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Transcript
Physics Challenge Question 22: Solutions
Part 1
We know that the power dissipated in a resistor is P  I  V . We can rewrite
this equation using Ohm’s law:
P  I  V  I  I  R   I 2 R
V2
V 
P  I V    V 
R
R
Part 2
Although not all the energy we use to light a light bulb goes to creating light
(some of it also goes to heat), we will assume that the power dissipated is
directly proportional to the light bulb’s brightness.
In series, the two light bulbs will have the same current running through
them. However, one has twice the resistance. We can use our equation from
part 1 to easily calculate the ratio in dissipated power:
P6 I 2  6 

P3 I 2  3 
The current is the same, so it cancels out. We get
P6 6
 2
P3 3
The 6  bulb is twice as bright as the 3  bulb. The reason is that the
larger resistance causes a larger voltage drop over the 6  bulb.
Part 3
Again, we will assume that the power in a bulb is directly proportional to its
brightness.
The two bulbs are in parallel in this circuit, which means they have the same
voltage. Using the other equation from part 1:
V2
P6 
6
 2
P3 V
3
V cancels out, and we are left with
1
P6 
1
 6
1
P3
2
3
This time, the 3  bulb is twice as bright as the 6  bulb. (This is opposite
of part 2.) The reason is that the lower resistance bulb gets more current.