The name is absent



Rectilinear Drawing

61


faarg(r sin ψ)dψ==O

Thus we infer that the integral last written vanishes identi-
cally in
r. Now introduce the variable s=r sin ψ in this
integral. In this way we conclude that we must have


g(ʃ)^ʃ


= 0.


This is a special case of a type of integral equation treated
by Abel to which we shall refer later. Let us solve it ex-
plicitly by his simple, direct method, of which the gen-
eralization is immediate. Multiply this integral through by
r∕V'p2
2 where ʃ <r <p, and integrate as to r from 0 to p.
We obtain thus
dr = 0.

rg(ʃ)^ʃ

-r2)(r≡-J2)


Making a valid interchange of the order of integration (see
fig. 6) this becomes

fp / ∕,p rdr

J0 gt'sjs √(p2-r2) (r2-J2)Λ≡0

Fig. 6




More intriguing information

1. Output Effects of Agri-environmental Programs of the EU
2. NATURAL RESOURCE SUPPLY CONSTRAINTS AND REGIONAL ECONOMIC ANALYSIS: A COMPUTABLE GENERAL EQUILIBRIUM APPROACH
3. Accurate and robust image superresolution by neural processing of local image representations
4. Cultural Neuroeconomics of Intertemporal Choice
5. Evidence on the Determinants of Foreign Direct Investment: The Case of Three European Regions
6. I nnovative Surgical Technique in the Management of Vallecular Cyst
7. The name is absent
8. The name is absent
9. CONSUMER ACCEPTANCE OF GENETICALLY MODIFIED FOODS
10. Consciousness, cognition, and the hierarchy of context: extending the global neuronal workspace model