(a) From charle's law: V∝T ⇒V=k1T (at cons. P) ⇒(dTdV)P=k1=0
(b) From GayLussac's law: P∝T (at cons. V ) ⇒P=K2T ⇒(dTdP)V=k2=0
(c) For an ideal gas, change in internal energy is zero at constant temperature. (dU)T=0 ⇒(dVdU)T=0
(d) ΔU=nCVΔT (at cons. V ) ⇒(dTdU)V=nCV=0