We study the Kondo effect in a quantum dot coupled to two noncollinear ferromagnetic leads. First, we study the spin splitting δε = ε↓ - ε↑+ in the quantum dot by the tunnel coupling to the ferromagnetic leads, using the Poor man's scaling method. The spin splitting takes place in an intermediate direction between magnetic moments in the two leads. δε ∝ p cos(θ/2), where p is the spin polarization in the leads and θ is the angle between the magnetic moments; spin splitting is maximal in the parallel alignment of two ferromagnets (θ = 0) and minimal in the antiparallel alignment (0 = π). Second, we calculate the Kondo temperature TK The scaling calculation yields an analytical expression of TK as a function of θ and p, T K(θ,P), when δε << TK. When δε is relevant, we evaluate TK(δε,θ,P) using the slave-boson mean-field method. The Kondo resonance is split into two by finite δε, which results in the suppression of Kondo effect.