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Equivalent infinitesimal replacement
∵ln(1 x)~x
∴ln[e^sinx ³√(1-cosx)]=ln[1 e^sinx ³√(1-cosx)-1]~e^sinx ³√(1-cosx)-1
∵arctanx~x
∴arctan[2³√(1-cosx)]~2³√(1-cosx)
∴Original formula=(1/2)lim(x→0) [e^sinx ³√(1-cosx)-1]/³√(1-cosx)
=(1/2){lim(x→0) [e^sinx-1]/³√(1-cosx) lim(x→0)³√(1-cosx)/³√(1- cosx)}
=1/2 (1/2)lim(x→0) [e^sinx-1]/³√(1-cosx)
Replace with equivalent infinitesimal value
∵e^x-1~x
∴e^sinx-1~sinx~x
1-cosx~x²/2
∴Original formula=1/2 (1/2)lim(x→0) [e^sinx-1]/³√(1-cosx)
=1/2 (1/2)lim(x→0) x/³√(x²/2)
=1/2 (1/2)lim(x→0) ³√(2x)
=1/2
There are two main problems with the approach of the questioner:
1. The quad function is used to calculate numerical integrals, and the function expression cannot contain symbolic quantities;
2. The expression of the integrand function should be written in a vectorized form about the integrand variable (that is, point arithmetic should be used).
Reference Code:
R=1;
syms L;
rr = 0 : 0.1 : 1;
for ii = 1 : length(rr)
r = rr(ii);
f = @(l)(acos((1 l*l-r*r)/(2*l)) r*r*acos((r*r l*l-1)/(2*r*l) )-0.5*sqrt(4*r*r-(1 r*r-l*l)^2))*2*l/(pi*r^4);
fun = @(L) arrayfun(f,L);
J(ii) = quadl(fun,0,r);
end
plot(rr, J)
Or you can borrow part of the code from Fengxiao 1 upstairs and write:
R=1;
syms L;
rr = 0 : 0.1 : 1;
for ii = 1 : length(rr)
r = rr(ii);
SOA=R^2*acos((R^2 L^2-r^2)/(2*R*L)) r^2*acos((r^2 L^2-R^2) /(2*r*L))-...
0.5*sqrt(4*R^2*r^2-(R^2 r^2-L^2)^2);
PAB=SOA/(pi*r^2);
p=2*L/r^2;
f=PAB*p;
fun = eval(['@(L)' vectorize(f)]);
fun = @(l) arrayfun(@(L)eval(f),l);
J(ii) = quadl(fun,0,r);
end
plot(rr, J)
Although the above code can be run, there is a problem with the integrand - the value of the inverse cosine of the first term of SOA may be a complex number (because when r is slightly smaller, the parameter of acos is greater than 1), please ask the question again Check it carefully.
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