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Screw Jack Design
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Self-locking & overhauling of screw

T=Wtan(ϕα).dm2 --------------(1)

Where T=torque required to lower the screw

ϕ = angle of friction

α = helix angle

W=load to be lifted

dm=mean diameter

The torque required to lower the screw is given in equation (1). In equation (1) if ϕ<α then the torque required to lower the load will be negative (-ve). In other words, load will start moving downward without application of any torque such condition is known as overhauling of the screw

If ϕ>α, then torque required to lower the load will be positive (+ve) indicating that an effort is applied to lower the load. Such a screw is called self-locking screw.


Q. Design a screw jack to lift load of 250 KN and having a maximum lift of 270 mm select proper material and draw a proportional sketch

enter image description here

Selection of material for screw

The screw is under compression due to steady load but undergoes tension when rotated. It is subjected to buckling also when the load is raised through the max lift. Therefore from strength consideration, let us select steel as the material of the screw.

Let us take C40

Selection of FOS

As screw is subjected to both compressive as well as torsional shear stress and to account for high-stress concentration in threads.

Hence consider higher FOS

Take n=4 based on σy value

Permissible stresses for screw From PSG 1.9

Take σy=330 N/mm2

σt=σc=σyFOS=3304=82.5 N/mm2

Take σc=82 N/mm2

By maximum shear stress theory

e=0.5×σyFOS

e=41.25 N/mm2

Take e=41 N/mm2

Selection of material for nut

Considering nut material like cast iron which is easy to manufacture and cheap C.I also wear rest.

Taking Grey C.I. i.e. GCI 20

Form PSG 1.4

σ4=200 N/mm2

Selection of FOS

As the material is brittle and to account for high-stress concentration threads, consider high FOS=6 based on σu

Permissible stress for nut

σt=σuFOS=2006=33.33 N/mm2

Considering e=σt=33 N/mm2

As compressive strength of C.I. is more than tension strength consider σc=2σt=66 N/mm2

Bearing stress selection

from PSG 7.8.7

From screw and C.I. nut combination

σbr=80 Kgf/cm2

=80×10 N/cm2

=800×102 N/mm2

=8 N/mm2

Design of screw

Consider the compressive failure of the screw

σc=WAc

Ac=2.50×10382

Ac=3.0487×103 mm2

Ac=π4d2c where dc=62.3 mm

Above diameter is based on only direct compressive stress but the actual screw is also subjected to torsional shear stress. Hence to take into account the effect of torsional shear stress take a diameter 30% greater than the above value

dc=1.3×62.3=80.9 mm

Ac=π4d2c=5151.72 mm2

from PSG 5.7 and 5.71 selecting normal series we can provide a standard screw of the cover area Ac

Take Ac=5411 mm2

nominal diameter

do=95 mm

cover dia dc=23 mm

pitch dia p=12 mm

Mean dia dm = d0+dc2=39 mm

helix angle is selected by a single shot

tan(α) = pitchπdm

α=tan1(12π×89)

α=2.45\degree

Selecting the angle of friction

ϕ =6 to 8\degree from PSG 7.87 as ϕ >α, self-locking will be provided

frictional torque acting on the screw, T1=P×dm2=wtan(ϕ+α)dm2

=250×103tan(6+2.45)892

T1=1.65×106 Nmm

shear stress developed in screw '

e=16T1πd3c

as TIp=er

Ip=π64d4+π64d4=π32d4

e=16×1.65×106π×832

e=14.89 N/mm2

the maximum principal stress in screw

σcmax = 12[σc+(σ2c+4e2)]

where σc is the direct compressive stress developed in the screw

σc=wAc = 250×1035411

σc=46.20 N/mm2

σcmax=12[46.20+(46.20)2+4(14.69)2]

σcmax=50.47 N/mm2

σcmax=50.47<σc=82 N/mm2

screw is safe in compressive stress Maximum shear stress developed in the screw,

τmax = 12[(σ2c+4τ2)]

τmax = 12[((46.2)2+4(14.69)2)]

