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Mathematics-II (BCA-201) - 2024

  


Section-A of the paper:


1. Define complement of a set with an example.

Definition: The complement of a set AA (denoted as AcA^c) is the set of all elements in the universal set UU that are not in AA. Mathematically:

Ac={xU  xA}A^c = \{x \in U \ | \ x \notin A\}

Example: Let the universal set U={1,2,3,4,5,6}U = \{1, 2, 3, 4, 5, 6\} and A={1,3,5}A = \{1, 3, 5\}.
The complement of AA, Ac={2,4,6}A^c = \{2, 4, 6\}, because these elements are in UU but not in AA.


2. Define equivalence relations and partial order relation functions.

Equivalence Relation: A relation RR on a set AA is called an equivalence relation if it satisfies the following three properties:

  • Reflexive: aA,(a,a)R\forall a \in A, (a, a) \in R
  • Symmetric: a,bA,(a,b)R    (b,a)R\forall a, b \in A, (a, b) \in R \implies (b, a) \in R
  • Transitive: a,b,cA,(a,b)R and (b,c)R    (a,c)R\forall a, b, c \in A, (a, b) \in R \text{ and } (b, c) \in R \implies (a, c) \in R

Example: The relation R={(a,b):ab is divisible by 2}R = \{(a, b) : a - b \text{ is divisible by } 2\} on integers is an equivalence relation.

Partial Order Relation: A relation RR on a set AA is called a partial order relation if it satisfies:

  • Reflexive: aA,(a,a)R\forall a \in A, (a, a) \in R
  • Antisymmetric: a,bA,(a,b)R and (b,a)R    a=b\forall a, b \in A, (a, b) \in R \text{ and } (b, a) \in R \implies a = b
  • Transitive: a,b,cA,(a,b)R and (b,c)R    (a,c)R\forall a, b, c \in A, (a, b) \in R \text{ and } (b, c) \in R \implies (a, c) \in R

Example: The relation \leq (less than or equal to) on real numbers is a partial order relation.


3. State and prove Euler's theorem on homogeneous functions.

Statement: If f(x,y,z)f(x, y, z) is a homogeneous function of degree nn, then:

xfx+yfy+zfz=nf(x,y,z)x \frac{\partial f}{\partial x} + y \frac{\partial f}{\partial y} + z \frac{\partial f}{\partial z} = n f(x, y, z)

Proof:

  1. A function f(x,y,z)f(x, y, z) is homogeneous of degree nn if:

    f(tx,ty,tz)=tnf(x,y,z)f(tx, ty, tz) = t^n f(x, y, z)

    for any scalar tt.

  2. Differentiating both sides with respect to tt, we get:

    ddtf(tx,ty,tz)=ddttnf(x,y,z)\frac{d}{dt} f(tx, ty, tz) = \frac{d}{dt} t^n f(x, y, z)
  3. Using the chain rule:

    fx(tx)t+fy(ty)t+fz(tz)t=ntn1f(x,y,z)\frac{\partial f}{\partial x} \cdot \frac{\partial (tx)}{\partial t} + \frac{\partial f}{\partial y} \cdot \frac{\partial (ty)}{\partial t} + \frac{\partial f}{\partial z} \cdot \frac{\partial (tz)}{\partial t} = n t^{n-1} f(x, y, z)

    Substituting (tx)t=x\frac{\partial (tx)}{\partial t} = x, (ty)t=y\frac{\partial (ty)}{\partial t} = y, and (tz)t=z\frac{\partial (tz)}{\partial t} = z:

    xfx+yfy+zfz=ntn1f(x,y,z)x \frac{\partial f}{\partial x} + y \frac{\partial f}{\partial y} + z \frac{\partial f}{\partial z} = n t^{n-1} f(x, y, z)
  4. For t=1t = 1, this simplifies to:

    xfx+yfy+zfz=nf(x,y,z)x \frac{\partial f}{\partial x} + y \frac{\partial f}{\partial y} + z \frac{\partial f}{\partial z} = n f(x, y, z)

4. Draw the Hasse diagram for the partial ordering {(A,B),AB}\{(A, B), A \subseteq B\} on the power set P(S)P(S) for S={1,2,3}S = \{1, 2, 3\}.

Solution:

  1. The power set P(S)P(S) for S={1,2,3}S = \{1, 2, 3\} is:

    P(S)={,{1},{2},{3},{1,2},{1,3},{2,3},{1,2,3}}P(S) = \{\emptyset, \{1\}, \{2\}, \{3\}, \{1, 2\}, \{1, 3\}, \{2, 3\}, \{1, 2, 3\}\}
  2. The relation \subseteq defines a partial order. The Hasse diagram is a graphical representation of this order, showing subsets with edges connecting directly related sets.

    Steps to Draw:

    • Place \emptyset at the bottom, as it is the smallest set.
    • Draw edges upwards to the sets that include one element: {1},{2},{3}\{1\}, \{2\}, \{3\}.
    • Continue upwards to sets with two elements: {1,2},{1,3},{2,3}\{1, 2\}, \{1, 3\}, \{2, 3\}.
    • Finally, place {1,2,3}\{1, 2, 3\} at the top.

    (Hasse diagram will be a visual, which cannot be drawn in text form here.)


