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    Elementary Triangle GeometryMark Dabbs

    The Mathematical Association ConferenceUniversity of York, U.K

    Spring 2004

    Version 1.1 April 2004(www.mfdabbs.com)

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    Contents

    Motivating Problem. 5

    1: Basic Trigonometrical Formulae. 11

    2: Further Trigonometrical Formulae. 13

    3: Ratio Theorems. 15Theorem (3.1).

    Theorem (3.2).

    4: Basic Triangle Formulae. 17Cosine Rule.Sine Rule and Cicumcircle.

    Tangent Rule.

    5: Other Triangle Formulae. 21Area Formulae in terms ofa, band c.

    Sin A, sin B and sin C in terms ofa, band c.

    Cos A, cos B and cos C in terms ofa, band c.

    Tan A, tan B and tan C in terms ofa, band c.

    6: Associated Circles. 25Incircle.

    Excircles.Herons Area Formula.

    7: Further Triangle Formulae. 33

    ( ) ( ) ( )1 12 2 2an , tan and tan in terms of , and .A B C a b c ( ) ( ) ( )1 12 2 2os , cos and cos in terms of , and .A B C a b c ( ) ( ) ( )1 12 2 2in , sin and sin in terms of , and .A B C a b c

    8: Further Triangle Relationships. 37

    elationship between and .Rr elationships between , , and .

    A B Cr r r R

    he distances A , and C .I BI I he distances A , and C .

    A B CI BI I

    he distances , and .A B C

    II II II

    9: Further Triangle Centres. 47The Orthocentre of any Triangle ABC.

    The Pedal Triangle of any Triangle ABC.

    The Circumcircle and the Pedal Triangle.The Excentric Triangle.

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    10: Special Cevian Lengths. 55The Centroid and Medians of any Triangle.

    Cevians Bisecting Angles Internally.

    Cevians Bisecting Angles Externally.

    Apollonius Theorem.A Generalisation of Apollonius Theorem Stewarts Theorem

    11: Problems. 63

    Appendix: Concurrences of Straight Lines in a Triangle. 67Circumcentre.

    Incentre.

    Centroid.

    Orthocentre.

    Bibliography. 73

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    Motivating Problem

    a ch

    x b - x

    PC

    B

    A

    The motivation for this work came from an open question to a class to find the

    area of a triangle whose base is known but whose perpendicular height is not

    known.A typical diagram is shown in Figure MP.1

    Figure MP.1

    The area of the triangle, , is seen to be

    ( ) ( )12

    12

    base height

    ,bh

    =

    =(MP.1)

    where and h .b AC= BP=

    After some discussion, two methods were proposed

    o Method 1: Using Trigonometry

    o Method 2: Using Pythagoras

    Method 1 is perhaps the more familiar and progresses thus:

    In triangle BPCwe have:

    sin

    sin

    PBC

    BC

    h

    C a

    =

    =

    Therefore, sinh a C= (MP.2)

    From (MP.1) and (MP.2) we have the general area formula

    12 sinab C = (MP.3)

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    Method 2 was somewhat more involved and led to quite a voyage of discovery!

    Note the following Pythagorean relations within the two triangles CBPand ABP.

    2 2

    a x h

    2

    = + (MP.4)and ( )

    22c b x h2= + . (MP.5)

    Eliminating hfrom (MP.4) and (MP.5) gives:

    ( )22 2 2a x c b x =

    That is: .( )22 2 2a c x b x =

    Thus, by the difference of two squares formula we have

    ( ) ( )

    ( )(

    ( ) ( )

    2 2

    2 2

    2 2 2

    a c x b x x b x

    a c x b x x b x

    a c x b b

    = +

    = + +

    =

    )

    Hence,2 2

    2

    a b cx

    b

    2+ = . (MP.6)

    Substituting (MP.6) into (MP.4) gives22 2 2

    2 2

    2

    a b ch a

    b

    + =

    .

