Section-A of the paper:
1. Define complement of a set with an example.
Definition:
The complement of a set (denoted as ) is the set of all elements in the universal set that are not in . Mathematically:
Example:
Let the universal set and .
The complement of , , because these elements are in but not in .
2. Define equivalence relations and partial order relation functions.
Equivalence Relation:
A relation on a set is called an equivalence relation if it satisfies the following three properties:
- Reflexive:
- Symmetric:
- Transitive:
Example:
The relation on integers is an equivalence relation.
Partial Order Relation:
A relation on a set is called a partial order relation if it satisfies:
- Reflexive:
- Antisymmetric:
- Transitive:
Example:
The relation (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 is a homogeneous function of degree , then:
Proof:
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A function is homogeneous of degree if:
for any scalar .
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Differentiating both sides with respect to , we get:
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Using the chain rule:
Substituting , , and :
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For , this simplifies to:
4. Draw the Hasse diagram for the partial ordering on the power set for .
Solution:
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The power set for is:
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The relation 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 at the bottom, as it is the smallest set.
- Draw edges upwards to the sets that include one element: .
- Continue upwards to sets with two elements: .
- Finally, place at the top.
(Hasse diagram will be a visual, which cannot be drawn in text form here.)
5. Evaluate .
Solution:
The given integral is:
-
Solve the inner integral:
- For the first term:
- For the second term:
Combining both terms:
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Now, solve the outer integral:
- For :
- For :
Adding both results:
Final Answer:
Section-B of the paper:
6. Show that the lines and are coplanar. Find the equation of the plane containing them.
Solution:
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Parametric equations of the lines:
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For the first line:
Let this be line .
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For the second line:
Let this be line .
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Direction vectors of the lines:
- For , direction vector is .
- For , direction vector is .
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A point on each line:
- Point on : .
- Point on : .
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Vector joining the points and :
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Check coplanarity:
The lines are coplanar if the scalar triple product of is zero. The scalar triple product is:
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First, compute :
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Now compute :
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:
Solution:
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Understand the integration limits:
- The outer integral has ranging from to .
- The inner integral has ranging from to .
- This describes the region where and .
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Change the order of integration:
The new limits must describe the same region:
- ranges from to (from the diagram of the region).
- For a fixed , ranges from to .
Thus, the new integral is:
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Evaluate the inner integral:
So the inner integral becomes:
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Evaluate the outer integral:
- For :
- For :
Combine the results:
Final Answer:
8. If are three functions such that , show that the composition of functions is not necessarily commutative.
Solution:
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Associativity of composition:
The given condition states that function composition is associative:
This property always holds true for function composition.
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Non-commutativity:
To prove that composition is not commutative, we need to find functions and such that .
Example:
Let:
Compute and :
Since , 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:
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Definition of a Lattice:
A lattice is an algebraic structure , where (join) and (meet) satisfy:
- Commutativity
- Associativity
- Absorption laws
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Dual of a Lattice:
The dual of a lattice is obtained by interchanging the operations and , meaning:
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Show the Dual is a Lattice:
To prove that the dual structure is also a lattice, we need to verify that the dual operations and (reversed) satisfy:
- Commutativity:
Since the original lattice satisfies commutativity, the dual does as well.
- Associativity:
The original lattice satisfies associativity, so the dual does as well.
- Absorption laws:
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 is a lattice with operation and , for any , show that:
Solution:
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Property 1: Commutativity of :
The meet operation is defined as:
Since and are symmetric, it follows that:
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Property 2: Commutativity of :
The join operation is defined as:
Since and are symmetric, it follows that:
Thus, both operations and are commutative.
10. (i) If , show that:
Solution:
Let .
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Partial derivatives of :
- For :
- For :
Thus:
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Multiply :
- Substitute:
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Simplify and verify:
Since is a property of homogeneous functions, the equation is satisfied by the given function .
11. (i) Find the maximum or minimum values of the function .
Solution:
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Given function:
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Find critical points:
Take partial derivatives with respect to and :
- ,
- .
Set and :
- ,
- .
Solve and :
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Determine maximum or minimum:
Compute the second partial derivatives:
The Hessian determinant is:
Since , the critical point is a saddle point. No maximum or minimum exists.
12. (i) Show that , given the region of integration.
Solution Outline:
The integral is over a specific region bounded by planes .
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Set up limits of integration:
- ranges from to ,
- ranges from to ,
- ranges from to .
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Integrate step by step:
The integral is:
Perform the remaining steps to evaluate the triple integral, and you will find:
We are tasked with evaluating the triple integral:
where the region of integration is bounded by the planes , and .
Step 1: Define the Region of Integration
The region is the tetrahedron formed by:
- ,
- .
The limits of integration are:
- ranges from to ,
- For a fixed , ranges from to ,
- For fixed and , ranges from to .
Thus, the integral becomes:
Step 2: Evaluate the Integral with Respect to
The inner integral is:
Since is independent of , we treat it as a constant:
Substitute this result into the integral:
Step 3: Evaluate the Integral with Respect to
Now consider:
Expand :
The integral becomes:
Separate the terms:
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First Term:
The integral of is:
So:
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Second Term:
The integral of is:
So:
Combine the two terms:
Simplify:
So:
Step 4: Evaluate the Integral with Respect to
Now substitute into the integral:
Factor out :
Expand :
So:
The integral becomes:
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First Term:
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Second Term:
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Third Term:
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Fourth Term:
Substitute these values:
Simplify:
Combine fractions:
Step 5: Final Answer
Now multiply by :
Thus, the value of the triple integral is:
Here is the solution for 12 (ii):
Problem Statement:
For any sets and , define:
Given A={1,2}A = \{1, 2\} and B={2,3,4}B = \{2, 3, 4\}:
- What is ∣AB∣|AB|?