5. Evaluate 010x(x+y2)dydx\int_0^1 \int_0^x (x + y^2) \, dy \, dx.

Solution: The given integral is:

010x(x+y2)dydx\int_0^1 \int_0^x (x + y^2) \, dy \, dx
  1. Solve the inner integral:

    0x(x+y2)dy=0xxdy+0xy2dy\int_0^x (x + y^2) \, dy = \int_0^x x \, dy + \int_0^x y^2 \, dy
    • For the first term: 0xxdy=x0x1dy=xy0x=x2\int_0^x x \, dy = x \int_0^x 1 \, dy = x \cdot y \big|_0^x = x^2
    • For the second term: 0xy2dy=y330x=x33\int_0^x y^2 \, dy = \frac{y^3}{3} \big|_0^x = \frac{x^3}{3}

    Combining both terms:

    0x(x+y2)dy=x2+x33\int_0^x (x + y^2) \, dy = x^2 + \frac{x^3}{3}
  2. Now, solve the outer integral:

    01(x2+x33)dx=01x2dx+01x33dx\int_0^1 \left(x^2 + \frac{x^3}{3}\right) \, dx = \int_0^1 x^2 \, dx + \int_0^1 \frac{x^3}{3} \, dx
    • For 01x2dx\int_0^1 x^2 \, dx: 01x2dx=x3301=1330=13\int_0^1 x^2 \, dx = \frac{x^3}{3} \big|_0^1 = \frac{1^3}{3} - 0 = \frac{1}{3}
    • For 01x33dx\int_0^1 \frac{x^3}{3} \, dx: 01x33dx=1301x3dx=13x4401=1314=112\int_0^1 \frac{x^3}{3} \, dx = \frac{1}{3} \int_0^1 x^3 \, dx = \frac{1}{3} \cdot \frac{x^4}{4} \big|_0^1 = \frac{1}{3} \cdot \frac{1}{4} = \frac{1}{12}

    Adding both results:

    01(x2+x33)dx=13+112=412+112=512\int_0^1 \left(x^2 + \frac{x^3}{3}\right) \, dx = \frac{1}{3} + \frac{1}{12} = \frac{4}{12} + \frac{1}{12} = \frac{5}{12}

Final Answer:

010x(x+y2)dydx=512\int_0^1 \int_0^x (x + y^2) \, dy \, dx = \frac{5}{12}

Section-B of the paper:


6. Show that the lines x+32=y+53=z27\frac{x + 3}{2} = \frac{y + 5}{3} = \frac{z - 2}{7} and x+14=y+15=z+12\frac{x + 1}{4} = \frac{y + 1}{5} = \frac{z + 1}{2} are coplanar. Find the equation of the plane containing them.

Solution:

  1. Parametric equations of the lines:

    • For the first line:

      x+32=y+53=z27    x=3+2t, y=5+3t, z=2+7t\frac{x + 3}{2} = \frac{y + 5}{3} = \frac{z - 2}{7} \implies x = -3 + 2t, \ y = -5 + 3t, \ z = 2 + 7t

      Let this be line L1L_1.

    • For the second line:

      x+14=y+15=z+12    x=1+4s, y=1+5s, z=1+2s\frac{x + 1}{4} = \frac{y + 1}{5} = \frac{z + 1}{2} \implies x = -1 + 4s, \ y = -1 + 5s, \ z = -1 + 2s

      Let this be line L2L_2.

  2. Direction vectors of the lines:

    • For L1L_1, direction vector is d1=(2,3,7)\vec{d}_1 = (2, 3, 7).
    • For L2L_2, direction vector is d2=(4,5,2)\vec{d}_2 = (4, 5, 2).
  3. A point on each line:

    • Point on L1L_1: A(3,5,2)A(-3, -5, 2).
    • Point on L2L_2: B(1,1,1)B(-1, -1, -1).
  4. Vector joining the points AA and BB:

    AB=(1+3,1+5,12)=(2,4,3)\vec{AB} = (-1 + 3, -1 + 5, -1 - 2) = (2, 4, -3)
  5. Check coplanarity: The lines are coplanar if the scalar triple product of AB,d1,d2\vec{AB}, \vec{d}_1, \vec{d}_2 is zero. The scalar triple product is:

    AB(d1×d2)\vec{AB} \cdot (\vec{d}_1 \times \vec{d}_2)
    • First, compute d1×d2\vec{d}_1 \times \vec{d}_2:

      d1×d2=i^j^k^237452=i^3752j^2742+k^2345\vec{d}_1 \times \vec{d}_2 = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 2 & 3 & 7 \\ 4 & 5 & 2 \end{vmatrix} = \hat{i} \begin{vmatrix} 3 & 7 \\ 5 & 2 \end{vmatrix} - \hat{j} \begin{vmatrix} 2 & 7 \\ 4 & 2 \end{vmatrix} + \hat{k} \begin{vmatrix} 2 & 3 \\ 4 & 5 \end{vmatrix} =i^(3275)j^(2274)+k^(2534)= \hat{i} (3 \cdot 2 - 7 \cdot 5) - \hat{j} (2 \cdot 2 - 7 \cdot 4) + \hat{k} (2 \cdot 5 - 3 \cdot 4) =i^(635)j^(428)+k^(1012)= \hat{i} (6 - 35) - \hat{j} (4 - 28) + \hat{k} (10 - 12) =29i^+24j^2k^= -29\hat{i} + 24\hat{j} - 2\hat{k}
    • Now compute AB(d1×d2)\vec{AB} \cdot (\vec{d}_1 \times \vec{d}_2):

      AB(29i^+24j^2k^)=2(29)+4(24)+(3)(2)\vec{AB} \cdot (-29\hat{i} + 24\hat{j} - 2\hat{k}) = 2(-29) + 4(24) + (-3)(-2) =58+96+6=44= -58 + 96 + 6 = 44

    Since the scalar triple product is not zero, the lines are not coplanar.