    That is

    ( )22 2 2 2 2

    2

    2

    4

    4

    a b a b ch

    b

    + = (MP.7)

    Once again, by the difference of two squares formula we have the alternative form

    of(MP.7):

    ( )( )2 2 2 2 2 22

    2

    2 2

    4

    ab a b c ab a b ch

    b

    + + + = ,

    ( ) ( )2 2 2 2 2 22

    2 2

    4

    ab a b c ab a b c

    b

    + + + = ,

    ( ) ( )2 2 2 2 2 2

    22 2

    4c a ab b a ab b c

    b + + + = ,

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    That is:

    ( )( )2 2 2 2 2 22

    2

    2 2

    4

    c a ab b a ab b ch

    b

    + + + = ,

    which, on factorising gives:

    ( )( ) ( )( )2 22 22

    24

    c a b a b ch

    b

    + = .

    Therefore, on using the difference of two squares formula again we have:

    ( )( ) ( ) ( )22

    4

    c a b c a b a b c a b ch

    b

    + + + +=

    ( )( )( ) ( )224

    c a b c a b a b c a b ch

    b

    + + + + += . (MP.8)

    Now its time to ask which of the four factors in the numerator looks the nicest

    and hope that the answer to come back is the fourth or last one of ( ) !a b c+ +

    Having established this, the suggestion is then made that it is a pity that the other

    three factors do not have this same elegant symmetry and once agreed that we

    ought to insistthat such symmetry exist in these other three factors.

    It is eventually determined that a suitable trick is to rewrite them in the

    following manner:

    ( ) ( )

    ( ) (

    ( ) (

    2

    2

    2

    c a b a b c a

    c a b a b c b

    a b c a b c c

    + + +

    + + +

    + + +

    )

    )

    )

    (MP.9)

    Realising that (a b c+ + is just the perimeter of the original triangle ABC, sayp

    gives (MP.8) as:

    ( )( )( )( )22

    2 2 2

    4

    p a p b p c ph

    b

    = . (MP.10)

    However, if we then let the new variable, s, be defined as the semi-perimeterthen

    (MP.10) is re-written

    ( ) ( ) ( ) ( )22

    2 2 2 2 2 2 2

    4

    s a s b s c sh

    b

    = .

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    This is then easily factorised to give:

    ( )( )( )( )22

    16

    4

    s a s b s c sh

    b

    =

    or( )( )( )2

    2

    4s s a s b s ch

    b

    = .

    Hence,( )( ) ( )2 s s a s b s c

    hb

    = (MP.11)

    Finally then, substituting (MP.11) back into (MP.1) gives

    ( )( ) ( )12 2 s s a s b s cbb

    =

    or

    (MP.12)( )( )( )s s a s b s c =

    Which is the familiar result of Heron of Alexandria (First Century A.D)

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    What a marvel that so simple a figure as the triangle is so

    inexhaustible in its properties!

    (A. L. Crelle, 1821)

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    1: Basic Trigonometrical Formulae

    sintan

    cos

    = (1.1)

    2 2sin cos 1 + = (1.2)

    0 30 45 60 90

    sin 01

    2

    2

    2

    3

    2 1

    cos 13

    2

    2

    2

    1

    2

    0

    (1.3)

    tan 01

    3 1 3

    1cosec

    sin1

    seccos

    1cot

    tan

    =

    =

    =

    (1.4)

    2tan 1 sec2 + = (1.5)

    21 cot cosec2 + = (1.6)

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    2: Further Trigonometrical Formulae

    (2.1)( )sin sin cos cos sinA B A B A B+ = +

    (2.2)( )sin sin cos cos sinA B A B A B =

    (2.3)( )cos cos cos sin sinA B A B A B+ =

    (2.4)( )cos cos cos sin sinA B A B A B = +

    ( )tan tan

    tan1 tan tan

    AA B

    A B

    B++ =

    (2.5)

