(a) Equation of newton's law of cooling,
∫(T−T0)dT=−∫kdt
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−T0)=−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)⟹t=1hour
b (i) Given dtdy=(1−2t)y2 and y=c−t+t21
Differentiating y with respect to x,
dxdy=−(c−t+t21)2(−1+2t)=(c−t+t21)2(1−2t)
replacing value of y
dtdy=(1−2t)y2
(ii) dtdy=y2sin(t) and y=c+cost1
differentiating both sides with respect to x,
dtdy=−(c+cost1)2(−sint)=(c+cost1)2(sint)=y2sin(t)
(iii) ∫01x2(4−x2)3dx
let x=2sin(u) then dx=2cos(u)du
Let us solve integration first without limit
I=∫8cos(u)sin2(u)(4−4sin2(u))3/2du=∫8cos(u)sin2(u)(4cos2(u))3/2du=∫64cos4(u)sin2(u)du=∫64cos6(u)(1−cos2(u))du
Integrating it,
I=−6x(4−x2)5/2+6x(4−x2)3/2+x(4−x2)1/2+4asin(2x)
putting limits,
∫01x2(4−x2)3dx=32π