet knocks one electron, if it has the energy  Higher intensity does NOT equal more energetic electrons

 Low frequency light produces low energy electrons. These electrons cannot push through the negative screen.  Sending more packets of low frequency light will not help. It will just produce more low energy electrons, none of which can get past the screen.

 High frequency light produces high frequency electrons.  Even a dim beam of high frequency light will get a current reading in the meter.  Increasing the intensity of the beam in this case will mean an increased current reading in the meter.

 Applying the law of conservation of energy: E before = E after  If we treat this like a perfectly elastic collision E light = E electron  Turns out this is not quite right. It takes some energy to eject the electron from the atom, so the electron ends up with less energy than the light. Every element has a different hold on its electrons. The work done removing the electron is called the work function, W. E light = W + E electron