ON ACOUSTIC-GRAVITY WAVES GENERATED BY AN IMPULSIVE POINT SOURCE IN THE MIDDLE ATMOSPHERE

In this paper the Row's¹ results are extanded from the special condition to the general condition. Besides the J_0\left(\omega_c \sqrt(t-\alpha)^2-t_0^2\right) H\left(t-\alpha-t_0\right), the corrective factorJ_1\left(\omega_c \sqrt(t-\alpha)^2-t_0^2\right) H\left(t-\alpha-t_0\right) is gained. The J_0\left(\omega_c \sqrtt^2-t_0^2\right) H\left(t-t_0\right) of formula (12) in row (1967)¹ must be changed into J_0\left(\omega_c \sqrt(t-\alpha)^2-t_0^2\right) H\left(t-\alpha-t_0\right) where α is a retarded time. The (1ω_ct₀)ⁿ indicates that: when to is greater, the corrective effect is less; when T_c is longer, the corrective effect is more.