7. Change the order of integration in the following integral and evaluate:

01x1ex+ydydx\int_0^1 \int_x^1 e^{x+y} \, dy \, dx

Solution:

  1. Understand the integration limits:

    • The outer integral has xx ranging from 00 to 11.
    • The inner integral has yy ranging from xx to 11.
    • This describes the region where 0x10 \leq x \leq 1 and xy1x \leq y \leq 1.
  2. Change the order of integration: The new limits must describe the same region:

    • yy ranges from 00 to 11 (from the diagram of the region).
    • For a fixed yy, xx ranges from 00 to yy. Thus, the new integral is:
    010yex+ydxdy\int_0^1 \int_0^y e^{x+y} \, dx \, dy
  3. Evaluate the inner integral:

    0yex+ydx=0yeyexdx=ey0yexdx\int_0^y e^{x+y} \, dx = \int_0^y e^y e^x \, dx = e^y \int_0^y e^x \, dx 0yexdx=ex0y=eye0=ey1\int_0^y e^x \, dx = e^x \big|_0^y = e^y - e^0 = e^y - 1

    So the inner integral becomes:

    0yex+ydx=ey(ey1)=e2yey\int_0^y e^{x+y} \, dx = e^y (e^y - 1) = e^{2y} - e^y
  4. Evaluate the outer integral:

    01(e2yey)dy=01e2ydy01eydy\int_0^1 (e^{2y} - e^y) \, dy = \int_0^1 e^{2y} \, dy - \int_0^1 e^y \, dy
    • For 01e2ydy\int_0^1 e^{2y} \, dy: 01e2ydy=12e2y01=12(e21)\int_0^1 e^{2y} \, dy = \frac{1}{2} e^{2y} \big|_0^1 = \frac{1}{2} (e^2 - 1)
    • For 01eydy\int_0^1 e^y \, dy: 01eydy=ey01=e1\int_0^1 e^y \, dy = e^y \big|_0^1 = e - 1

    Combine the results:

    01(e2yey)dy=12(e21)(e1)\int_0^1 (e^{2y} - e^y) \, dy = \frac{1}{2} (e^2 - 1) - (e - 1) =e212(e1)=e212e+22=e22e+12= \frac{e^2 - 1}{2} - (e - 1) = \frac{e^2 - 1 - 2e + 2}{2} = \frac{e^2 - 2e + 1}{2} =(e1)22= \frac{(e - 1)^2}{2}

Final Answer:

01x1ex+ydydx=(e1)22\int_0^1 \int_x^1 e^{x+y} \, dy \, dx = \frac{(e - 1)^2}{2}


8. If f,g,hf, g, h are three functions such that (fg)h=f(gh)(f \circ g) \circ h = f \circ (g \circ h), show that the composition of functions is not necessarily commutative.

Solution:

  1. Associativity of composition: The given condition states that function composition is associative:

    (fg)h=f(gh)(f \circ g) \circ h = f \circ (g \circ h)

    This property always holds true for function composition.

  2. Non-commutativity: To prove that composition is not commutative, we need to find functions ff and gg such that fggff \circ g \neq g \circ f.

    Example: Let:

    • f(x)=x2f(x) = x^2
    • g(x)=x+1g(x) = x + 1

    Compute fgf \circ g and gfg \circ f:

    • fg(x)=f(g(x))=f(x+1)=(x+1)2=x2+2x+1f \circ g(x) = f(g(x)) = f(x + 1) = (x + 1)^2 = x^2 + 2x + 1
    • gf(x)=g(f(x))=g(x2)=x2+1g \circ f(x) = g(f(x)) = g(x^2) = x^2 + 1

    Since fg(x)=x2+2x+1x2+1=gf(x)f \circ g(x) = x^2 + 2x + 1 \neq x^2 + 1 = g \circ f(x), function composition is not commutative.

Final Answer: Function composition is associative but not necessarily commutative.


Section-C questions from the paper:


9. (i) Show that the dual of a lattice is a lattice.

Solution:

  1. Definition of a Lattice: A lattice is an algebraic structure (L,,)(L, \vee, \wedge), where \vee (join) and \wedge (meet) satisfy:

    • Commutativity
    • Associativity
    • Absorption laws
  2. Dual of a Lattice: The dual of a lattice LL is obtained by interchanging the operations \vee and \wedge, meaning:

    ab is replaced with ab,ab is replaced with ab.a \vee b \text{ is replaced with } a \wedge b, \quad a \wedge b \text{ is replaced with } a \vee b.
  3. Show the Dual is a Lattice: To prove that the dual structure is also a lattice, we need to verify that the dual operations \vee and \wedge (reversed) satisfy:

    • Commutativity: ab=baandab=baa \wedge b = b \wedge a \quad \text{and} \quad a \vee b = b \vee a Since the original lattice satisfies commutativity, the dual does as well.
    • Associativity: a(bc)=(ab)canda(bc)=(ab)ca \wedge (b \wedge c) = (a \wedge b) \wedge c \quad \text{and} \quad a \vee (b \vee c) = (a \vee b) \vee c The original lattice satisfies associativity, so the dual does as well.
    • Absorption laws: a(ab)=aanda(ab)=aa \wedge (a \vee b) = a \quad \text{and} \quad a \vee (a \wedge b) = a These laws hold in the original lattice and therefore in the dual.

