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Saturday, August 13, 2022

Chapter 8.1 - Binomial Theorem for Any Positive Integer

In the previous section, we saw the basic details about Pascal's triangle. We saw the necessity for developing a rule to find the various numbers in the Pascal's triangle. In this section, we will see such a rule.

The basics about the rule can be written in 6 steps:
1. We have seen the concept of combination in the previous chapter.
We saw the formula: nCr = n!r!(nr)!
2. Let us check whether this formula is applicable to the Pascal's triangle. The triangle is shown below for easy reference:

Any row in the Pascal's triangle can be written if the row above it is known.
Fig.8.2

The check can be done in 3 steps:
(i) Consider any coefficient in the Pascal's triangle, say the fourth coefficient for index 5
    ♦ The fourth coefficient of index 5 is 10
    ♦ 5C3 is also 10
(ii) Consider any other coefficient in the Pascal's triangle, say the third coefficient for index 7
    ♦ The third coefficient of index 7 is 21
    ♦ 7C2 is also 21
(iii) Let us check one more coefficient in the Pascal's triangle, say the fifth coefficient for index 8
    ♦ The fifth coefficient of index 8 is 70
    ♦ 8C4 is also 70
3. This gives us an idea to pick out any coefficient in the Pascal’s triangle:
The xth coefficient for any index n will be nCx-1
• For example, let n be 6 and x be 5
   ♦ Then the 5th coefficient of index 6 will be be 6C5-1 = 6C4 = 15
   ♦ From the Pascal's triangle, we see that, this is true.
4. Based on this information, the Pascal’s triangle can be modified as shown in fig.8.3 below:

Method to obtain any value in the Pascal's triangle.
Fig.8.3

• In the modified triangle, we see two points:
(i) In any row, the subscript on the right side of ‘C’ progressively increases in the order: 0, 1, 2, 3, . . . n
   ♦ Where n is the index of that row.
(ii) In any row, the superscript on the left side of ‘C’ does not change.
   ♦ It is equal to n, the index of the row.
5. The above two points give us an idea to quickly write any row of the Pascal’s triangle.
• For example, based on the two points, the row for index 12 will be:
12
C0, 12C1, 12C2, 12C3, 12C4, 12C5, 12C6, 12C7, 12C8, 12C9, 12C10, 12C11, 12C12
6. If we can write any row of the Pascal’s triangle quickly, we will be able to write the expansion corresponding to that index also quickly.
• Let us see an example:
Expand (a+b)7
Solution:
1. The coefficients will be:
7C0, 7C1, 7C2, 7C3, 7C4, 7C5, 7C6, and 7C7
2. So the expansion will be:
(a+b)7 =
7C0 a7 + 7C1 a6b1 + 7C2 a5b2 + 7C3 a4b3 + 7C4 a3b4 + 7C5 a2b5 + 7C6 a1b6  + 7C7 b7
• Remember that, the indices of a and b are calculated using the three peculiarities that we wrote in the previous section. They are given below for easy reference:

(i) The total number of terms in the expansion, is one more than the index.
(ii) Powers of the first quantity ‘a’ go on decreasing by 1 whereas the powers of the second quantity ‘b’ increase by 1, in the successive terms.
(iii) In each term of the expansion, the sum of the indices of a and b is the same and is equal to the index of (a+b).

• Thus we can write the complete expansion.


Now we can write the general form. It can be written in 3 steps:
(i) All the coefficients are of the form nCr
   ♦ For any particular problem, ‘n’ will be a constant.
         ✰ It will be equal to the index in the question.
   ♦ r will increase from 0 to n
(ii) The indices of a and b are calculated using the three peculiarities that we wrote in the previous section (also shown in the box above).
(iii) Based on this, the general form will be:
(a+b)n = nC0an + nC1an1b + nC2an2b2 + nC3an3b3 + . . . + nCn1abn1 + nCnbn


• Let us use this general form to expand (2x+5)6
We get:

(2x+5)6
=6C0(2x)650+6C1(2x)551+6C2(2x)452+6C3(2x)353+6C4(2x)254+6C5(2x)155+6C6(2x)056=6C026x650+6C125x551+6C224x452+6C323x353+6C422x254+6C521x155+6C620x056=6C0×64×x6×50+6C1×32×x5×51+6C2×16×x452+6C3×8×x3×53+6C4×4×x2×54+6C5×2×x155+6C6×1×x056=1×64×x6×50+6×32×x5×51+15×16×x4×52+20×8×x3×53+15×4×x2×54+6×2×x1×55+1×1×x0×56=1×64×x6×1+6×32×x5×5+15×16×x4×25+20×8×x3×125+15×4×x2×625+6×2×x1×3125+1×1×x0×15625=64x6+960x5+6000x4+20000x3+37500x2+37500x+15625


We have seen the general form. The RHS of that general form is a bit lengthy. It can be easily shortened as explained by the 4 steps below:

1. We see that, the RHS is a sum of a finite number of terms. So it is a summation.
• We can use the symbol '∑' (Greek upper case letter sigma) to denote summation. Thus the general form becomes:
(a+b)n = k=nk=0nCkankbk
2. We know that, for any particular problem, n will be a constant. It is the index.
3. k is not a constant. It takes different values in different terms.
• 'k=0' at the bottom of '∑' indicates that, the value of k starts from zero. In other words, the value of k in the first term is zero.
• 'k=n' at the top of '∑' indicates that, the value of k ends at n. In other words, the value of k in the last term is n.
• So the values of k are: 0, 1, 2, 3, . . . n
• It is known as the summation from k = 0 to k = n.
4. The index of a is (n-k). The index of b is k.
This shows that, the sum of the indices of a and b will be n in every term.


