(a) Equation of newton's law of cooling,
"\\int \\frac{dT}{(T-T_0)} = - \\int k dt"
Where T is temperature at any time t and T0 is the temperature of surrounding.
Given, (i) at t = 0, T = 500C = 323K
(ii) at t = 0.5 hrs, T = 20 C = 293 K
Temperature of the surrounding is T0 = 5 C = 293 K
Solving equation we obtain,
"ln(T-T_0) = -kt + lnC"
applying condition (i)
"lnC = ln (45)"
applying (ii) condition,
"k = 2ln(3)"
Hence final equation will be,
"ln(T-293) = -2ln(3) t + ln(45)"
If T = 10 C = 283 K, then for time calculation,
"ln(283-278) = -2ln(3)t + ln(45) \\implies t = 1 hour"
b (i) Given "\\frac{dy}{dt} = (1-2t)y^2" and "y = \\frac{1}{c-t+t^2}"
Differentiating y with respect to x,
"\\frac{dy}{dx} = -(\\frac{1}{c-t+t^2})^2(-1+2t) = (\\frac{1}{c-t+t^2})^2(1-2t)"
replacing value of y
"\\frac{dy}{dt} = (1-2t)y^2"
(ii) "\\frac{dy}{dt} = y^2sin(t)" and "y = \\frac{1}{c+cost}"
differentiating both sides with respect to x,
"\\frac{dy}{dt} = -(\\frac{1}{c+cost})^2(-sint) = (\\frac{1}{c+cost})^2(sint) = y^2sin(t)"
(iii) "\\int_0^1 x^2 (\\sqrt{4-x^2})^3dx"
let "x = 2sin(u)" then "dx = 2cos(u) du"
Let us solve integration first without limit
"I=\\int 8cos(u)sin^2(u)(4-4sin^2(u))^{3\/2}du\n=\\int 8cos(u)sin^2(u)(4cos^2(u))^{3\/2}du =\\int 64cos^4(u)sin^2(u)du = \\int 64cos^6(u)(1-cos^2(u))du"
Integrating it,
"I = -\\frac{x(4-x^2)^{5\/2}}{6} + \\frac{x(4-x^2)^{3\/2}}{6}+x(4-x^2)^{1\/2} + 4asin(\\frac{x}{2})"
putting limits,
"\\int_0^1 x^2 (\\sqrt{4-x^2})^3dx = \\frac{2\\pi}{3}"
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