In [16]:
%pylab inline
%precision 4
Out[16]:
A wire is shown in Figure P1-6 below which is carrying 2.0 A in the presence of a magnetic field.
In [17]:
B = 0.5 #[T]
i = 2.0 #[A]
l = 1.0 #[m]
The force on this wire can be calculated from the equation $$ \vec{F} = i(\vec{l}\times\vec{B}) = ilB$$
In [18]:
F = i*l*B
F
Out[18]:
Newton, into the page.
The wire is shown in Figure P1-7 is moving in the presence of a magnetic field.
In [19]:
v = 10.0 # [m/s]
B = 0.2 # [T]
l = 0.25 # [m]
theta = 45 # [deg]
The induced voltage on this wire can be calculated from the equation shown below. The voltage on the wire is positive downward because the vector quantity $\vec{v}\times \vec{B}$ points downward. $$ e_\text{ind} = (\vec{v}\times \vec{B}) \cdot \vec{l} = vBl\cos(\theta)$$
In [20]:
e_ind = v*B*l* cos(deg2rad(theta))
e_ind
Out[20]:
Volt, positive down.
Repeat Problem 1-10 for the wire in Figure P1-8 below:
In [21]:
v = 1.0 # [m/s]
B = 0.5 # [T]
l = 0.5 # [m]
theta = 90 # [deg]
The induced voltage on this wire can be calculated from the equation shown below. The total voltage is zero, because the vector quantity $\vec{v}\times \vec{B}$ points into the page, while the wire runs in the plane of the page.
$$ e_\text{ind} = (\vec{v}\times \vec{B}) \cdot \vec{l} = vBl\cos(\theta)$$
In [22]:
e_ind = v*B*l* cos(deg2rad(90))
e_ind
Out[22]:
Volts.