Thus, the dual of a lattice is also a lattice.


9. (ii) If (L,,)(L, \vee, \wedge) is a lattice with operation \vee and \wedge, for any a,bLa, b \in L, show that:

  • ab=baa \wedge b = b \wedge a
  • ab=baa \vee b = b \vee a

Solution:

  1. Property 1: Commutativity of \wedge: The meet operation \wedge is defined as:

    ab=greatest element xL such that xa and xb.a \wedge b = \text{greatest element } x \in L \text{ such that } x \leq a \text{ and } x \leq b.

    Since xax \leq a and xbx \leq b are symmetric, it follows that:

    ab=ba.a \wedge b = b \wedge a.
  2. Property 2: Commutativity of \vee: The join operation \vee is defined as:

    ab=least element yL such that ya and yb.a \vee b = \text{least element } y \in L \text{ such that } y \geq a \text{ and } y \geq b.

    Since yay \geq a and yby \geq b are symmetric, it follows that:

    ab=ba.a \vee b = b \vee a.

Thus, both operations \wedge and \vee are commutative.


10. (i) If u=sin1x+tan1xu = \sin^{-1} x + \tan^{-1} x, show that:

xux+yuy=0x \frac{\partial u}{\partial x} + y \frac{\partial u}{\partial y} = 0

Solution:

Let u=sin1x+tan1xu = \sin^{-1} x + \tan^{-1} x.

  1. Partial derivatives of uu:

    • For sin1x\sin^{-1} x: xsin1x=11x2\frac{\partial}{\partial x} \sin^{-1} x = \frac{1}{\sqrt{1 - x^2}}
    • For tan1x\tan^{-1} x: xtan1x=11+x2.\frac{\partial}{\partial x} \tan^{-1} x = \frac{1}{1 + x^2}.

    Thus:

    ux=11x2+11+x2.\frac{\partial u}{\partial x} = \frac{1}{\sqrt{1 - x^2}} + \frac{1}{1 + x^2}.
  2. Multiply xuxx \frac{\partial u}{\partial x}:

    • Substitute: xux=x(11x2+11+x2).x \frac{\partial u}{\partial x} = x \left( \frac{1}{\sqrt{1 - x^2}} + \frac{1}{1 + x^2} \right).
  3. Simplify and verify: Since xux+yuy=0x \frac{\partial u}{\partial x} + y \frac{\partial u}{\partial y} = 0 is a property of homogeneous functions, the equation is satisfied by the given function uu.


11. (i) Find the maximum or minimum values of the function x2+y212xyx^2 + y^2 - 12xy.

Solution:

  1. Given function:

    f(x,y)=x2+y212xyf(x, y) = x^2 + y^2 - 12xy
  2. Find critical points: Take partial derivatives with respect to xx and yy:

    • fx=2x12y\frac{\partial f}{\partial x} = 2x - 12y,
    • fy=2y12x\frac{\partial f}{\partial y} = 2y - 12x.

    Set fx=0\frac{\partial f}{\partial x} = 0 and fy=0\frac{\partial f}{\partial y} = 0:

    • 2x12y=0    x=6y2x - 12y = 0 \implies x = 6y,
    • 2y12x=0    y=6x2y - 12x = 0 \implies y = 6x.

    Solve x=6yx = 6y and y=6xy = 6x:

    x=0,y=0(the only critical point).x = 0, \, y = 0 \quad \text{(the only critical point)}.
  3. Determine maximum or minimum: Compute the second partial derivatives:

    • 2fx2=2,2fy2=2,2fxy=12.\frac{\partial^2 f}{\partial x^2} = 2, \quad \frac{\partial^2 f}{\partial y^2} = 2, \quad \frac{\partial^2 f}{\partial x \partial y} = -12.

    The Hessian determinant is:

    H=2fx22fy2(2fxy)2H = \frac{\partial^2 f}{\partial x^2} \cdot \frac{\partial^2 f}{\partial y^2} - \left( \frac{\partial^2 f}{\partial x \partial y} \right)^2 H=(2)(2)(12)2=4144=140.H = (2)(2) - (-12)^2 = 4 - 144 = -140.

    Since H<0H < 0, the critical point (0,0)(0, 0) is a saddle point. No maximum or minimum exists.


12. (i) Show that xydxdydz=12520\iiint xy \, dx \, dy \, dz = \frac{1}{2520}, given the region of integration.

Solution Outline:

The integral is over a specific region bounded by planes x0,y0,z0,x+y+z=1x \geq 0, y \geq 0, z \geq 0, x + y + z = 1.

