Animated Solution for Physics - Electromagnetic Induction: An aeroplane with its wings spread 10 m, is flying at a speed of 180 km/h in a horizontal direction. The total intensity of Earth's field at that part is 2.5×10−4 Wb/m2 and the angle of dip is 60∘. The emf induced between the tips of the plane wings will be
Select Answer:
Visualized Solution
\text{Visualizing the Airplane in Earth's Magnetic Field}
l=10 m
v=180 km/h
B=2.5×10−4 T
θ=60∘
\text{Resolving the Magnetic Field}
BH=Bcosθ (Horizontal)
BV=Bsinθ (Vertical)
Only BV is perpendicular to both v and l
\text{Motional EMF Formula}
ε=B⊥lv
ε=(Bsinθ)lv
\text{Unit Conversion & Substitution}
v=180×185=50 m/s
ε=(2.5×10−4sin60∘)×10×50
\text{Evaluating the Expression}
sin60∘=23
ε=2.5×10−4×23×500
\text{Final Calculation}
ε=1250×10−4×21.732
ε=625×1.732×10−4
ε=1082.5×10−4 V
\text{Converting to Millivolts}
ε=108.25×10−3 V
ε=108.25 mV
\text{What if the plane flies vertically?}
If v∥BV⟹No flux cut
ε=BHlv
00:00 / 00:00
The Sigma Insight: Motional EMF
Solution Diagram
The Giant Flying Generator
Motional EMF in the Sky
Imagine an airplane soaring horizontally through the sky. While it cuts through the air to generate lift, it is simultaneously slicing through something invisible: Earth's magnetic field. Because the airplane's wings are made of conducting metal, this motion turns the entire aircraft into a giant flying battery! This phenomenon is a classic example of Motional EMF.
Analyzing the Setup
To understand how much voltage is generated across the wingtips, we first need to break down the physical parameters given in the problem:
Wingspan (l):10 mVelocity (v):180 km/hEarth's Magnetic Field (B):2.5×10−4 TAngle of Dip (θ):60∘
Earth's magnetic field is not perfectly horizontal; it dips downwards at an angle θ. We can resolve this field into two components: a horizontal component BH=Bcosθ and a vertical component BV=Bsinθ.
The Master Equation
For an EMF to be induced, the conductor must cut across the magnetic field lines. Mathematically, the motional EMF is given by the scalar triple product ε=(v×B)⋅l.
Since the airplane is flying horizontally, its velocity v and its wings l both lie in the horizontal plane. The horizontal component of the magnetic field BH also lies in this plane. Therefore, the wings do not "cut" the horizontal field lines in a way that produces an EMF along the wingspan.
However, the vertical component BV points straight down, perfectly perpendicular to both the velocity and the wings. This is the component that does the heavy lifting! Our master equation simplifies to:
ε=BVlv=(Bsinθ)lv
Final Calculation
Before we substitute our values, we must avoid a classic physics trap: unit mismatch. The velocity is given in km/h, which we must convert to standard SI units (m/s):
v=180×185=50 m/s
Now, we substitute everything into our EMF equation:
ε=(2.5×10−4sin60∘)×10×50
Knowing that sin60∘=23, we can simplify the expression:
ε=2.5×10−4×23×500
ε=1250×10−4×21.732
ε=625×1.732×10−4
ε=1082.5×10−4 V
To match the options provided, we format our answer into millivolts (mV) by shifting the decimal point:
ε=108.25×10−3 V=108.25 mV
And there we have it! The airplane generates an induced EMF of 108.25 mV across its wingtips. It's a beautiful demonstration of how the abstract laws of electromagnetism operate on a massive scale right above our heads.