- #1
Jenab2
- 85
- 22
I set about trying to use HiPER Calc Pro on my phone to solve the integral for the Bessel function of the first kind and of order one, so that I could get the ordinate value for the first root of the function to 99 significant figures, then divide that by π to 99 significant figures, in order to get the Raleigh criterion constant to 99 significant figures. But then I discovered that the HiPER Calc Pro won't do the integration.
In general,
Jɴ(x) = (1/π) ∫(0,π) cos[Nt − x sin t] dt − [sin(Nπ)/π] ∫(0,∞) exp[−x sinh t − Nt] dt
However, for any integer value of N, sin(Nπ) = 0.
And so, when N is an integer, you can just solve the former term,
Jɴ(x) = (1/π) ∫(0,π) cos[Nt − x sin t] dt
And, in this case, it happens that N=1. Then you find the least positive value for x for which J₁(x) = 0.
The HP Prime G2 will solve this integral, and, to 12 significant figures, the Raleigh criterion constant is 1.21966989127. But that's as much precision as I can get from the HP Prime G2.
The Raleigh criterion (or Dawes limit) is the minimum angular size or separation, θᵣ , that can be resolved by a telescope having a circular aperture of diameter D, at wavelength λ, where D and λ have the same length units. The equation for the Raleigh criterion is
sin θᵣ = 1.21966989127 λ/D
I found another way to solve the Bessel function of the first kind for integer orders.
Jɴ(x) = Σ(k=0,∞) (−1)ᵏ (x/2)ᴺ⁺²ᵏ / [(N+k)! k!]
and
J₁(3.831705970207512315614435886308160766564545274287801928762298989918839309519011470214112874757423127) = 0.
That argument, divided by π, is the Raleigh criterion constant to 99 significant digits:
1.21966989126650445492653884746525517787935933077511212945638126557694328028076014425087191879391333
In general,
Jɴ(x) = (1/π) ∫(0,π) cos[Nt − x sin t] dt − [sin(Nπ)/π] ∫(0,∞) exp[−x sinh t − Nt] dt
However, for any integer value of N, sin(Nπ) = 0.
And so, when N is an integer, you can just solve the former term,
Jɴ(x) = (1/π) ∫(0,π) cos[Nt − x sin t] dt
And, in this case, it happens that N=1. Then you find the least positive value for x for which J₁(x) = 0.
The HP Prime G2 will solve this integral, and, to 12 significant figures, the Raleigh criterion constant is 1.21966989127. But that's as much precision as I can get from the HP Prime G2.
The Raleigh criterion (or Dawes limit) is the minimum angular size or separation, θᵣ , that can be resolved by a telescope having a circular aperture of diameter D, at wavelength λ, where D and λ have the same length units. The equation for the Raleigh criterion is
sin θᵣ = 1.21966989127 λ/D
I found another way to solve the Bessel function of the first kind for integer orders.
Jɴ(x) = Σ(k=0,∞) (−1)ᵏ (x/2)ᴺ⁺²ᵏ / [(N+k)! k!]
and
J₁(3.831705970207512315614435886308160766564545274287801928762298989918839309519011470214112874757423127) = 0.
That argument, divided by π, is the Raleigh criterion constant to 99 significant digits:
1.21966989126650445492653884746525517787935933077511212945638126557694328028076014425087191879391333