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Introductory Physics Volume Two

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2.8 Homework 53<br />

add up potential due to each small section making up the entire line:<br />

∫<br />

x+L ∫ Q<br />

V (x) = dV ′ 1<br />

L<br />

=<br />

dx′<br />

4πɛ 0 x ′<br />

x<br />

= Q ( ) x + L<br />

4πɛ 0 L ln x<br />

Let’s check that this gives the expected result for L → 0, which will<br />

result in Q being a point charge. We need the limit:<br />

( ) (<br />

x + L<br />

lim ln = lim ln 1 + L )<br />

≈ L<br />

L→0 x L→0 x x<br />

So<br />

lim V (x) = Q<br />

L→0 4πɛ 0 L · L<br />

x = Q<br />

4πɛ 0 x ,<br />

which is indeed the electric potential a distance x from a point charge<br />

Q.<br />

§ 2.8 Homework<br />

⊲ Problem 2.16<br />

Through what potential difference would an electron need to be accelerated<br />

for it to achieve a speed of 40% of the speed of light, starting<br />

from rest?<br />

⊲ Problem 2.17<br />

How much work is required to move one mole of electrons from a region<br />

where the electric potential is 9V to a region where the electric potential<br />

is -5V?<br />

⊲ Problem 2.18<br />

An electron moving along the x axis has an initial speed of 2.7×10 6 m s<br />

at<br />

the origin. Its speed is reduced to 1.4 × 10 5 m s<br />

at the point x = 2.0cm.<br />

Calculate the potential difference between the origin and this point.<br />

Which point is at the higher potential?<br />

⊲ Problem 2.19<br />

In Rutherford’s experiments alpha particles (charge +2e, mass 6.6 ×<br />

10 −27 kg) were fired at a gold nucleus (charge +79e). An alpha particle<br />

initially very far from the gold nucleus is fired at 2.0 × 10 7 m s<br />

directly<br />

toward the center of the nucleus. How close does the alpha particle get<br />

to this center before turning around?<br />

⊲ Problem 2.20<br />

Show that the amount of work required to assemble four identical<br />

charges Q at the corners of a square of side s is 5.41kQ 2 /s.

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