184 MECHANICAL ENGINEERING PRINCIPLES
a 2
a 2
a 1
T 2
T 1
F 1 F 2
R 2
R 1
(a) (b)
Figure 16.3
16.2 Motion on a curved banked track
Problem 2. A railway train is required to
travel around a bend of radiusrat a uniform
speed ofv. Determine the amount that the
‘outer’ rail is to be elevated to avoid an
outward centrifugal thrust in these rails, as
shown in Figure 16.4.
L
q
R 1
R 2
Outer
rail
mg
O
h
r CG CF
Figure 16.4
To balance the centrifugal force:
(R 1 +R 2 )sinθ=CF=
mv^2
r
from which, sinθ=
mv^2
r(R 1 +R 2 )
LetR=R 1 +R 2
Then sinθ=
mv^2
rR
( 16. 9 )
Resolving forces vertically gives:
Rcosθ=mg
from which, R=
mg
cosθ
( 16. 10 )
Substituting equation (16.10) into equation (16.9)
gives:
sinθ=
mv^2
rmg
cosθ
Hence tanθ=
v^2
rg
(
since
sinθ
cosθ
=tanθ
)
Thus, the amount that the outer rail has to be
elevated to avoid an outward centrifugal thrust on
these rails,
θ=tan−^1
(
v^2
rg
)
( 16. 11 )
Problem 3. A locomotive travels around a
curve of 700 m radius. If the horizontal
thrust on the outer rail is 1/40thof the
locomotive’s weight, determine the speed of
the locomotive (in km/h). The surface that
the rails are on may be assumed to be
horizontal and the horizontal force on the
inner rail may be assumed to be zero. Takeg
as 9.81 m/s^2.
Centrifugal force on outer rail
=
mg
40
Hence,
mv^2
r
=
mg
40
from which, v^2 =
gr
40
=
9. 81 × 700
40
= 171 .675 m^2 /s^2
i.e. v=
√
171. 675 = 13 .10 m/s
=( 13. 10 × 3. 6 )km/h
i.e.the speed of the locomotive,v= 47 .17 km/h