    ( )tan tan

    tan1 tan tan

    AA B

    A B

    B =

    +(2.6)

    sin sin 2sin cos2 2

    P Q P QP Q

    + + =

    (2.7)

    sin sin 2cos sin2 2

    P Q P QP Q

    + =

    (2.8)

    cos cos 2cos cos2 2

    P Q P QP Q

    + + =

    (2.9)

    cos cos 2sin sin2 2

    P Q P QP Q

    + =

    (2.10)

    ( )sin 2 2sin cosA A A= (2.11)

    (2.12)( ) 2 2 2cos 2 cos sin 2cos 1 1 2sinA A A A= = = 2A

    ( )( )2 12sin 1 cos 2A = A (2.13)

    ( )( )2 12cos 1 cos 2A = + A (2.14)

    Notice further, if we define 12tant = then it can be shown that

    2

    2 2

    2 1sin , cos and tan .

    1 1

    t t

    t t

    = = =

    + +2

    2

    1

    t

    t

    (2.15)

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    3: Ratio Theorems

    Theorem (3.1)If we have that p a

    q b= then p q a , for any numbersb

    mp nq ma nb + +=

    + +, , and .m n

    Proof:

    Letp a

    tq b

    =

    , .p qt a bt= =

    Therefore, ( )( )qt qp q t

    mp nq m qt nq mt n ++ += =+ + +

    and

    ( )

    ( )

    bt qa b t

    ma nb m bt nq mt n

    ++ += =

    + + +

    Theorem (3.2)

    If we have that then , for any numbersp aq b=

    p a p aq b q b

    += =+

    and .

    Proof:

    Letp a

    tq b

    =

    , .p qt a bt= =

    Therefore,( ) ( ) ( )

    ( )

    qt bt t q bp a ptq b q b q b q

    a

    b

    + ++

    = = = + + +

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    c ah

    b

    x y

    A

    B

    C

    4: Basic Triangle Formulae

    Cosine Rule

    Figure 4.1

    Notice that: cos , cosx y

    A Cc a

    = =

    Therefore, cos , cosx c A y a C= =

    Hence cos cosb x y c A a C = + +

    Using symmetry we interchange the variables to yield the complete set of results

    thus:cos cos

    cos cos

    cos cos

    a b C c B

    b c A a C

    c a B b A

    = +

    = +

    = +

    (4.1)

    The formulae of(4.1) are known as the Projection Formulae.If we now multiply the equations of(4.1) by a, band c, respectively, we have:

    (4.2)2 cos cosa ab C ac= + B

    A

    A

    (4.3)2 cos cosb bc A ab C = +

    (4.4)2 cos cosc ac B bc= +

    Now construct (4.3) + (4.4) - (4.2) to give:

    2 2 2 2 cosb c a bc+ =

    Therefore,

    (4.5)2 2 2 2 cosa b c bc= + A

    a

    bc

    Equation (4.5) is known as the Cosine Rule for triangles.Symmetry yields the other forms:

    2 2 2 2 2 22 cos and 2 cosb c a ca B c a b ab= + = + C

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    Sine RuleAlso from Figure 4.1 we have the further set of relations:

    sin , sinh h

    A C

    c a

    = =

    Therefore, sin or sinh c A h a C = =

    Hence, sin sinc A a C h=

    Therefore,sin sinA C

    a c=

    However, the initial orientation of the triangle ABC was arbitrary

    (4.6)sin sin sinA B C

    a b c= =

    Equation (4.6) is known as the Sine Rule for triangles.The Sine Rule can be extended by considering a circle through the apexes of the

    triangle ABC (known as the Circumcircleof the triangle ABC)

    P

    P

    OO

    B

    A C

    A

    B

    C

    Figure 4.2 Figure 4.3

    In both Figure 4.2 and 4.3 the red lines AP and PC have been added to the

    original Circumcircle problem. In both cases the line segment AP is draw so as to

    pass through the centre of the Circumcircle and is therefore a diameter.

