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Exact(10)
We then obtain, (10) where J1 is a Bessel function of the first order.
where ρ ( y ) = y − [ y ] − 1 2 is the Bernoulli function of the first order.
where ρ ( y ) = y − [ y ] − 1 2 is a Bernoulli function of the first order.
where E 1 ( z ) = ∫ z ∞ e − t t dt (24). is the exponential integral function of the first order [25].
Note that, according to the condition of Theorem 5.1, the Cauchy function of the first order equation (5.3) is positive for 0 ≤ s ≤ t ≤ + ∞.
where we set p 2 i ( s ) = 0 for s < 0, implies the positivity of the Cauchy function of the first order equation (5.3) (see Theorem 15.7, p.358 in [28]).
Similar(50)
The solution to the Goursat system is related to the solution of a simpler, explicitly solvable Goursat system through a suitable infinite series of powers of partial derivatives which is summed explicitly in terms of special functions, including Bessel functions and the generalized Marcum Q-functions of the first order.
where J 1 and Y 1 are the Bessel functions of the first order.
On the other hand, a performance, along with its physical trappings, falls under the heading of interpretation, commonly held to be a creative function of the second order, though it does not have to be.
The formula of the peak factor is simplified to a function of the third order moment (skewness) considering the spatial correlation of wind velocity, the resonance response and the background response.
where κ is the Rician factor, and I0 represents the modified Bessel function of the zeroth order and first kind.
More suggestions(14)
function of the first wall
function of the first term
function of the first player
function of the 6th order
function of the 24th order
function of the first type
function of the first level
function of the same order
function of the fifth order
function of the temporal order
function of the right order
function of the third order
function of the optimum order
function of the infinite order
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