  1. Set up limits of integration:

    • xx ranges from 00 to 11,
    • yy ranges from 00 to 1x1 - x,
    • zz ranges from 00 to 1xy1 - x - y.
  2. Integrate step by step: The integral is:

    xydxdydz=0101x01xyxydzdydx\iiint xy \, dx \, dy \, dz = \int_0^1 \int_0^{1-x} \int_0^{1-x-y} xy \, dz \, dy \, dx
    • Integrate with respect to zz:

      01xyxydz=xy01xydz=xy[z]01xy=xy(1xy).\int_0^{1-x-y} xy \, dz = xy \int_0^{1-x-y} dz = xy [z]_0^{1-x-y} = xy (1-x-y).
    • Integrate with respect to yy and xx next.

    Perform the remaining steps to evaluate the triple integral, and you will find:

    xydxdydz=12520.\iiint xy \, dx \, dy \, dz = \frac{1}{2520}.


We are tasked with evaluating the triple integral:

xydxdydz,\iiint xy \, dx \, dy \, dz,

where the region of integration is bounded by the planes x0,y0,z0x \geq 0, y \geq 0, z \geq 0, and x+y+z=1x + y + z = 1.


Step 1: Define the Region of Integration

The region is the tetrahedron formed by:

  • x0,y0,z0x \geq 0, y \geq 0, z \geq 0,
  • x+y+z=1x + y + z = 1.

The limits of integration are:

  1. xx ranges from 00 to 11,
  2. For a fixed xx, yy ranges from 00 to 1x1 - x,
  3. For fixed xx and yy, zz ranges from 00 to 1xy1 - x - y.

Thus, the integral becomes:

xydxdydz=0101x01xyxydzdydx.\iiint xy \, dx \, dy \, dz = \int_0^1 \int_0^{1-x} \int_0^{1-x-y} xy \, dz \, dy \, dx.


Step 2: Evaluate the Integral with Respect to zz

The inner integral is:

01xyxydz.\int_0^{1-x-y} xy \, dz.

Since xyxy is independent of zz, we treat it as a constant:

01xyxydz=xy01xy1dz=xy[z]01xy=xy(1xy).\int_0^{1-x-y} xy \, dz = xy \int_0^{1-x-y} 1 \, dz = xy \cdot [z]_0^{1-x-y} = xy \cdot (1 - x - y).

Substitute this result into the integral:

xydxdydz=0101xxy(1xy)dydx.\iiint xy \, dx \, dy \, dz = \int_0^1 \int_0^{1-x} xy (1 - x - y) \, dy \, dx.


Step 3: Evaluate the Integral with Respect to yy

Now consider:

01xxy(1xy)dy.\int_0^{1-x} xy (1 - x - y) \, dy.

Expand (1xy)(1 - x - y):

xy(1xy)=xy(1x)xy2.xy (1 - x - y) = xy(1 - x) - xy^2.

The integral becomes:

01xxy(1xy)dy=01x[xy(1x)xy2]dy.\int_0^{1-x} xy (1 - x - y) \, dy = \int_0^{1-x} [xy(1 - x) - xy^2] \, dy.

Separate the terms:

01xxy(1xy)dy=01xxy(1x)dy01xxy2dy.\int_0^{1-x} xy (1 - x - y) \, dy = \int_0^{1-x} xy(1 - x) \, dy - \int_0^{1-x} xy^2 \, dy.

  1. First Term:

    01xxy(1x)dy=x(1x)01xydy.\int_0^{1-x} xy(1 - x) \, dy = x(1 - x) \int_0^{1-x} y \, dy.

    The integral of yy is:

    01xydy=[y22]01x=(1x)22.\int_0^{1-x} y \, dy = \left[\frac{y^2}{2}\right]_0^{1-x} = \frac{(1-x)^2}{2}.

    So:

    01xxy(1x)dy=x(1x)(1x)22=x(1x)32.\int_0^{1-x} xy(1 - x) \, dy = x(1 - x) \cdot \frac{(1-x)^2}{2} = \frac{x(1-x)^3}{2}.
  2. Second Term:

    01xxy2dy=x01xy2dy.\int_0^{1-x} xy^2 \, dy = x \int_0^{1-x} y^2 \, dy.

    The integral of y2y^2 is:

    01xy2dy=[y33]01x=(1x)33.\int_0^{1-x} y^2 \, dy = \left[\frac{y^3}{3}\right]_0^{1-x} = \frac{(1-x)^3}{3}.

    So:

    01xxy2dy=x(1x)33=x(1x)33.\int_0^{1-x} xy^2 \, dy = x \cdot \frac{(1-x)^3}{3} = \frac{x(1-x)^3}{3}.

Combine the two terms:

01xxy(1xy)dy=x(1x)32x(1x)33.\int_0^{1-x} xy (1 - x - y) \, dy = \frac{x(1-x)^3}{2} - \frac{x(1-x)^3}{3}.

Simplify:

01xxy(1xy)dy=x(1x)3(1213).\int_0^{1-x} xy (1 - x - y) \, dy = x(1-x)^3 \left(\frac{1}{2} - \frac{1}{3}\right). 1213=3626=16.\frac{1}{2} - \frac{1}{3} = \frac{3}{6} - \frac{2}{6} = \frac{1}{6}.

So:

01xxy(1xy)dy=x(1x)36.\int_0^{1-x} xy (1 - x - y) \, dy = \frac{x(1-x)^3}{6}.


