Deflection and Magnetic Fields in Thomson's Experiment

Your fellow scientistIn summary, to calculate the magnetic field required for a deflection of 0.20 radians in Thomson's experiment, we use the equation B = √(u theta / e/m(e) * x * d) and plug in the given values of u, theta, e/m(e), x, and d. This gives us a value of 0.00203 T, which is significantly stronger than the Earth's magnetic field of 0.5 * 10^-4 T.
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Homework Statement



Calculate the magnetic field required to produce a deflection of .20 radians in Thomson's experiment. Assume the potential across the deflection plate is u=200V, the length of the deflection plates is x=5.0 cm, and their separation d=1.5cm. Compare this value of B to the Earth's magnetic field (B=.5 G = .5 * 10^-4 T).

Homework Equations



e/m(e) = u theta / B^2 * x * d

e/m(e) = 1.7588 * 10^11 C/kg

The Attempt at a Solution



1.7588 * 10^11 C/kg = (200V) (.2 rad) / (B^2)(.05m)(.015m)

B^2 = (1.516*10^-6 T^2)(.2 rad)

Now I can't figure out how to convert theta from radians to make this make sense. Do I just multiply by .2? Then I get that B=.55*10^-3 T, but I think the right answer is closer to the Earth's magnetic field.
 
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Dear fellow scientist,

To calculate the magnetic field required for a deflection of 0.20 radians in Thomson's experiment, we first need to rearrange the equation e/m(e) = u theta / B^2 * x * d to solve for B. This gives us B = √(u theta / e/m(e) * x * d).

Next, we can plug in the given values: u = 200V, theta = 0.20 radians, e/m(e) = 1.7588 * 10^11 C/kg, x = 0.05m, and d = 0.015m.

This gives us B = √((200V)(0.20 rad) / (1.7588 * 10^11 C/kg)(0.05m)(0.015m)) = 0.00203 T.

Comparing this value to the Earth's magnetic field of 0.5 * 10^-4 T, we can see that the required magnetic field for the deflection in Thomson's experiment is significantly stronger.

I hope this helps with your calculations. Keep up the good work!
 

FAQ: Deflection and Magnetic Fields in Thomson's Experiment

What is Thomson's experiment?

Thomson's experiment, also known as the Cathode Ray Tube (CRT) experiment, was conducted by physicist J.J. Thomson in 1897 to discover the properties of electrons. It involved passing an electric current through a gas-filled tube to study the behavior of electrons in the presence of magnetic and electric fields.

How did Thomson use deflection in his experiment?

Thomson used a magnetic field to deflect the path of the electrons in the CRT. By varying the strength of the magnetic field and measuring the amount of deflection, he was able to determine the charge-to-mass ratio of the electron.

What is the significance of Thomson's experiment?

Thomson's experiment provided evidence for the existence of subatomic particles and helped to establish the concept of the electron as a fundamental unit of matter. It also led to the discovery of the electron's charge and mass, which were crucial for understanding atomic structure and the development of modern physics.

How does the magnetic field affect the path of electrons in Thomson's experiment?

The magnetic field exerts a force on the electrons, causing them to experience a deflection from their original path. The strength and direction of the force depends on the strength and orientation of the magnetic field, as well as the charge and velocity of the electrons.

What are the applications of Thomson's experiment?

Thomson's experiment laid the foundation for the study of electromagnetism and the development of technology such as television, computer monitors, and particle accelerators. It also provided a better understanding of the behavior of electrons, which has been crucial in fields such as quantum mechanics and nuclear physics.

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