A wire made of nickel has 50 m long and 0.5 mm in diameter. between the ends of this wire is
applied a potential difference of 110 volts. The electrical resistivity of nickel is
0.342 Ω.mm
2.m
−1. Determine:
a) The electrical conductivity of nickel;
b) the resistance of wire;
c) the conductance of it;
d) the intensity of the current;
e) The absorbed power.
f) the energy absorbed in 1 hour;
Problem data:
- Wire length: L = 50 m;
- Wire diameter: d = 0.5 mm;
- Potential difference between the ends of the wire: U = 110 V;
- Electrical resistivity of nickel: ρ = 0.342 Ω.mm2.m−1.
Problem diagram:
Solution
First, we will convert the diameter of the wire given in millimeters (mm) to meters (m), the nickel
resistivity given in ohm-square millimeter per meter (Ω.mm
2.m
−1)
to ohm-meter (Ω.m) and, in the item (f), the interval of time in hours (h) to seconds (s),
used in the
International System of Units (
SI).
\[
\begin{gather}
d=0.5\;\cancel{\text{mm}}\times \frac{10^{-3}\;\text{m}}{1\;\cancel{\text{mm}}}=5\times 10^{-1}\times 10^{-3}\;\text{m}=5\times 10^{-4}\;\text{m}\\[10pt]
\rho=0.342\;\frac{\Omega.\cancel{\text{mm}^{2}}}{\text{m}}\times \frac{\left(10^{-3}\;\text{m}\right)^{2}}{1\;\cancel{\text{mm}^{2}}}=3.42\times 10^{-1}\;\frac{\Omega}{\cancel{\text{m}}}\times 10^{-6}\;\text{m}^{\cancel{2}}=3.42\times 10^{-7}\;\Omega\text{m}\\[10pt]
1\;\text{hora}=3600\;\text{segundos}
\end{gather}
\]
a) Conductivity σ is given by
\[ \bbox[#99CCFF,10px]
{\sigma =\frac{1}{\rho }}
\]
\[
\begin{gather}
\sigma =\frac{1}{3.42\times 10^{-7}}\\
\sigma =0.292\times 10^{7}\\
\sigma =2.92\times 10^{-1}\times 10^{7}
\end{gather}
\]
\[ \bbox[#FFCCCC,10px]
{\sigma =2.92\times 10^{6}\;\text{S/m}}
\]
b) The resistance
R of the wire is
\[
\begin{gather}
\bbox[#99CCFF,10px]
{R=\rho \frac{L}{A}} \tag{I}
\end{gather}
\]
where
A is the cross-section area of the wire, the area a circle is given by
\[ \bbox[#99CCFF,10px]
{A=\pi r^{2}}
\]
the radius of the wire will be half of the diameter given in the problem
\( r=\dfrac{d}{2} \)
\[
\begin{gather}
A=\pi \left(\frac{d}{2}\right)^{2} \tag{II}
\end{gather}
\]
substituting the expression (II) into (I), the resistance will be
\[
R=\rho \frac{L}{\pi \left(\dfrac{d}{2}\right)^{2}}
\]
substituting the data of the problem and assuming π = 3.14, we have
\[
\begin{gather}
R=3.42\times 10^{-7}\times \frac{50}{3.14\times \left(\dfrac{5\times 10^{-4}}{2}\right)^{2}}\\
R=3.42\times 10^{-7}\times \frac{50}{3.14\times \dfrac{25\times 10^{-8}}{4}}\\
R=\frac{4\times 3.42\times 10^{-7}\times 50}{3.14\times 25\times 10^{-8}}\\
R=\frac{4\times 3.42\times 2}{3.14}\times 10^{-7}\times 10^{8}\\
R=\frac{13.68}{3.14}\times 10
\end{gather}
\]
\[ \bbox[#FFCCCC,10px]
{R=87.1\;\Omega}
\]
c) The conductance
G is given by
\[ \bbox[#99CCFF,10px]
{G=\frac{1}{R}}
\]
\[
G=\frac{1}{87.1}
\]
\[ \bbox[#FFCCCC,10px]
{G=0.011\;\text{S}}
\]
d) Using
Ohm's Law, we have
\[ \bbox[#99CCFF,10px]
{U=Ri}
\]
\[
\begin{gather}
i=\frac{U}{R}\\
i=\frac{110}{67.1}
\end{gather}
\]
\[ \bbox[#FFCCCC,10px]
{i=1.26\;\text{A}}
\]
e) The power absorbed by the wire is given by
\[ \bbox[#99CCFF,10px]
{P=Ri^{2}}
\]
\[
\begin{gather}
P=87.1\times (1.26)^{2}\\
P=87.1\times 1.59
\end{gather}
\]
\[ \bbox[#FFCCCC,10px]
{P=138.5\;\text{W}}
\]
f) The energy is given by
\[ \bbox[#99CCFF,10px]
{\Delta E=P\Delta t}
\]
\[
\Delta E=138.5\times 3600
\]
\[ \bbox[#FFCCCC,10px]
{\Delta E=498600\;\text{J}}
\]