Explanations & Calculations
Available data
Magnetic field = 0.4 G = 0.4 × 1 0 − 4 μ T = 0.4 × 1 0 − 10 T \small 0.4G = 0.4\times10^{-4}\mu T=0.4\times10^{-10}T 0.4 G = 0.4 × 1 0 − 4 μ T = 0.4 × 1 0 − 10 T Angle of dip = 6 0 0 \small 60^0 6 0 0 Speed of the moving rod = 10 m s − 1 \small 10ms^{-1} 10 m s − 1 Length of it = 5 m \small 5m 5 m
Then,
The horizontal component of the field is B h ⃗ = 0.4 G × cos 60 = 0.2 G \qquad\qquad
\begin{aligned}
\small \vec{B_h}&=\small 0.4G\times\cos60=0.2G
\end{aligned} B h = 0.4 G × cos 60 = 0.2 G
Vertical component of it is B v ⃗ = 0.4 G × sin 60 = 0.346 G \qquad\qquad
\begin{aligned}
\small \vec{B_v}&=\small 0.4G\times\sin 60=0.346G
\end{aligned} B v = 0.4 G × sin 60 = 0.346 G
(1) When the rod is moved parallel to the horizontal component, it is the magnetic field's vertical component that is being cut by the rod.
Then the induced EMF will be E ⃗ = ∣ B v ⃗ ∣ . l . v = 0.346 × 1 0 − 10 T × 5 m × 10 m s − 1 = 1.73 × 1 0 − 9 V \qquad\qquad
\begin{aligned}
\small \vec{E}&=\small |\vec{B_v}|.l.v\\
&=\small 0.346\times10^{-10}T\times5m\times10ms^{-1}\\
&=\small \bold{1.73\times 10^{-9}V}
\end{aligned} E = ∣ B v ∣. l . v = 0.346 × 1 0 − 10 T × 5 m × 10 m s − 1 = 1.73 × 1 0 − 9 V
(2) Similarly it is the horizontal component of the field that is being cut when the rod is moved parallel to the vertical component.
Then the induced EMF will be E ⃗ = 0.2 × 1 0 − 10 × 5 × 10 = 1 n V \qquad\qquad
\begin{aligned}
\small \vec{E}&=\small 0.2\times10^{-10}\times5\times10\\
&=\small \bold{1\,nV}
\end{aligned} E = 0.2 × 1 0 − 10 × 5 × 10 = 1 nV
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