Using C3→C3−C2 and C2→C2−C1, we can write
Δh2=∣∣
∣
∣∣tanx[tan(x+h)−tanx]/h[tan(x+2h)−tan(x+h)]/htan(x+2h)[tanx−tan(x+2h)]/h[tan(x+h)−tanx]/htan(x+h)[tan(x+2h)−tan(x+h)]/h[tanx−tan(x+2h)]/h∣∣
∣
∣∣
But
limh→0tan(x+h)−tanxh
=limh→01hsin(x+h)cosx−cos(x+h)sinxcos(x+h)cosx
=limh→01hsinhcos(x+h)cosx=sec2x or (use ddx(tanx)=sec2x)
Similarly, =limh→0tan(x+2h)−tan(x+h)h=sec2x
and =limh→0tanx−tan(x+2h)h=−2sec2x
Thus,
Δ(x)h2=∣∣
∣
∣∣tanxsec2xsec2xtanx−sec2xsec2xtanxsec2x−2sec2x∣∣
∣
∣∣ =∣∣
∣
∣∣tanxsec2xsec2x0−3sec2x000−3sec2x∣∣
∣
∣∣
=9tanxsec4x [Using R2→R2−R1 and R3→R3−R1]
So limh→0√3Δ(π/3)h2=9×3×24=216