Instead of integrating the power pattern function directly and discounting the effect of the element factor to find the total radiated power of a line source, we show herein that an exact analytical expression for the radiated power can be obtained by singular knowledge of the source’s current distribution. The expression is found by using the Fourier principles associated with convolution integrals, autocorrelation integrals, Parseval’s Identity, and the Helmholtz operator in one dimension. Knowledge of the exact radiated power is used to find the expressions for directivity and radiation resistance. Furthermore, we show that the efficiency of the line source is explicitly a function of the relative proportion of two autocorrelation integrals. This newly developed theory is validated by considering large and small argument approximations in which closed-form results are readily known. Additional validation is obtained by comparing the exact result with the data obtained from numerical integration of the power pattern function. Examples associated with the half-wave dipole, cosine distribution, cosine-squared distribution, generalized dipole, triangular distribution, and the uniform distribution are provided. Other than the half-wave and generalized dipole solutions, we believe that the expressions obtained in this investigation have never been reported in the open literature. This is particularly true for the uniform line source in which the classical asymptotic result for the directivity (i.e., $2L/\lambda$ ) is shown to be deficient.