27.3. Identify: The force
on the particle is in the direction of the deflection of the
particle. Apply the right-hand rule to the directions of
and
. See if your thumb is in the direction of
, or opposite to that direction. Use
with
to calculate F.
Set Up: The
directions of
,
and
are shown in Figure
27.3.
Execute: (a) When
you apply the right-hand rule to
and
, your thumb points east.
is in this direction,
so the charge is positive.
(b) ![]()
Evaluate: If
the particle had negative charge and
and
are unchanged, the particle would be deflected toward the
west.

Figure 27.3
27.5. Identify: Apply
and solve for v.
Set Up: An
electron has
.
Execute: ![]()
Evaluate: Only
the component
of the magnetic field
perpendicular to the velocity contributes to the force.
27.7. Identify: Apply
.
Set Up:
, with
.
and
.
Execute: (a)
.
![]()
which is consistent
with
as given in the problem. There is no force component along
the direction of the velocity.
.
.
(b)
is not determined. No force due to this component of
along
; measurement of the force tells us nothing about ![]()
(c) ![]()
.
and
are perpendicular (angle is
.
Evaluate: The
force is perpendicular to both
and
, so
is also zero.
27.9. Identify: Apply
to the force on the proton and to the force on the electron. Solve
for the components of
.
Set Up:
is perpendicular to both
and
. Since the force on the proton is in the +y-direction,
and
. For the proton,
.
Execute: (a) For the proton,
so
. The force on the proton is independent of
. For the electron,
.
.
The magnitude of the force is
. Since
,
.
. The sign of
is not determined by measuring
the magnitude of the force on the electron.
.
.
.
is in the xz-plane
and is either at
from the +x-direction toward the
or
from the
toward the
.
(b)
.
.
. ![]()
.
.
. The force is in the xz-plane
and is directed at
from the
toward either the +z or
axis, depending on the
sign of
.
Evaluate: If the direction of the force on the first
electron were measured, then the sign of
would be determined.
27.53. (a)
Identify: Use Eq.(27.2) to relate ![]()
Set Up: The directions of
are shown in Figure
27.53a.
|
|
|
|
Figure 27.53a |
|
The directions of
are shown in Figure
27.53b.
|
|
|
|
Figure 27.53b |
|
Both pieces of information
taken together say that
is in the y-direction;
![]()
Execute: Use the information given about
to calculate ![]()
![]()
![]()
(b) ![]()
Evaluate:
is perpendicular
to
whereas only the
component of
perpendicular to
contributes to the
force, so it is expected that
as we found.
27.55. Identify: The sum of the magnetic, electrical, and gravitational forces must be zero to aim at and hit the target.
Set Up: The
magnetic field must point to the left when viewed in the direction of the
target for no net force. The net force is zero, so
and qvB – qE – mg = 0.
Execute: Solving for B gives
![]()
The direction should be perpendicular to the initial velocity of the coin.
Evaluate: This is a very strong magnetic field, but achievable in some labs.