Ch 29: The Magnetic Field

Knight Calc - Physics for Scientists and Engineers 5th Edition

Knight Calc5th EditionPhysics for Scientists and EngineersISBN: 9780137344796Non è quello che usi tu?Cambia libro di testo

Knight Calc 5th Edition

Ch 29: The Magnetic Field

Problema 27

Capitolo 29, Problema 27

A proton moves in the magnetic field B = 0.50 î T with a speed of 1.0 x 10⁷ m/s in the directions shown in FIGURE EX29.27. For each, what is magnetic force F on the proton? Give your answers in component form.

Guida verificata passo dopo passo

Step 1: Recall the formula for the magnetic force on a charged particle: $ \mathbf{F} = q \mathbf{v} \times \mathbf{B} $, where $ q $ is the charge of the particle, $ \mathbf{v} $ is the velocity vector, and $ \mathbf{B} $ is the magnetic field vector. For a proton, $ q = +1.6 \times 10^{-19} \, \mathrm{C} $.

Step 2: For part (a), the velocity vector $ \mathbf{v} $ is directed along the negative $ z $-axis ($ \mathbf{v} = -v \hat{z} $), and the magnetic field vector $ \mathbf{B} $ is directed along the positive $ x $-axis ($ \mathbf{B} = B \hat{x} $). Use the cross product $ \mathbf{v} \times \mathbf{B} $ to find the direction and components of $ \mathbf{F} $.

Step 3: Compute the cross product for part (a): $ \mathbf{v} \times \mathbf{B} = (-v \hat{z}) \times (B \hat{x}) $. Using the right-hand rule, the result is $ \mathbf{F} = q v B \hat{y} $, where $ \hat{y} $ is the positive $ y $-direction.

Step 4: For part (b), the velocity vector $ \mathbf{v} $ makes a 45° angle with the positive $ y $-axis in the $ y $-$ z $ plane. Decompose $ \mathbf{v} $ into components: $ \mathbf{v} = v \cos(45°) \hat{y} + v \sin(45°) \hat{z} $. The magnetic field vector remains $ \mathbf{B} = B \hat{x} $.

Step 5: Compute the cross product for part (b): $ \mathbf{v} \times \mathbf{B} = (v \cos(45°) \hat{y} + v \sin(45°) \hat{z}) \times (B \hat{x}) $. Using the distributive property and the right-hand rule, calculate the components of $ \mathbf{F} $ in the $ y $- and $ z $-directions. The final force vector will be expressed in component form.

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Magnetic Force on a Charged Particle

The magnetic force acting on a charged particle, such as a proton, moving in a magnetic field is given by the Lorentz force equation: F = q(v × B). Here, F is the magnetic force, q is the charge of the particle, v is its velocity vector, and B is the magnetic field vector. The direction of the force is determined by the right-hand rule, which states that if you point your thumb in the direction of the velocity and your fingers in the direction of the magnetic field, your palm will face the direction of the force.

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09:08

Magnetic Force Between Two Moving Charges

Cross Product

The cross product is a mathematical operation that takes two vectors and produces a third vector that is perpendicular to the plane formed by the original vectors. In the context of the magnetic force, the cross product v × B determines the direction of the force on the charged particle. The magnitude of the cross product is given by |v||B|sin(θ), where θ is the angle between the two vectors, which is crucial for calculating the force when the velocity is not perpendicular to the magnetic field.

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Vector (Cross) Product and the Right-Hand-Rule

Component Form of Vectors

Vectors can be expressed in component form, which breaks them down into their respective components along the coordinate axes. For example, a vector in three-dimensional space can be represented as F = (Fx, Fy, Fz), where Fx, Fy, and Fz are the components along the x, y, and z axes, respectively. This representation is essential for solving problems involving forces in different directions, allowing for easier calculations and clearer understanding of the vector's influence in each dimension.

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Vector Addition By Components

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