As an example we take the DC experiment (part 1).
In particular, we look at
the setup for the parallel connection of the light bulbs
(see also fig.5, at pg. 56 in the Lab. manual).
As you may recall,
you are asked to measure the values of voltage drop across the:
a) battery: U0
b) first bulb (A): Ua
c) second bulb (B): Ub
If you work carefully, then you hopefully notice that the
voltages
across the battery and the light bulbs obey the relationship
U0 > Ua >
Ub
The difference between them is typically about 0.1 to 0.3 V.
This fact might
be surprising at a first glance, since one would expect to find instead:
U0
= Ua = Ub, as the theory predicts
for the case of parallel connection.
One of the reasons for this
mismatch
is that there is some voltage drop across the wires.
Of course, the values of voltages
U0 , Ua , and Ub by
themselves are subject
to errors as well (due to accuracy and/or precision of the V-meters), but at
this point you are interested in the observed trend
U0 > Ua > Ub.
The other phenomenon some of you observed happening, was that the battery
had a voltage unstable in time (decreasing, for large current output).
Although this effect really takes place, and is expected to occur, it cannot
explain the observed inequality between the voltages (it may explain why they
all drop together as you wait...)
It is now
the time to check numerically that your guess for this
source of voltage mismatch is indeed the voltage drop
across the wires.
You
have to give some numerical arguments for this.
It is mandatory to sustain your discussion with numerical argumentation
of your
claims!
N.B.
This discussion is
one of high level (say, for A+ ) ;
I don't expect you to do this in full
at the first experiment. My example is intended to show you the extension
and depth of discussions you have to achieve for the
experiments to follow.
Getting the numbers
Method #1
Set the V-meter on the "200mV" scale
and measure directly the voltage
drop across each of the connecting wires and the bulbs. On the diagram of your
setup (see above) write down all the voltages (across the wires).
Keep the diagram neat!
Hopefully, with the voltage drops you just measured, the 2-nd Kirchhoff's rule
holds with a better precision (I mean: the mismatch is much smaller than at
the beginning, when you didn't account for the wires).
Method #2
You take aside a few wires (4 or more), connect them in series, plug the multimeter
as Ohm-meter and try to get some reading for the resistance
of the wires.
Of course,
you have to choose the right range on the Ohm-meter ("200 Ohms" scale).
You'll get (roughly) for the resistance of 4 identical
wires connected in series
R = 0.4 Ohm.
Of course, you cannot really trust those digits; nevertheless they give us a
clue that the resistance of the wires is not zero!
There are a few reasons one cannot "really trust"
this value for R.
The first one is that you work at the level of the last
digit. For this scale, the accuracy error is
(0.5% of the reading + 4 digits),
the reading error being (1/2 digit).
Hence, the value of R can easily be
anywhere between 0 to 0.8 Ohms (!).
The second reason is that beside the "intrinsic"
resistance of the wires, you have also
resistance at the connection
points (though, in this case, this might be negligible. Well, in fact
you never
know for sure, so better safe than sorry...).
Nevertheless, all in all, roughly,
you can probably assume that (2 wires + the connection
points) have a resistance of about 0.2 Ohms.
Now, we go back to the currents we have measured, and
we see that roughly
we have
I0 =2 A, Ia =1A, Ib=1A.
Therefore, we may conclude that the voltage drop across the wires
is about
dU = I×R = 1A × 0.2 Ohm = 0.2 V,
which, hopefully is approximately equal to
the difference you found between Ua
and Ub.
For the wires between battery and first bulb (A)
you have a bigger current,
so the corresponding voltage drop is even bigger.
Have you seen this in the experiment?
Hint:
to measure the voltage across the bulbs use the V-meter on a scale
that provides at least 3-significant
digits ("2V" or "20V" scales).
Conclusion:
You have to bring numerical arguments in
the game, to prove that what you say is true!
N.B. As you may see, our argument was sustained
by the large values
of the currents through the wires. Although
not explicitly, our reasoning was based
on the small values of the resistances of the light bulbs,
which was comparable with
the resistance of the wires
(only about one order of magnitude between them).
If, in the part (2) of DC-I, you try to "blame"
the wires for this type of mismatch it won't work!
That's because there the currents have
10 to 20 times smaller values,
the resistors you're using have resistances of hundreds of Ohms or more,
so the resistance of the connecting wires
doesn't play any significant role.
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Last updated: May 16, 2003
© 2003, Sorin Codoban