Although a great number of attempts have been made to evaluate the canopy photosynthesis, almost all of them have mainly been devoted to calculations of photosynthesis of horizontally uniform canopies such as well grown rice, maize, wheat and soybean field. Hence it seems that less information is obtained on light environment and photosynthesis of a hedgerow type canopy usually adopted for the cultivation of horticultural crops. This paper presents an approach to the light environment within hedgerow type canopies, particularly the penetration of direct sunlight into them. A silhouette method was used to obtain phytometrical data of cucumber canopies (var. Ougon) raised in a vinylhouse. The phytometrical measurements were repeated at an interval of one week during the period from April 25 to May 16 in 1973.In the calculation of penetration of direct solar radiation into the hedgerow type canopy, the cross section of the cucumber row was divided into two parts: the first part is irradiated by direct sunlight penetrated through the top surface of the canopy and the second by sunlight penetrated through the side surface of the canopy. Geometrical characteristics for the first part can be obtained by the ordinary method (Eqs. 2-4, c.f., UCHIJIMA et al., 1968).In order to assess the geometrical characteristics (effective leaf area projection function GL←, extinction coefficient of direct sunlight kd←) of the second part of the canopy, the rectangular system (x, y, z) set in parallel with the cross section of row is transformed to a new system x′=z, y′=y, z′=x by rotating only the z-axis at 90°. Extinction coefficient of direct sunlight in the second part kd← is given as a function of the angle of incidence of solar rays on the side surface of the crop rows, which is defined by both the sun and row directions. Numerical experiments are made to determine the dependence of the extinction coefficient kd← on the directions of the sun and row. Results obtained are summarized as follows:(1) A following simple relation was obtained between the leaf area of cucumber crop A and the product of leaf length l (from joint of leaf-stalk to leaf-tip) and leaf width w, and used to determine non-destructively the canopy structure of cucumber crop:A=0.937(l⋅w)-9. (cm2)(2) Inclination angle of cucumber leaves increases with the depth of the crop layer, viz., with leaf age, and the foliage inclination angle of leaves (βL) also increases with the progress of plant stages (early stage-14°, middle stage-21-24°). It seems that the azimuthal distribution of leaf area shows predominance in a direction perpendicular to the row direction (E45°S-W45°N)(Fig. 3).(3) The effective leaf area projection function for the whole stand GL↓ calculated from Eq. (2) increases with increasing sun altitude ho, and its dependence on ho agrees fairly well with the theoretical result for a horizontal-leaved cancopy (ROSS, 1970). The value of GL↓ changes a little with depth of the crop layer (Fig. 4).(4) Extinction coefficient kd↓ of direct solar radiation in the first part of the cucumber canopy is shown as a function of sun altitude (Fig. 8). Diurnal changes of extinction coefficient kd← calculated from the following equations for the four rows with different direction (N-S, E-W, E45°S-W45°N, E45°N-W45°S) show different features with the time of a year (Fig. 6, 7).kd(bn, i)←=soc i GL(bn, θo)←