logx has no direct formula so it must be u (rule (i) of §11.7.5); the other three have u=xn for n≥2, so Bernoulli's formula (§11.7.6) is the efficient route.
Part (i): xlogx. Take u=logx,dv=xdx⇒du=x1dx,v=2x2.
∫xlogxdx=2x2logx−∫2x2⋅x1dx=2x2logx−21∫xdx=2x2logx−4x2+c.
Check: dxd[2x2logx−4x2]=xlogx+2x−2x=xlogx ✓.
Part (ii): 27x2e3x. Bernoulli with u=x2(u′=2x,u′′=2), dv=e3xdx(v=3e3x,v1=9e3x,v2=27e3x):
∫x2e3xdx=x2⋅3e3x−2x⋅9e3x+2⋅27e3x+c=3x2e3x−92xe3x+272e3x+c.
Multiplying by 27: 27∫x2e3xdx=9x2e3x−6xe3x+2e3x+c.
Check: dxd[9x2e3x−6xe3x+2e3x]=18xe3x+27x2e3x−6e3x−18xe3x+6e3x=27x2e3x ✓.
Part (iii): x2cosx. Bernoulli with u=x2(u′=2x,u′′=2), dv=cosxdx(v=sinx,v1=−cosx,v2=−sinx):
∫x2cosxdx=x2sinx−2x(−cosx)+2(−sinx)+c=x2sinx+2xcosx−2sinx+c.
Check: dxd[x2sinx+2xcosx−2sinx]=2xsinx+x2cosx+2cosx−2xsinx−2cosx=x2cosx ✓. …