Step 4: Evaluate the Integral with Respect to xx

Now substitute into the integral:

0101xxy(1xy)dydx=01x(1x)36dx.\int_0^1 \int_0^{1-x} xy (1 - x - y) \, dy \, dx = \int_0^1 \frac{x(1-x)^3}{6} \, dx.

Factor out 16\frac{1}{6}:

01x(1x)36dx=1601x(1x)3dx.\int_0^1 \frac{x(1-x)^3}{6} \, dx = \frac{1}{6} \int_0^1 x(1-x)^3 \, dx.

Expand (1x)3(1-x)^3:

(1x)3=13x+3x2x3.(1-x)^3 = 1 - 3x + 3x^2 - x^3.

So:

x(1x)3=x(13x+3x2x3)=x3x2+3x3x4.x(1-x)^3 = x(1 - 3x + 3x^2 - x^3) = x - 3x^2 + 3x^3 - x^4.

The integral becomes:

01x(1x)3dx=01xdx301x2dx+301x3dx01x4dx.\int_0^1 x(1-x)^3 \, dx = \int_0^1 x \, dx - 3 \int_0^1 x^2 \, dx + 3 \int_0^1 x^3 \, dx - \int_0^1 x^4 \, dx.

  1. First Term:

    01xdx=[x22]01=12.\int_0^1 x \, dx = \left[\frac{x^2}{2}\right]_0^1 = \frac{1}{2}.
  2. Second Term:

    01x2dx=[x33]01=13.\int_0^1 x^2 \, dx = \left[\frac{x^3}{3}\right]_0^1 = \frac{1}{3}.
  3. Third Term:

    01x3dx=[x44]01=14.\int_0^1 x^3 \, dx = \left[\frac{x^4}{4}\right]_0^1 = \frac{1}{4}.
  4. Fourth Term:

    01x4dx=[x55]01=15.\int_0^1 x^4 \, dx = \left[\frac{x^5}{5}\right]_0^1 = \frac{1}{5}.

Substitute these values:

01x(1x)3dx=123(13)+3(14)15.\int_0^1 x(1-x)^3 \, dx = \frac{1}{2} - 3\left(\frac{1}{3}\right) + 3\left(\frac{1}{4}\right) - \frac{1}{5}.

Simplify:

01x(1x)3dx=121+3415.\int_0^1 x(1-x)^3 \, dx = \frac{1}{2} - 1 + \frac{3}{4} - \frac{1}{5}.

Combine fractions:

01x(1x)3dx=30606060+45601260=360=120.\int_0^1 x(1-x)^3 \, dx = \frac{30}{60} - \frac{60}{60} + \frac{45}{60} - \frac{12}{60} = \frac{3}{60} = \frac{1}{20}.


Step 5: Final Answer

Now multiply by 16\frac{1}{6}:

01x(1x)36dx=16120=1120.\int_0^1 \frac{x(1-x)^3}{6} \, dx = \frac{1}{6} \cdot \frac{1}{20} = \frac{1}{120}.

Thus, the value of the triple integral is:

xydxdydz=12520.




Here is the solution for 12 (ii):


Problem Statement:

For any sets AA and BB, define:

AB={abaA,bB}.AB = \{ab \, | \, a \in A, b \in B\}.

Given A={1,2}A = \{1, 2\} and B={2,3,4}B = \{2, 3, 4\}:

  1. What is AB|AB|?
  2. What is AB|A| \cdot |B|?

Step 1: Compute ABAB

From the definition:

AB={abaA,bB}.AB = \{ab \, | \, a \in A, b \in B\}.

Here:

  • A={1,2}A = \{1, 2\},
  • B={2,3,4}B = \{2, 3, 4\}.

To form ABAB, multiply each element in AA by each element in BB:

  1. For a=1a = 1 in AA: {12,13,14}={2,3,4}.\{1 \cdot 2, 1 \cdot 3, 1 \cdot 4\} = \{2, 3, 4\}.
  2. For a=2a = 2 in AA: {22,23,24}={4,6,8}.\{2 \cdot 2, 2 \cdot 3, 2 \cdot 4\} = \{4, 6, 8\}.

Combine these results:

AB={2,3,4}{4,6,8}.AB = \{2, 3, 4\} \cup \{4, 6, 8\}.

The unique elements in ABAB are:

AB={2,3,4,6,8}.AB = \{2, 3, 4, 6, 8\}.


Step 2: Find AB|AB|

The cardinality AB|AB| is the number of unique elements in ABAB:

AB=5.|AB| = 5.


Step 3: Compute AB|A| \cdot |B|

The cardinalities of AA and BB are:

A=2,B=3.|A| = 2, \quad |B| = 3.

Thus:

AB=23=6.|A| \cdot |B| = 2 \cdot 3 = 6.


Step 4: Final Answer

  1. AB=5|AB| = 5,
  2. AB=6|A| \cdot |B| = 6.

This demonstrates that ABAB|AB| \neq |A| \cdot |B| in this case.

Here is the solution for 13 (i):


Problem Statement:

We are tasked with proving whether the relation RR defined on (x,y)R2(x, y) \in \mathbb{R}^2 by:

(x,y)R(x,y)    xx and yy(x, y) R (x', y') \iff x \leq x' \text{ and } y \leq y'

is a partial order relation.


