Conducting rod moving on an inclined rail and electromagnetic induction
Problem Statement
Conducting rod moving on an inclined rail and electromagnetic induction
Problem Statement
Two smooth, parallel conductive rails are fixed at a distance L, inclined at an angle θ with respect to the horizontal plane. A resistor with resistance R is connected to the highest point of each rail. A uniform magnetic field (magnetic flux density B) is applied to the entire inclined plane formed by the rails, perpendicular to the incline and directed upward.
A conducting rod of mass m is placed on these rails perpendicular to the rails and released gently. The conducting rod slides down the incline along the rails. Assume that the resistance of the conducting rod and rails, the self-inductance of the circuit, and air resistance are all negligible, and the magnitude of the acceleration due to gravity is g.
After a sufficient amount of time has elapsed since the release of the conducting rod, it begins to move in a straight line at a constant velocity v. Find the algebraic expression for the magnitude of this velocity v.
Constraints
- m=0.200 kg
- g=9.80 m/s2
- θ=30.0∘
- R=4.00 Ω
- B=0.700 T
- L=1.00 m
Input Format
Calculate the magnitude of the velocity of the conducting rod v [m/s] after a sufficient amount of time has elapsed, and input a natural number representing that value.
Solution
Explanation
Equations for Induced Electromotive Force and Current
When a conducting rod moves downward along a rail at a speed v, electromagnetic induction occurs when the conducting rod crosses a magnetic wire. The magnitude of the induced electromotive force V in the conducting rod is expressed as follows: V=vBL
According to Lenz's law, this electromotive force tries to induce a current in a direction that opposes the change in magnetic flux (counterclockwise when viewed from above). Since the resistance of the resistor is R and other resistances can be ignored, according to Ohm's law, the magnitude of the current I flowing through the circuit is as follows: I=RV=RvBL
Force Acting on the Conducting Rod and Equation of Motion
A conducting rod through which current I flows is subjected to an Ampere force (electromagnetic force) from the magnetic field. According to Fleming's left-hand rule, the direction of this force is upward along the inclined plane. Its magnitude FA is expressed as follows: FA=IBL=RvB2L2
The conducting rod is subjected to a gravitational component mgsinθ acting parallel to the inclined plane downwards. Therefore, the equation of motion for the conducting rod, with the downward direction of the inclined plane as positive, is as follows: mdtdv=mgsinθ−RvB2L2
Calculation of Velocity during Uniform Linear Motion
After a sufficient amount of time has elapsed, the conducting rod will move in a uniform linear motion at a constant velocity. At this time, the acceleration is 0 (dtdv=0), so the forces in the direction of the inclined plane are balanced. mgsinθ−RvB2L2=0
Solve this equation for v.
v=B2L2mgRsinθ
Numerical Substitution
We substitute the given constraint values and calculate. Note that sin30.0∘=0.500.
v=0.7002×1.0020.200×9.80×4.00×0.500
We calculate the numerator and denominator separately.
- Numerator: 0.200×9.80×4.00×0.500=3.92
- Denominator: 0.7002×1.002=0.490
Therefore, the velocity v is as follows:
v=0.4903.92=8.00 m/s
The natural number to input is 8.
Answer: 8