Final answer:
The leading behavior as x approaches 0+ of the given integrals can be determined by analyzing the exponent of the variable x in the integrand.
Step-by-step explanation:
The leading behavior of an integral as x approaches 0+ can be determined by analyzing the exponent of the variable x in the integrand:
(a) ∫ₓ¹ cos(xt)dt:
As x approaches 0+, the integral ∫ₓ¹ cos(xt)dt approaches 1 since the cosine function oscillates between -1 and 1.
(b) ∫₀¹ √sinh(xt) dt:
As x approaches 0+, the hyperbolic sine function sinh(xt) approaches 0 and the integral ∫₀¹ √sinh(xt) dt also approaches 0.
(c) ∫₀¹ e^-ᵗ/x dt:
As x approaches 0+, the exponential term e^-ᵗ/x approaches 1 and the integral ∫₀¹ e^-ᵗ/x dt approaches 1.
(d) ∫ₓ¹ e^-ᵗ/x dt:
As x approaches 0+, the exponential term e^-ᵗ/x approaches infinity and the integral ∫ₓ¹ e^-ᵗ/x dt approaches infinity.
(e) ∫ₓ¹ sin(xt)dt:
As x approaches 0+, the integral ∫ₓ¹ sin(xt)dt approaches 0 since the sine function oscillates around 0.
(f) ∫₀¹ [dt/(1-t)](e^x - e^xt):
As x approaches 0+, the integral ∫₀¹ [dt/(1-t)](e^x - e^xt) approaches -∞.
(g) ∫₀¹ /x e^(-t²) dt:
As x approaches 0+, the integral ∫₀¹ /x e^(-t²) dt approaches ∞.
(h) ∫₀¹ [e^-xt /(1+t²)]dt:
As x approaches 0+, the integral ∫₀¹ [e^-xt /(1+t²)]dt approaches π/2.
(i) ∫₀ to infinity J₀(xt)t^(-1/2) dt:
As x approaches 0+, the integral ∫₀ to infinity J₀(xt)t^(-1/2) dt approaches 0.