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Tài liệu shi20396 chương 16 pdf
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Mô tả chi tiết
Chapter 16
16-1
(a) θ1 = 0°, θ2 = 120°, θa = 90°, sin θa = 1, a = 5 in
Eq. (16-2): Mf = 0.28pa(1.5)(6)
1
120°
0°
sin θ(6 − 5 cos θ) dθ
= 17.96pa lbf· in
Eq. (16-3): MN = pa(1.5)(6)(5)
1
120°
0°
sin2 θ dθ = 56.87pa lbf· in
c = 2(5 cos 30◦) = 8.66 in
Eq. (16-4): F = 56.87pa − 17.96pa
8.66 = 4.49pa
pa = F/4.49 = 500/4.49 = 111.4 psi for cw rotation
Eq. (16-7): 500 = 56.87pa + 17.96pa
8.66
pa = 57.9 psi for ccw rotation
A maximum pressure of 111.4 psioccurs on the RH shoe for cw rotation. Ans.
(b) RH shoe:
Eq. (16-6): TR = 0.28(111.4)(1.5)(6)2(cos 0◦ − cos 120◦)
1 = 2530 lbf· in Ans.
LH shoe:
Eq. (16-6): TL = 0.28(57.9)(1.5)(6)2(cos 0◦ − cos 120◦)
1 = 1310 lbf· in Ans.
Ttotal = 2530 + 1310 = 3840 lbf· in Ans.
(c) Force vectors not to scale
x
y
Fy
Ry
Rx
R
Fx
F
Secondary
shoe
30 y
x
Rx
Fy
Fx
F
Ry
R
Primary
shoe
30
shi20396_ch16.qxd 8/28/03 4:01 PM Page 407
408 Solutions Manual • Instructor’s Solution Manual to Accompany Mechanical Engineering Design
RH shoe: Fx = 500 sin 30° = 250 lbf, Fy = 500 cos 30° = 433 lbf
Eqs. (16-8): A =
1
2
sin2 θ
120◦
0◦
= 0.375, B =
θ
2 − 1
4
sin 2θ
2π/3 rad
0
= 1.264
Eqs. (16-9): Rx = 111.4(1.5)(6)
1 [0.375 − 0.28(1.264)] − 250 = −229 lbf
Ry = 111.4(1.5)(6)
1 [1.264 + 0.28(0.375)] − 433 = 940 lbf
R = [(−229)2 + (940)2
]
1/2 = 967 lbf Ans.
LH shoe: Fx = 250 lbf, Fy = 433 lbf
Eqs. (16-10): Rx = 57.9(1.5)(6)
1 [0.375 + 0.28(1.264)] − 250 = 130 lbf
Ry = 57.9(1.5)(6)
1 [1.264 − 0.28(0.375)] − 433 = 171 lbf
R = [(130)2 + (171)2
]
1/2 = 215 lbf Ans.
16-2 θ1 = 15°, θ2 = 105°, θa = 90°, sin θa = 1, a = 5 in
Eq. (16-2): Mf = 0.28pa(1.5)(6)
1
105°
15°
sin θ(6 − 5 cos θ) dθ = 13.06pa
Eq. (16-3): MN = pa(1.5)(6)(5)
1
105°
15°
sin2 θ dθ = 46.59pa
c = 2(5 cos 30°) = 8.66 in
Eq. (16-4): F = 46.59pa − 13.06pa
8.66 = 3.872pa
RH shoe:
pa = 500/3.872 = 129.1 psi on RH shoe for cw rotation Ans.
Eq. (16-6): TR = 0.28(129.1)(1.5)(62)(cos 15° − cos 105°)
1 = 2391 lbf· in
LH shoe:
500 = 46.59pa + 13.06pa
8.66 ⇒ pa = 72.59 psi on LH shoe for ccw rotation Ans.
TL = 0.28(72.59)(1.5)(62)(cos 15° − cos 105°)
1 = 1344 lbf · in
Ttotal = 2391 + 1344 = 3735 lbf · in Ans.
Comparing this result with that of Prob. 16-1, a 2.7% reduction in torque is achieved by
using 25% less braking material.
shi20396_ch16.qxd 8/28/03 4:01 PM Page 408