τmax=27.37 N/mm2<τ=41 N/mm2

screw is safe in shear stress

Let us check screw for buckling

Assume the nut is a solid

from PSG 7.87, for solid nut

Ratio Hdp= 2 where H = 2×dm=2×89=178 mm

Length of the screw for buckling purpose i.e. unsupport length of screw

L= lifting height +H/2

L=270+178/2=359 mm

Considering screw as a short column whose one end is fixed to nut and other end is free

The end fixing coefficient is n=0.25 from PSG 6.8 using Johnson's parabolic formula,

Pc=acσy[1σy4nπ2E(tk)2]

where K= radius of gyration

K=0.25×dc=0.25×83=20.75 mm

E=2.1×105N/mm2

Pc=5411×330[13304(0.25)π2×2.1×105(35920.75)2]

Pc=1.7×106 N>250×103 N

As value of buckling load is greater than the load at which screw is designed so there is no chance of screw to buckle hence it is safe.

Design of nut

We know nominal dia of screw is d0=95 mm Taking d=d0+10 mm=105 mm

Considering crushing failure of nut column W=π4(D2d2)×σE

D=125.88 mm

Let n be the no of threads in engagement

height of the nut ,

H=pitch×n

178=p×n=12×n

n=14.83 take n=15

Let us check bearing stress developed in nut threads

W = π4(d20d2c)×n×σbr

250×103=π4(952832)×15×σbr

Nut threads fails in bearing stress.

Increase no of threads in engagement

Taking n=20

W = π4(d20d2c)×20×σbr

σbr=7.45 N/mm2<σbr=8 N/mm2

enter image description here

nut threads are safe

Let us check shear stress developed in nut threads W = π× d_0×t_1×n×T induced

t_1 = \frac{pitch}{2}

\therefore 250×10^3 = π×95×6×20×T_{\text{induced}}

T_{\text{induced}}=6.98 < T_{\text{nut}} =33 \therefore nuts and threads are safe

Let us check shear stress developed in the nut threads

\therefore W = π \times d_0\times t_1\times n \times T_{\text{induced}}

t_1 =\frac{pitch}{2}= 12/2 =6mm

\therefore 250×10^3 = π×6×20×T_{\text{induced}}

T_{\text{induced}}=6.98\ N/mm^2\ltT_{\text{nut}}=33

\therefore nuts and threads are safe in shear.

Now calculate 't’ by considering the shear failure of nut column

W= π×d×t×T

250\times 10^3=\pi \times 105 \times \ t \times \ 33

t=22.93 \ mm

Take t=23\ mm

Height of nut H = pitch×n H = 240\ mm

Design of handle

The diameter of the head (D_1) on top of the screw is taken 1.5 to 1.7 of d_0

\therefore D_1 = 1.6× d_0 =1.6×95 = 152\ mm D_2 = 0.5 D_1 = 76mm

Then find the torque required to overcome friction at the top of the screw assuming uniform pressing

T_2 = \frac{2}{3} \mu N\frac{R_1^3-R_3^3}{R_1^2-R_2^2}

R_1 =D_1/2 =152/2=76

R_2 =D_2/2=76/2=38

Assuming coefficient of friction \mu = tan\phi

\mu = 0.1

T_2 = \frac{2}{3} \mu N\frac{R_1^3-R_3^3}{R_1^3-R_2^3}

T_2=\frac{2}{3} \times 0.1 \times 250 \times 10^3 [\frac{76^3 - 38^3}{76^2 - 38^2}]

= 1.47×10^6 \ N-mm

\therefore Total torque to lift load

T=T_1+T_2 = 1.65 \times 10^6 +1.47 \times 10^6 = 3.12×10^6\ N-mm

Let L_n be the length of the handle T = F \times L_n L_n = T / F = 7.8m

Generally length of handle is 1m

Maximum bending moment will be M = \text{force} \times {Length} =400×1000

Consider material of handle C40 and FOS 2 \sigma_c = \sigma_{\text{bending}}= \frac{\sigma_y}{FOS}=330/2=165\ N/mm^2

165 = \frac{400×10^3}{\frac{π}{32}×d_h^3}

d_h = 29.12\ mm

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