This paper examines the theory and computational methods behind predic
ting the linear unsteady motion of a ship with steady forward speed in
waves. The focus is on the wave exciting force impulse-response funct
ion as computed via the transient free-surface Green function. The lin
ear equation of motion for a ship in waves was first written in a rati
onal form. using the concept of the impulse-response function, by Cumm
ins (1962). Some years later King et al (1988) added the corresponding
wave exciting force in its appropriate convolution form. We extend th
is work by clarifying the definition of the impulsive incident wave in
following seas. and show it to be easily computable. Continuing trunc
ated calculations towards infinite time becomes especially important i
n following waves, and the method suggested by Bingham et al (1994) is
employed here. A novel filtering scheme is also introduced to prevent
short wave contamination of the solution. These developments allow ca
lculations in following waves to be presented for the first time using
this approach. The integral equation formulation of the linear seakee
ping problem is reviewed in some detail. and the relevant equations de
rived. Transient Haskind relations for bodies with forward speed are a
lso derived although, like their frequency-domain counterparts, these
are only approximate. Computed, first-order exciting forces and respon
se-amplitude operators for real ship geometries, in head and following
seas, are presented that demonstrate the usefulness of the transient
approach for the diffraction problem.