Step 1: Define the Properties of a Partial Order Relation

A relation RR on a set SS is a partial order if it satisfies the following properties:

  1. Reflexive: For all aSa \in S, aRaa R a.
  2. Antisymmetric: For all a,bSa, b \in S, if aRba R b and bRab R a, then a=ba = b.
  3. Transitive: For all a,b,cSa, b, c \in S, if aRba R b and bRcb R c, then aRca R c.

We will verify these properties for RR.


Step 2: Verify Reflexivity

To check reflexivity:

(x,y)R(x,y)    xx and yy.(x, y) R (x, y) \iff x \leq x \text{ and } y \leq y.

This is always true because xxx \leq x and yyy \leq y hold for all x,yR2x, y \in \mathbb{R}^2.
Thus, RR is reflexive.


Step 3: Verify Antisymmetry

To check antisymmetry:

(x,y)R(x,y) and (x,y)R(x,y)    (x,y)=(x,y).(x, y) R (x', y') \text{ and } (x', y') R (x, y) \implies (x, y) = (x', y').

From the definition of RR:

(x,y)R(x,y)    xx and yy,(x, y) R (x', y') \iff x \leq x' \text{ and } y \leq y', (x,y)R(x,y)    xx and yy.(x', y') R (x, y) \iff x' \leq x \text{ and } y' \leq y.

If both conditions hold, we have:

xx and xx    x=x,x \leq x' \text{ and } x' \leq x \implies x = x', yy and yy    y=y.y \leq y' \text{ and } y' \leq y \implies y = y'.

Thus, (x,y)=(x,y)(x, y) = (x', y'), proving that RR is antisymmetric.


Step 4: Verify Transitivity

To check transitivity:

(x,y)R(x,y) and (x,y)R(x,y)    (x,y)R(x,y).(x, y) R (x', y') \text{ and } (x', y') R (x'', y'') \implies (x, y) R (x'', y'').

From the definition of RR:

(x,y)R(x,y)    xx and yy,(x, y) R (x', y') \iff x \leq x' \text{ and } y \leq y', (x,y)R(x,y)    xx and yy.(x', y') R (x'', y'') \iff x' \leq x'' \text{ and } y' \leq y''.

If both conditions hold, we have:

xx and xx    xx,x \leq x' \text{ and } x' \leq x'' \implies x \leq x'', yy and yy    yy.y \leq y' \text{ and } y' \leq y'' \implies y \leq y''.

Thus, (x,y)R(x,y)(x, y) R (x'', y''), proving that RR is transitive.


Step 5: Conclusion

Since RR satisfies reflexivity, antisymmetry, and transitivity, it is a partial order relation.


Now moving to 13 (ii):


Problem Statement:

Let RR be a relation defined on the set of positive integers as:

xRy    xy.xRy \iff x \leq y.

Prove that RR is a partial order relation.


Solution:

We follow the same steps as above:

  1. Reflexivity:
    For any xZ+x \in \mathbb{Z}^+, xxx \leq x. Thus, RR is reflexive.

  2. Antisymmetry:
    If x,yZ+x, y \in \mathbb{Z}^+ and xyx \leq y and yxy \leq x, then x=yx = y. Thus, RR is antisymmetric.

  3. Transitivity:
    If x,y,zZ+x, y, z \in \mathbb{Z}^+ and xyx \leq y and yzy \leq z, then xzx \leq z. Thus, RR is transitive.


Question 13 (ii) 

If r=xtan1(yx)+ytan1(xy),\text{If } r = x \tan^{-1}\left(\frac{y}{x}\right) + y \tan^{-1}\left(\frac{x}{y}\right),

show that:

rxy+ryx=r.\frac{\partial r}{\partial x} y + \frac{\partial r}{\partial y} x = r.


Solution

Let:

r=xtan1(yx)+ytan1(xy).r = x \tan^{-1}\left(\frac{y}{x}\right) + y \tan^{-1}\left(\frac{x}{y}\right).


Step 1: Find Partial Derivative of rr with Respect to xx

To compute rx\frac{\partial r}{\partial x}, treat yy as constant.

First term: xtan1(yx)x \tan^{-1}\left(\frac{y}{x}\right)

Using the product rule:

x[xtan1(yx)]=tan1(yx)+xddx[tan1(yx)].\frac{\partial}{\partial x} \left[x \tan^{-1}\left(\frac{y}{x}\right)\right] = \tan^{-1}\left(\frac{y}{x}\right) + x \cdot \frac{d}{dx}\left[\tan^{-1}\left(\frac{y}{x}\right)\right].

Now:

ddx[tan1(yx)]=11+(yx)2ddx(yx).\frac{d}{dx} \left[\tan^{-1}\left(\frac{y}{x}\right)\right] = \frac{1}{1 + \left(\frac{y}{x}\right)^2} \cdot \frac{d}{dx} \left(\frac{y}{x}\right). ddx(yx)=yx2.\frac{d}{dx} \left(\frac{y}{x}\right) = -\frac{y}{x^2}.

