Metals said:
I wasn't aware that the current of a series circuit was constant.
Metals said:
That defies everything I had previously learned, and makes resistors seems utterly useless.
Metals said:
There must clearly be a concept I am missing here.
You are in a muddle here and I'm surprised that no one seems to have picked up on it fully. (Too polite, I guess

)
Resistors would certainly be "utterly useless" if things worked the way you have "learned". I think you need to start at the beginning again and make no assumptions based on what you have understood so far.
To understand the relationship between Current and Volts in a resistive circuit there are two rules that apply: Kirchhoff's First and Second Laws. These are the "concept" that you need to learn and apply.
Google Kirchhoff's Laws and trawl around till you find a site that you are happy with. A .edu or .org URL will usually be reliable. Steer clear of most forums if you want to be sure to get your basics right. PF is pretty reliable because BS is usually spotted and dealt with.

But the following is more or less what you will learn.
The first law says that charge cannot 'build up' in any point of a resistive circuit so the total current flowing in and out of a junction ('node') must be zero. The second law says that the total energy put into a charge (from a battery, for instance) that flows round a loop within that circuit must be dissipated by the resistors in that loop, according to their Resistance. That implies nothing about a 'constant current' around a circuit.
If any resistor in a circuit is changed, you can expect it to affect the Volts and Currents
throughout that circuit. So no resistor is "useless". Circuits are full of resistors that will either produce a desired current from a source of Voltage or a desired Voltage by suitably sharing a supplied voltage between two resistors.
Working out simple circuits is easy if you approach things in the right order. You can often make things easier by spotting where two resistors can be reduced to just one resistor for analysis- where there are two (or more) in parallel between the same two nodes, you can always reduce them to one equivalent resistor and where there is a chain of two or more resistors joining two nodes (with no other possible paths) you can reduce them to a single equivalent resistor.
So in your OP diagram, the parallel pair can be reduced to a single resistor and that leads you to two resistors in series. That will allow you to work out the current flowing from the battery (I = V/R) Ignore any resistor values until you have worked out the principle. K1 tells you that the total current through R2 and R3 is the same as the current through R1. You can then calculate the Volts across R1. K2 tells you that the Volts across R2 and R3 is the left over Volts from the battery volts.
That info is enough to work out the Power dissipated by R1, R2 and R3.
I can't find any figures in your post but you only need to slot in the values that you have and Bob's Your Uncle.
PS You will very soon find that you can look at a circuit and do a lot of this stuff in your head, writing down intermediate answers directly.