We investigate the nonlinear regime of charge and energy transport through Coulomb-blockaded quantum dots. We discuss crossed effects that arise when electrons move in response to thermal gradients (Seebeck effect) or energy flows in reaction to voltage differences (Peltier effect). We find that the differential thermoelectric conductance shows a characteristic Coulomb butterfly structure due to charging effects. Importantly, we show that experimentally observed thermovoltage zeros are caused by the activation of Coulomb resonances at large thermal shifts. Furthermore, the power dissipation asymmetry between the two attached electrodes can be manipulated with the applied voltage, which has implications for the efficient design of nanoscale coolers. [8,9]. Importantly, nonlinearities and rectification mechanisms that lead to the phenomena reported in Refs. [1,2] can be more easily tested in small conductors with strongly energy-dependent densities of states [3,[10][11][12][13][14][15][16][17][18][19][20][21][22]. We emphasize that there is a close relation between the thermopower of a junction and its heat dissipation properties, as demonstrated in Refs. [23][24][25] for the linear regime of transport. Therefore, ascertaining the conditions under which thermovoltages acquire a significant nonlinear contribution has broader implications for power generation and cooling applications [26].We begin our discussion by noticing that vanishing thermovoltages imply the existence of zero thermocurrent states. Unlike voltage-driven currents, which have a definite sign for a bias voltage V > 0 and never cross the V axis for normal conductors (an exception is the Hall resistance of an illuminated two-dimensional electron gas [27]), electric transport subjected a thermal gradient θ displays regions of positive or negative thermocurrents depending on the thermopower sign (positive for electronlike carriers, negative for holelike ones [28]). Nevertheless, this is not sufficient for the thermocurrent to cross the θ axis since the thermopower is constant in linear response. Therefore, a strongly negative