Fueled by the hydrolysis of ATP, the motor protein kinesin literally walks on two legs along the biopolymer microtubule. The number of accidental backsteps that kinesin takes appears to be much larger than what one would expect given the amount of free energy that ATP hydrolysis makes available. This is puzzling as more than a billion years of natural selection should have optimized the motor protein for its speed and efficiency. But more backstepping allows for the production of more entropy. Such entropy production will make free energy available. With this additional free energy, the catalytic cycle of the kinesin can be speeded up. We show how measured backstep percentages represent an optimum at which maximal net forward speed is achieved. Processive motor proteins are among the tiniest engines known to man. These proteins utilize the energy of ATP hydrolysis to literally walk along a biopolymer [1]. In a living cell they help maintain organization by transporting cargo, like organelles or vesicles filled with chemicals.Already one and a half decade ago the stepping of the processive motor protein kinesin was made visible on the nanometer scale with optical tweezers [1]. Early communications [2,3] reported that 5% to 10% of all steps of kinesin were backward. But smaller fractions were described later on as methods and materials improved and better resolutions were achieved; Ref.[4] gave 1/220 and Ref.[5] gave 1/802. Theoreticians have always been interested in backstep fractions as they can help verify stochastic models. However, throughout the literature backstepping has implicitly and explicitly been seen as an occasional malfunction of the stepping motor protein. In this Letter we will show how, in the Brownian environment of the motor protein, a "well-tuned" backstep fraction can actually help the motor speed up. We will show how the backstep fraction that leads to the highest net speed can be evaluated and how the resulting expression contains no freely adjustable parameters. Finally, we will see how the experimentally established backstep fraction of kinesin is close to our predicted optimal backstep fraction.The operation of an ion pump is generally modeled with a cycle as depicted in Fig. 1. At equilibrium the product of the forward rates, k 12 × k 23 × ... × k n1 , equals the product of the backward rates, k 21 × k 32 × ... × k 1n , and no net cycling occurs. To drive the protein through the sequence of states, S 1 , S 2 ... S n , a driving energy is necessary [6]. Such energy comes available if one of the steps involves the binding of ATP and if the protein, in subsequent steps, catalyzes the hydrolysis of the bound ATP. Eventually the remaining ADP and an inorganic phosphate have to be released so as to complete the cycle and to put the protein again in a state in which it can bind a new ATP. Under physiological conditions the hydrolysis of ATP makes G ATP = 22 k B T units of free energy available. In the course of a cycle of a membrane pump like Na,K-ATPase, part of G ATP is utilized to bind, t...