log 2 ⁡ ( 4 ) = 2 {\displaystyle \log _{2}(4)=2} 2 Gosper curve Its boundary is the Gosper island.

log 3 ⁡ ( 2 ) {\displaystyle \log _{3}(2)} 0.6309 Cantor set Built by removing the central third at each iteration.

log 2 ⁡ ( 8 ) = 3 {\displaystyle \log _{2}(8)=3} 3 3D Hilbert curve A Hilbert curve extended to 3 dimensions.

log 2 ⁡ ( 4 ) = 2 {\displaystyle \log _{2}(4)=2} 2 H-fractal Also the Mandelbrot tree which has a similar pattern.

log 3 ⁡ ( 7 ) {\displaystyle \log _{3}(7)} 1.7712 Hexaflake Built by exchanging iteratively each hexagon by a flake of 7 hexagons.

log 2 ⁡ ( 4 ) = 2 {\displaystyle \log _{2}(4)=2} 2 2D Greek cross fractal Each segment is replaced by a cross formed by 4 segments.

log 2 ⁡ ( 8 ) = 3 {\displaystyle \log _{2}(8)=3} 3 3D Moore curve A Moore curve extended to 3 dimensions.

is equivalent to n A n B {\displaystyle n_{A}n_{B}}

Each of the said Ln dispatcher aggregates mulitple Ln-1 dispatchers to dispatch the message to be transmitted.

The slope of a graph of ln ⁡ v {\displaystyle \ln v} as a function of ln ⁡ [ A ] {\displaystyle \ln[A]} then corresponds to the order x with respect to reactant A.[9][10]

Ln), wherein each work station (L1, L2, L3 ...

log 3 ⁡ ( 5 ) {\displaystyle \log _{3}(5)} 1.4649 Vicsek fractal Built by exchanging iteratively each square by a cross of 5 squares.

The graph slope of ln r as a function of ln[A] corresponds to the order x concerning reactant A.

Imagine a constant of the natural logarithm, C = ln |C|, then:ln|xy| = ln|C|, where xy = C.

The mole fraction of Ln in relation to the total of Y and Ln in such an instance is preferably no greater than 0.2.