Thanks =)
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Note that the differential in the numerator names the function, and the differential in the denominator names the variable, thus this is equivalent to the second derivative of T(x).
T''(x) + C = 0
Integrating both sides:
∫ T''(x)dx + ∫C dx = ∫ (0) dx
T'(x) + Cx = K
Where K is another arbitrary constant obtained from the integrals. Again:
∫ T'(x) dx + ∫ Cx dx = ∫ K dx
T(x) + (1/2)Cx^2 = Kx + M
Where M is another arbitrary constant, thus we have:
T(x) = M + Kx - (1/2)Cx^2
Done!
T''(x) + C = 0
Integrating both sides:
∫ T''(x)dx + ∫C dx = ∫ (0) dx
T'(x) + Cx = K
Where K is another arbitrary constant obtained from the integrals. Again:
∫ T'(x) dx + ∫ Cx dx = ∫ K dx
T(x) + (1/2)Cx^2 = Kx + M
Where M is another arbitrary constant, thus we have:
T(x) = M + Kx - (1/2)Cx^2
Done!