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Introductory Physics Volume Two

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4.7 Homework 93<br />

Imagine the closed loop to be divided up into many d ⃗ l i , approximated<br />

by a many-sided polygon:<br />

B<br />

I<br />

So, the integral is just the limit of a sum over all of the small segments:<br />

∮<br />

d ⃗ l × ⃗ B = d ⃗ l 1 × ⃗ B + d ⃗ l 2 × ⃗ B + · · ·<br />

= (d ⃗ l 1 + d ⃗ l 2 + · · ·) × B ⃗ (∮ )<br />

= d ⃗ l × B ⃗<br />

⃗B is outside the integral because it is constant. The vector sum indicated<br />

by the integral in the last line must vanish since the vectors form<br />

a close polygon; graphical vector addition yields zero. Thus,<br />

∮<br />

⃗F = I d ⃗ l × B ⃗<br />

(∮ )<br />

= I d ⃗ l × B ⃗<br />

= 0<br />

§ 4.7 Homework<br />

⊲ Problem 4.7<br />

Consider an electron near the equator. In which direction does it tend<br />

to deflect by the magnetic field of the earth if its velocity is directed<br />

(a) downward, (b) northward, (c) westward, or (d) southeastward?<br />

⊲ Problem 4.8<br />

An electron moving along the positive x axis perpendicular to a magnetic<br />

field experiences a magnetic deflection in the negative y direction.<br />

What is the direction of the magnetic field?<br />

⊲ Problem 4.9<br />

An electron in a uniform electric and magnetic field has a velocity of<br />

1.2×10 4 m s in the positive x direction and an acceleration of 2.0×1012 m s 2

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