Differential and Integral Calculus Questions and Answers – Change of Variables In a Double Integral

This set of Differential and Integral Calculus Questions and Answers for Experienced people focuses on “Change of Variables In a Double Integral”.

1. Evaluation of \(\int\int_R f(x,y) \,dx \,dy \) in cartesian coordinate can be done using change of variables principle, among the choices given below which is correct explanation of change of variables principle? (Given let x=g(u,v) & y=h(u,v))
a) \(\int\int_S f(g(u,v),h(u,v)) \,du \,dv\)
b) \(\int\int_S f(g(u,v),h(u,v)) \frac{d(x,y)}{d(u,v)} \,du \,dv\)
c) \(\int\int_S f(g(u,v),h(u,v)) \frac{∂(x,y)}{∂(u,v)} \,du \,dv\)
d) \(\int\int_S f(g(u,v),h(u,v)) \frac{∂(u,v)}{∂(x,y)} \,du \,dv\)
View Answer

Answer: c
Explanation: \(\int\int_S f(g(u,v),h(u,v)) \frac{∂(x,y)}{∂(u,v)} \,du \,dv\)
where \( \frac{∂(x,y)}{∂(u,v)} = \begin{vmatrix}
\frac{∂x}{∂u} \frac{∂x}{∂v}\\
\frac{∂y}{∂u} \frac{∂y}{∂v}\\
\end{vmatrix} = J(\frac{x,y}{u,v}) = \frac{∂x}{∂u} \frac{∂y}{∂v} – \frac{∂x}{∂v} \frac{∂y}{∂u} …..\)(‘J’ is Jacobian).

2. The value of ∬R (x-y)2 dx dy where R is the parallelogram with vertices (0,0), (1,1),(2,0), (1,-1) when solved using change of variables is given by____
Find value of ∬R (x-y)2 dx dy where R vertices (0,0), (1,1),(2,0), (1,-1) in given figure
a) 16/3
b) 8/3
c) 4/3
d) 0
View Answer

Answer: b
Explanation: W.K.T from change of variables principle
\(\int\int_R f(x,y)\,dx \,dy = \int\int_S f(g(u,v),h(u,v)) \frac{∂(x,y)}{∂(u,v)} \,du \,dv …..(1)\)
From the above diagram in the region R the equations are given by
x-y=0, x-y=2, x+y=0, x+y=2 from this we can observe that change of
variables is u=x-y, v=x+y solving we get \(x=\frac{u+v}{2}, y=\frac{v-u}{2}\)
\(\frac{∂(x,y)}{∂(u,v)} = \begin{vmatrix}
\frac{∂x}{∂u}&\frac{∂x}{∂v}\\
\frac{∂y}{∂u}&\frac{∂y}{∂v}\\
\end{vmatrix} = \begin{vmatrix}
0.5 &0.5\\
-0.5&0.5\\
\end{vmatrix} = 0.5\)
The region S in the (u,v) is the square 0<u<2,0<v<2. Since x-y=u integral
becomes \(\int_0^2 \int_0^2 0.5u^2 \,du \,dv\)……from(1)
\(=\int_0^2 \Big[\frac{u^3}{6}\Big]_0^2 \,dv = \int_0^2 \frac{4}{3} dv = \frac{8}{3}.\)

3. If double integral in Cartesian coordinate is given by ∬R f(x,y) dx dy then the value of same integral in polar form is _____
a) ∬P f(r cos θ, rsin θ)dr dθ
b) ∬P f(r cos⁡θ, r sin⁡θ)rdr dθ
c) ∬P f(r cos⁡θ, r sin⁡θ) r2 dr dθ
d) ∬P f(r sin⁡θ, r cos⁡θ)dr dθ
View Answer

Answer: b
Explanation: ∬R f(x,y)dx dy when converting this into polar form we take x = r cos θ
y=r sin θ as change of variables from
\(\int\int_R f(x,y) \,dx \,dy = \int\int_S f(g(u,v),h(u,v)) \frac{∂(x,y)}{∂(u,v)} \,du \,dv \) where u=r & v=θ
thus \(\frac{∂(x,y)}{∂(r,θ)} =\begin{vmatrix}
\frac{∂x}{∂r} &\frac{∂x}{∂θ}\\
\frac{∂y}{∂r} &\frac{∂y}{∂θ}\\
\end{vmatrix} = \begin{vmatrix}
cos⁡θ &-r sin⁡θ\\
sin⁡θ & rcos⁡θ\\
\end{vmatrix} = r(cos^2 θ + sin^2 θ) = r\)
substituting we get ∬P f(r cos θ,r sin θ)rdr dθ.
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4. The value of ∬R sin⁡(x2 + y2) dx dy where R is the region bounded by circle centered at origin with radius r=2 is _____
a) πcos 4
b) π(1-cos 4)
c) π
d) π(1-sin 4)
View Answer

Answer: b
Explanation: Using Polar variable transformation x = r cos θ & y=r sin θ, r varies from 0 to 2 & θ varies from 0 to 2π because radius of circle i.e r=2 & centered at origin
\(\int\int_P f(r cos θ,r sin θ )rdr \,dθ = \int\int_R sin⁡ (x^2+y^2) \,dx \,dy = \int_0^2π \int_0^2 r sin⁡ r^2 \,dr \,dθ\)
Using substitution t=r2 integral changes to \(\int_0^{2π} \int_0^4 0.5 \,sin⁡t \,dt \,dθ\)
\(\int_0^{2π} 0.5\big[-cos⁡t\big]_0^4 dθ = \int_0^{2π} 0.5(1-cos⁡4) dθ = π(1-cos 4)\).

5. Using change of variables principle in double integral we can reduce cartesian integral to simpler form.
a) True
b) False
View Answer

Answer: a
Explanation: The above statement is not necessarily true always but change of variables cartesian to polar form & changing into suitable form reduces the complexity in the evaluation of double integral however converse is also true for example ∬R x2 y3 dx dy is the given integral while solving there is no need of converting it into polar form since ∬P r6 cos2 θ sin3 θ dr dθ is tedious to solve when R only consists of constants but ∬R x2 y3 dx dy can be solved easily by ordinary method of integration.
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