- What is ∣A∣⋅∣B∣|A| \cdot |B|?
Step 1: Compute ABAB
From the definition:
AB={ab ∣ a∈A,b∈B}.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:
- For a=1a = 1 in AA:
{1⋅2,1⋅3,1⋅4}={2,3,4}.\{1 \cdot 2, 1 \cdot 3, 1 \cdot 4\} = \{2, 3, 4\}.
- For a=2a = 2 in AA:
{2⋅2,2⋅3,2⋅4}={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 ∣A∣⋅∣B∣|A| \cdot |B|
The cardinalities of AA and BB are:
∣A∣=2,∣B∣=3.|A| = 2, \quad |B| = 3.
Thus:
∣A∣⋅∣B∣=2⋅3=6.|A| \cdot |B| = 2 \cdot 3 = 6.
Step 4: Final Answer
- ∣AB∣=5|AB| = 5,
- ∣A∣⋅∣B∣=6|A| \cdot |B| = 6.
This demonstrates that ∣AB∣≠∣A∣⋅∣B∣|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′) ⟺ x≤x′ and y≤y′(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:
- Reflexive: For all a∈Sa \in S, aRaa R a.
- Antisymmetric: For all a,b∈Sa, b \in S, if aRba R b and bRab R a, then a=ba = b.
- Transitive: For all a,b,c∈Sa, 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) ⟺ x≤x and y≤y.(x, y) R (x, y) \iff x \leq x \text{ and } y \leq y.
This is always true because x≤xx \leq x and y≤yy \leq y hold for all x,y∈R2x, 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′) ⟺ x≤x′ and y≤y′,(x, y) R (x', y') \iff x \leq x' \text{ and } y \leq y',
(x′,y′)R(x,y) ⟺ x′≤x and y′≤y.(x', y') R (x, y) \iff x' \leq x \text{ and } y' \leq y.
If both conditions hold, we have:
x≤x′ and x′≤x ⟹ x=x′,x \leq x' \text{ and } x' \leq x \implies x = x',
y≤y′ and y′≤y ⟹ 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′) ⟺ x≤x′ and y≤y′,(x, y) R (x', y') \iff x \leq x' \text{ and } y \leq y',
(x′,y′)R(x′′,y′′) ⟺ x′≤x′′ and y′≤y′′.(x', y') R (x'', y'') \iff x' \leq x'' \text{ and } y' \leq y''.
If both conditions hold, we have:
x≤x′ and x′≤x′′ ⟹ x≤x′′,x \leq x' \text{ and } x' \leq x'' \implies x \leq x'',
y≤y′ and y′≤y′′ ⟹ y≤y′′.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 ⟺ x≤y.xRy \iff x \leq y.
Prove that RR is a partial order relation.
Solution:
We follow the same steps as above:
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Reflexivity:
For any x∈Z+x \in \mathbb{Z}^+, x≤xx \leq x. Thus, RR is reflexive.
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Antisymmetry:
If x,y∈Z+x, y \in \mathbb{Z}^+ and x≤yx \leq y and y≤xy \leq x, then x=yx = y. Thus, RR is antisymmetric.
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Transitivity:
If x,y,z∈Z+x, y, z \in \mathbb{Z}^+ and x≤yx \leq y and y≤zy \leq z, then x≤zx \leq z. Thus, RR is transitive.
Question 13 (ii)
If r=xtan−1(yx)+ytan−1(xy),\text{If } r = x \tan^{-1}\left(\frac{y}{x}\right) + y \tan^{-1}\left(\frac{x}{y}\right),
show that:
∂r∂xy+∂r∂yx=r.\frac{\partial r}{\partial x} y + \frac{\partial r}{\partial y} x = r.
Solution
Let:
r=xtan−1(yx)+ytan−1(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 ∂r∂x\frac{\partial r}{\partial x}, treat yy as constant.
First term: xtan−1(yx)x \tan^{-1}\left(\frac{y}{x}\right)
Using the product rule:
∂∂x[xtan−1(yx)]=tan−1(yx)+x⋅ddx[tan−1(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[tan−1(yx)]=11+(yx)2⋅ddx(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[tan−1(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[xtan−1(yx)]=tan−1(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: ytan−1(xy)y \tan^{-1}\left(\frac{x}{y}\right)
Since yy is treated as constant:
∂∂x[ytan−1(xy)]=y⋅ddx[tan−1(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[tan−1(xy)]=11+(xy)2⋅1y.\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[tan−1(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[ytan−1(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 ∂r∂x\frac{\partial r}{\partial x}:
∂r∂x=tan−1(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 ∂r∂y\frac{\partial r}{\partial y} is analogous. Treat xx as constant:
First term: xtan−1(yx)x \tan^{-1}\left(\frac{y}{x}\right)
∂∂y[xtan−1(yx)]=x⋅ddy[tan−1(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[tan−1(yx)]=11+(yx)2⋅1x.\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[tan−1(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[xtan−1(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: ytan−1(xy)y \tan^{-1}\left(\frac{x}{y}\right)
Using the product rule:
∂∂y[ytan−1(xy)]=tan−1(xy)+y⋅ddy[tan−1(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[tan−1(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[tan−1(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[ytan−1(xy)]=tan−1(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 ∂r∂y\frac{\partial r}{\partial y}:
∂r∂y=x2x2+y2+tan−1(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:
∂r∂xy+∂r∂yx=r.\frac{\partial r}{\partial x} y + \frac{\partial r}{\partial y} x = r.
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