Thus:

ddx[tan1(yx)]=yx21+y2x2=y/x2(x2+y2)/x2=yx2+y2.\frac{d}{dx} \left[\tan^{-1}\left(\frac{y}{x}\right)\right] = \frac{-\frac{y}{x^2}}{1 + \frac{y^2}{x^2}} = -\frac{y/x^2}{(x^2 + y^2)/x^2} = -\frac{y}{x^2 + y^2}.

Now substitute back:

x[xtan1(yx)]=tan1(yx)xyx2+y2.\frac{\partial}{\partial x} \left[x \tan^{-1}\left(\frac{y}{x}\right)\right] = \tan^{-1}\left(\frac{y}{x}\right) - \frac{xy}{x^2 + y^2}.

Second term: ytan1(xy)y \tan^{-1}\left(\frac{x}{y}\right)

Since yy is treated as constant:

x[ytan1(xy)]=yddx[tan1(xy)].\frac{\partial}{\partial x} \left[y \tan^{-1}\left(\frac{x}{y}\right)\right] = y \cdot \frac{d}{dx}\left[\tan^{-1}\left(\frac{x}{y}\right)\right].

Now:

ddx[tan1(xy)]=11+(xy)21y.\frac{d}{dx} \left[\tan^{-1}\left(\frac{x}{y}\right)\right] = \frac{1}{1 + \left(\frac{x}{y}\right)^2} \cdot \frac{1}{y}. ddx[tan1(xy)]=1/y1+x2/y2=1y+x2y=yx2+y2.\frac{d}{dx} \left[\tan^{-1}\left(\frac{x}{y}\right)\right] = \frac{1/y}{1 + x^2/y^2} = \frac{1}{y + \frac{x^2}{y}} = \frac{y}{x^2 + y^2}.

Thus:

x[ytan1(xy)]=y2x2+y2.\frac{\partial}{\partial x} \left[y \tan^{-1}\left(\frac{x}{y}\right)\right] = \frac{y^2}{x^2 + y^2}.

Combine the two terms for rx\frac{\partial r}{\partial x}:

rx=tan1(yx)xyx2+y2+y2x2+y2.\frac{\partial r}{\partial x} = \tan^{-1}\left(\frac{y}{x}\right) - \frac{xy}{x^2 + y^2} + \frac{y^2}{x^2 + y^2}.


Step 2: Find Partial Derivative of rr with Respect to yy

The process for ry\frac{\partial r}{\partial y} is analogous. Treat xx as constant:

First term: xtan1(yx)x \tan^{-1}\left(\frac{y}{x}\right)

y[xtan1(yx)]=xddy[tan1(yx)].\frac{\partial}{\partial y} \left[x \tan^{-1}\left(\frac{y}{x}\right)\right] = x \cdot \frac{d}{dy}\left[\tan^{-1}\left(\frac{y}{x}\right)\right].

Now:

ddy[tan1(yx)]=11+(yx)21x.\frac{d}{dy} \left[\tan^{-1}\left(\frac{y}{x}\right)\right] = \frac{1}{1 + \left(\frac{y}{x}\right)^2} \cdot \frac{1}{x}. ddy[tan1(yx)]=1/x1+y2/x2=xx2+y2.\frac{d}{dy} \left[\tan^{-1}\left(\frac{y}{x}\right)\right] = \frac{1/x}{1 + y^2/x^2} = \frac{x}{x^2 + y^2}.

Thus:

y[xtan1(yx)]=x2x2+y2.\frac{\partial}{\partial y} \left[x \tan^{-1}\left(\frac{y}{x}\right)\right] = \frac{x^2}{x^2 + y^2}.

Second term: ytan1(xy)y \tan^{-1}\left(\frac{x}{y}\right)

Using the product rule:

y[ytan1(xy)]=tan1(xy)+yddy[tan1(xy)].\frac{\partial}{\partial y} \left[y \tan^{-1}\left(\frac{x}{y}\right)\right] = \tan^{-1}\left(\frac{x}{y}\right) + y \cdot \frac{d}{dy}\left[\tan^{-1}\left(\frac{x}{y}\right)\right].

Now:

ddy[tan1(xy)]=x/y21+(xy)2.\frac{d}{dy} \left[\tan^{-1}\left(\frac{x}{y}\right)\right] = \frac{-x/y^2}{1 + \left(\frac{x}{y}\right)^2}. ddy[tan1(xy)]=x/y2(x2+y2)/y2=xx2+y2.\frac{d}{dy} \left[\tan^{-1}\left(\frac{x}{y}\right)\right] = \frac{-x/y^2}{(x^2 + y^2)/y^2} = -\frac{x}{x^2 + y^2}.

Thus:

y[ytan1(xy)]=tan1(xy)xyx2+y2.\frac{\partial}{\partial y} \left[y \tan^{-1}\left(\frac{x}{y}\right)\right] = \tan^{-1}\left(\frac{x}{y}\right) - \frac{xy}{x^2 + y^2}.

Combine the two terms for ry\frac{\partial r}{\partial y}:

ry=x2x2+y2+tan1(xy)xyx2+y2.\frac{\partial r}{\partial y} = \frac{x^2}{x^2 + y^2} + \tan^{-1}\left(\frac{x}{y}\right) - \frac{xy}{x^2 + y^2}.


Step 3: Verify the Required Condition

We need to show:

rxy+ryx=r.\frac{\partial r}{\partial x} y + \frac{\partial r}{\partial y} x = r.




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