Animated Solution for Physics - Magnetic Effects of Current: A proton and an alpha particle, after being accelerated through same potential difference, enter uniform magnetic field, the direction of which is perpendicular to their velocities. Find the ratio of radii of the circular paths of the two particles.
Visualized Solution
Visualizing the Setup
A proton (p+) and an alpha particle (α2+) are accelerated through the same potential difference V.
They enter a uniform magnetic field B perpendicular to their velocities.
Radius of Circular Path
When a charged particle moves perpendicular to a magnetic field, it follows a circular path.
The radius of this path is given by:
r=qBmv
Velocity from Accelerating Potential
The kinetic energy gained by accelerating through a potential difference V is:
K=qV=21mv2
Solving for velocity v:
v=m2qV
Radius in terms of Potential
Substitute the expression for v into the radius formula:
r=qBmm2qV
Bringing m and q inside the square root:
r=qB22mV
Establishing Proportionality
Since the potential difference V and the magnetic field B are constant for both particles:
r∝qm
Setting up the Ratio
The ratio of the radius of the proton to the alpha particle is:
rαrp=mαmp⋅qpqα
Properties of Particles
For a proton:
mp=m, qp=e
For an alpha particle (Helium nucleus):
mα=4m, qα=2e
Final Calculation
Substitute the values into the ratio:
rαrp=4mm⋅e2e
rαrp=42=21
The Way Forward
What if they had the same kinetic energy K instead of the same potential V?
r=qB2mK⟹r∝qm
Always pay attention to which physical quantity is kept constant!
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The Sigma Insight: Motion of a Charge in Magnetic Fields
Solution Diagram
The Setup
Entering the Magnetic Arena
Imagine a proton and an alpha particle standing at the starting line of a particle accelerator. They are both subjected to the exact same accelerating potential difference, V. As they speed up, they gain kinetic energy and shoot out into a region filled with a uniform magnetic field, B, which is perfectly perpendicular to their direction of motion.
When a charged particle enters a magnetic field perpendicularly, it experiences a magnetic force that acts as a centripetal force, causing it to move in a perfect circle. Our goal is to find the ratio of the radii of the circular paths they trace out.
The Master Equation
Radius of the Path
The fundamental equation governing the radius r of a charged particle moving in a magnetic field is:
r=qBmv
Here, m is the mass, v is the velocity, q is the charge, and B is the magnetic field strength. However, we have a slight problem: we don't know their velocities directly. We only know they were accelerated through the same potential difference V.
The Energy Connection
Accelerating Potential
To bridge this gap, we need to relate the velocity v to the accelerating potential V. The work done by the electric field is converted entirely into the particle's kinetic energy:
K=qV=21mv2
By rearranging this equation, we can solve for the velocity:
v=m2qV
Now, let's substitute this expression for velocity back into our master radius equation:
r=qBmm2qV
By bringing the m and q from the denominator inside the square root, we get a beautiful, unified expression:
r=qB22mV
The Final Showdown
Comparing the Radii
Look closely at this new equation. The problem states that both the potential difference V and the magnetic field B are identical for both particles. Therefore, all the terms in the equation are constant except for the mass m and the charge q. This gives us a powerful proportionality:
r∝qm
This means the ratio of their radii will simply be:
rαrp=mαmp⋅qpqα
Now, we just need to plug in the properties of our particles. A proton has a mass m and a charge e. An alpha particle is a helium nucleus, meaning it consists of two protons and two neutrons. Thus, its mass is roughly 4m and its charge is 2e.
Substituting these values into our ratio:
rαrp=4mm⋅e2e
The m and e terms cancel out beautifully, leaving us with:
rαrp=42=21
And there we have it! The radius of the proton's path is 21 times the radius of the alpha particle's path.