It is given that the velocity profile is
Uu=(1−hy)[1−3hy(1−n+12hh1)]
and load
P=h22(n−1)26μUL2[lnn−n+12(n−1)]
where n=h1/h2
Force on the slider in the x-direction is
Fs=∫0Lτsdx(1)cosαcosα+∫0L(p−p0)cosαdx(1)sinα
=∫0Lτsdx+tanα∫0L(p−p0)dx
Now, τs=−μ(∂y∂u)y=h
and u=U(1−hy)[1−3hy(1−n+12⋅hh1)], so we get
∂y∂u=U[−h1−3(h1−h22y)(1−n+12⋅hh1)]
∴τs=−μU[−h1+h3(1−n2⋅h1)]
=μU[−h2+n+16⋅h2h1]
Also, h=h1−(h1−h2)Lx
∴dh=−Lh1−h2dx
Thus, ∫0Lτsdx=h1−h2L∫h2h1τsdh
=h1−h2μLU∫h2h1(−h2+n+16⋅h2h1)dh
=h1−h2μUL(−2lnh−n+16⋅hh1)h2h1
=h2(n−1)μUL[−2lnn−n+16h1(h11−h21)]
=h2(n−1)μUL[−2lnn+n+16(n−1)]
Also, load P=∫0L(p−p0)cosαdxcosα (neglecting contribution of τs to load; α is small)
∴ Fs=∫0Lτsdx+tanα(P)
or Fs=∫0Lτsdx+tanα(P)Fs=h2(n−1)μUL(−2lnn+n+16(n−1))+[Lh1−h2]×
h22(n−1)26μUL2(lnn−n+12(n−1))
=h2(n−1)μUL(4lnn−n+16(n−1))
Now the force on the guide is
FG=∫0LτGdx
But τG=−μ(∂y∂u)y=0
=μU[h1+h3(1−n+12⋅hh1)]
The expression is τG=μU[h4−n+16⋅h2h1]
∴ FG=∫0LτGdx
=h1−h2L∫h2h1τGdh (as before)
=h2(n−1)μUL∫h2h1(h4−n+16⋅h2h1)dh
=h2(n−1)μUL[4lnn+n+16h1(h11−h21)]
=h2(n−1)μUL[4lnn−n+16(n−1)]
which is the same as Fs.