Let us see some special cases:
Case 1:
In this case, we investigate the expansion when the second quantity is -ve. This can be written in 3 steps:
1. Let us put a = x and b = -y. Then we get:
(a+b)n = (x-y)n = [x + (-y)]n
2. Expanding this using the general form, we get:
[x+(y)]n
=nC0xn(y)0+nC1xn1(y)1+nC2xn2(y)2+nC3xn3(y)3+. . . + nCnx0(y)n=nC0xn(1)0y0+nC1xn1(1)1y1+nC2xn2(1)2y2+nC3xn3(1)3y3+. . . + nCnx0(1)nyn
 = k=nk=0nCk(1)kxnkyk
3. Based on the above result, we can write:
(ab)n = k=nk=0nCk(1)kankbk

◼ Let us expand (x-2y)5 using this result. We get:
(x2y)5 = [x+(2y)]5 = k=5k=05Ck(1)kx6k(2y)k
• Once we write the sigma notation on the RHS, we will be able to write all the terms easily. We get:
(x2y)5
=5C0x5(1)0(2y)0+5C1x51(1)1(2y)1+5C2x52(1)2(2y)2+5C3x53(1)3(2y)3+5C4x54(1)4(2y)4+5C5x55(1)5(2y)5=1×x5×1×(2y)0+5×x4×1×(2y)+10×x3×1×(4y2)+10×x2×1×(8y3)+5×x1×1×(16y4)+1×x0×1×(32y5)=x510x4y+40x3y280x2y3+80xy432y5


Case 2:
In this case, we investigate the expansion when the first quantity is 1. This can be written in 3 steps:
1. Let us put a = 1 and b = x. Then we get:
(a+b)n = (1+x)n
2. Expanding this using the general form, we get:
(1+x)n
=nC01nx0+nC11n1x1+nC21n2x2+nC31n3x3+. . . + nCn10xn=nC01nx0+nC11n1x1+nC21n2x2+nC31n3x3+. . . + nCn10xn
= k=nk=0nCk1nkxk
3. So we can write:
(1+x)n = k=nk=0nCkxk
◼ Let us expand (1+2x)6 using this result. We get:
(1+2x)6 = k=6k=06Ck(2x)k
• Once we write the sigma notation on the RHS, we will be able to write all the terms easily. We get:
(1+2x)6
=6C016(2x)0+6C1(2x)1+6C2(2x)2+6C3(2x)3+6C4(2x)4+6C5(2x)5+6C6(2x)6=1×(2x)0+6×(2x)+15×(4x2)+20×(8x3)+15×(16x4)+6×(32x5)+1×(64x6)=1+12x+60x2+160x3+240x4+192x5+64x6

◼ x = 1 is a special case coming under this category. We get:
(1+x)n = (1+1)n = 2n = k=6k=0nCkxk = k=6k=0nCk1k = k=6k=0nCk
• Once we write the sigma notation on the RHS, we will be able to write all the terms easily. We get:
= nC0 + nC1 + nC2 + nC3 + . . . + nCn
• So we can write:
2n = nC0 + nC1 + nC2 + nC3 + . . . + nCn  


Case 3:
In this case, we investigate the expansion when the first quantity is 1 and the second quantity is -ve. This can be written in 3 steps:
1. Let us put a = 1 and b = -x. Then we get:
(a+b)n = (1-x)n = [1 + (-x)]n
2. Expanding this using the general form, we get:
[1+(x)]n
=nC01n(x)0+nC11n1(x)1+nC21n2(x)2+nC31n3(x)3+. . . + nCn10(x)n=nC01n(1)0x0+nC11n1(1)1x1+nC21n2(1)2x2+nC31n3(1)3x3+. . . + nCn10(1)nxn
= k=nk=0nCk(1)k1nkxk
3. Based on the above result, we can write:
(1x)n = k=nk=0nCk(1)kxk

◼ Let us expand (1-2x)5 using this result. We get:
(12x)5 = [1+(2x)]5 = k=5k=05Ck(1)k(2x)k
• Once we write the sigma notation on the RHS, we will be able to write all the terms easily. We get:
(12x)5
=5C0(1)0(2x)0+5C1(1)1(2x)1+5C2(1)2(2x)2+5C3(1)3(2x)3+5C4(1)4(2x)4+5C5(1)5(2x)5=1×1×(2x)0+5×1×(2x)+10×1×(4x2)+10×1×(8x3)+5×1×(16x4)+1×1×(32x5)=110x+40x280x3+80x432x5

• We wrote: (1x)n = k=nk=0nCk(1)kxk
◼ x = 1 is a special case coming under this category. We get:
(1x)n = (11)n = 0n = k=nk=0nCk(1)k1k = k=nk=0nCk(1)k
• Once we write the sigma notation on the RHS, we will be able to write all the terms easily. We get:
= nC0(1)0 + nC1(1)1 + nC2(1)2 + nC3 + . . . + nCn(1)n
• So we can write:
0n = nC0  nC1 + nC2  nC3 + . . . + (1)n × nCn


In the next section we will see some solved examples.

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