A wire with cross-sectional 0.50×10
−2 cm
2, conducts a direct
current equal to 4.0 A, given the elementary charge 1.6×10
−19 C,
determine:
a) The number of electrons passing through a cross-section per second;
b) The average speed of electrons, knowing that there are
1.8×10
20 electrons/cm
3.
Problem data:
- Cross-sectional area of wire: A = 0.50×10−2cm2;
- Electric current: i = 4.0 A;
- Elementary charge: e = 1.6×10−19 C.
Solution
a) In Figure 1, the electrons move across a cross-section, highlighted in gray. The electrical
current is given by
\[
\begin{gather}
\bbox[#99CCFF,10px]
{i=\frac{\Delta q}{\Delta t}} \tag{I}
\end{gather}
\]
The amount of charge that crosses a section is given by
\[
\begin{gather}
\Delta q=n{\mathrm e} \tag{II}
\end{gather}
\]
substituting the expression (II) into (I), we have
\[
\begin{gather}
i=\frac{n{\mathrm e}}{\Delta t}\\
n=\frac{i\Delta t}{\mathrm e}
\end{gather}
\]
substituting the problem data for Δ
t = 1 s
\[
\begin{gather}
n=\frac{4\times 1}{1.6\times 10^{-19}}\\
n=\frac{4\times 10^{19}}{1.6}
\end{gather}
\]
\[ \bbox[#FFCCCC,10px]
{n=2.5\times 10^{19}\;\text{elétrons}}
\]
b) The average speed is given by
\[
\begin{gather}
\bbox[#99CCFF,10px]
{\bar v=\frac{\Delta S}{\Delta t}} \tag{III}
\end{gather}
\]
then an electron passes through the cross-section of the wire in a instant will travel a
distance Δ
S in an interval of time Δ
t, the electron then passes
through another cross-section. These two cross-sections determine in the wire a cylinder with a
volume
V given by (Figure 2)
\[
\begin{gather}
\bbox[#99CCFF,10px]
{V=Bh} \tag{IV}
\end{gather}
\]
where
B is the area of the base of the cylinder, the cross-section area of wire
B =
A, and
h is the displacement of the electron,
h = Δ
S,
substituting these values in the expression (IV), we have
\[
\begin{gather}
V=A \Delta S\\
\Delta S=\frac{V}{A} \tag{V}
\end{gather}
\]
substituting the expression (V) in (III), we have
\[
\begin{gather}
\bar v=\frac{V}{A\Delta t} \tag{VI}
\end{gather}
\]
The density of charges
d is given by
\[
d=\frac{n}{V}
\]
where
n is the number of electrons contained in volume
V of the cylinder determined
by the two cross-sections on the wire, we have
\[
\begin{gather}
V=\frac{n}{d} \tag{VII}
\end{gather}
\]
substituting the expression (VII) into (VI), we obtain
\[
\bar v=\frac{n}{dA\Delta t}
\]
Using the problem data, the value of
n calculated in the previous item and the speed
calculated per unit of time we have Δ
t = 1 s
\[
\begin{gather}
\bar v=\frac{2.5\times 10^{19}}{1.8\times 10^{20}\times 0.50.10^{-2}\times 1}\\
\bar v=\frac{2.5\times 10^{19}}{9\times 10^{17}}\\
\bar v=\frac{2.5\times 10^{19}\times 10^{-17}}{9}\\
\bar v=0.28\times 10^{2}
\end{gather}
\]
\[ \bbox[#FFCCCC,10px]
{\bar v=28\;\text{cm/s}}
\]