The Definition of B — Question 1

Section 28-2 · Physics pages 4492–4493

Question 1 A magnetic cross product fixes both the force components and their perpendicularity A particle of charge q = 2.00 microcoulomb has velocity (3ˆx + 4ˆy)105 m/s in a uniform field .200ˆz tesla. No other force acts. x y⃗ v⃗ F to determine⃗ B = Bˆz Schematic; labels, not drawing lengths, specify the data. (a) Find the magnetic-force vector and its magnitude. (b) Calculate the instantaneous power and explain the consequence for kinetic energy.
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Question 1 - Solution A magnetic cross product fixes both the force components and their perpendicularity x y⃗ v⃗ F to determine⃗ B = Bˆz (a) Method and calculation⃗ F = q⃗v ×⃗B = qB(vyˆx −vxˆy).⃗ F = (.160ˆx −.120ˆy) N, F = .200 N. (b) Interpretation and further calculation P =⃗F ·⃗v = (.160)(3 × 105) −(.120)(4 × 105) = 0. dK dt = 0 ⇒K = constant. Physical check The force changes the direction of velocity, not its magnitude, in a purely magnetic field.

Question 1

A magnetic cross product fixes both the force components and their perpendicularity

A particle of charge q=2.00q=2.00 microcoulomb has velocity (3x̂+4ŷ)105(3\hat x+4\hat y)10^5 m/s in a uniform field .200ẑ.200\hat z tesla. No other force acts.

Diagram shown in the original SVG worksheet.

  1. Find the magnetic-force vector and its magnitude.

  2. Calculate the instantaneous power and explain the consequence for kinetic energy.

Question 1 - Solution

A magnetic cross product fixes both the force components and their perpendicularity

Diagram shown in the original SVG worksheet.

(a) Method and calculation

F→=qv→×B→=qB(vyx̂−vxŷ).\vec F=q\vec v\times\vec B=qB(v_y\hat x-v_x\hat y).F→=(.160x̂−.120ŷ)N,F=.200N.\vec F=(.160\hat x-.120\hat y)\,\mathrm N,\quad F=.200\,\mathrm N.

(b) Interpretation and further calculation

P=F→⋅v→=(.160)(3×105)−(.120)(4×105)=0.P=\vec F\cdot\vec v=(.160)(3\times10^5)-(.120)(4\times10^5)=0.dKdt=0⇒K=constant.\frac{dK}{dt}=0\Rightarrow K=\text{constant}.

Physical check

The force changes the direction of velocity, not its magnitude, in a purely magnetic field.