    ACP is a Right-Angle in both figures (Angle in a Semi-Circle is a right-

    angle).

    Further, APC = ABC since angles subtended by a single chord in the same

    segment of a circle are equal (Euclid Book III Prop. 21).

    Therefore, from Figure 4.2 we have: ( ) ( )sin sin2

    AC bAPC BAP R

    =

    where Ris the radius of the Circumcircle of triangle ABC.

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    From Figure 4.3 180APC B= (Cyclic Quadrilateral)

    Therefore, ( ) ( )sin sin 180 sinAPC B B=

    Hence, as for Figure 4.2 we have

    sin 1sin or

    2 2

    b BB

    R b R= =

    Therefore, from (4.6) we have:

    sin sin sin 1

    2

    A B C

    a b c(4.7)

    R= = =

    Tangent RuleFrom (4.7) we have that

    sin

    sin

    b

    c C=

    B

    Using Theorem (3.1) with and1 1m n = = this relation can be written

    ( )

    ( )

    ( ) ( )

    ( ) ( )

    sin1 sin

    1 1 in

    1

    s

    1B

    C

    + +

    +

    =

    +

    ( )

    ( )

    1

    1 1 sin

    b c

    b c B

    C

    That issin sin

    sin sin

    b c B C

    b c B C

    =

    + +

    Using (2.8) and (2.7) this can be rewritten as

    2cos sin2 2

    ,

    2sin cos

    2 2

    sin12

    ,

    cos sin2 2

    cos2

    tan

    2 .tan

    2

    B C B C

    b c

    B C B Cb c

    B C

    b c

    B C B Cb c

    B C

    B C

    b c

    B Cb c

    + =

    + +

    =

    ++

    +

    = ++

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    That is ( ) ( )1 12 2tan tanb c

    B C Bb c

    C

    =+

    + (4.8)

    However, 180A B C+ + = ( )12 9012B C+ =

    A (4.9)

    From (4.9) we see that

    ( ) ( )

    ( )

    1 12 2

    12

    12

    12

    12

    12

    1 12 2

    tan tan 90

    tan(90 ) tan

    1 tan(90 ) tan

    tan1

    tan(90 )1

    tantan(90 )

    1 00 tan

    tan cot

    B C A

    A

    A

    A

    A

    A

    B C A

    + =

    =

    +

    =+

    =+

    + =

    Hence (4.8) can be written in its alternative form

    (4.10)( )12tan cotb c

    B Cb c

    =

    +12 A

    Equation (4.10) is known as the Tangent Rule for triangles.Symmetry yields the other forms:

    ( )

    ( )

    1 12 2

    1 12 2

    tan cot

    tan cot

    c aC A B

    c a

    a bA B C

    a b

    =

    +

    =

    +

    a

    bc

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    5: Other Triangle Formulae

    c ah

    b

    A

    B

    C

    Area Formulae in terms of a, band c.

    Figure 5.1

    The area of triangle ABCis found from

    ( )

    12

    12

    , where sin ,

    sin

    hbh C

    ab a C

    = =

    =

    Hence, 12 sinab C = (5.1)a

    a

    bc

    By symmetry, 1 1 12 2 2sin sin sinab C bc A ca B = = =

    From (4.7) we have that sin2

    cC

    R=

    Therefore, (5.1) becomes 122

    cab

    R

    =

    That is:4

    abc

    R = (5.2)

    bc

    or4

    abcR =

    .

    Also, from (4.7) we have that sinsin

    a BbA=

    Therefore, (5.1) now becomes:

    12

    sinsin

    sin

    a Ba C

    A

    =

    That is: 212sin sin

    sin

    B Ca

    A =

    Hence,

    2 2 21 1 12 2 2

    sin sin sin sin sin sin

    sin sin sin

    B C C A Aa b c

    A B = = =

    B

    C(5.3)

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    SinA in terms of a, band c, etc.From (1.2)

    ( ) ( )( ) (

    2 2

    2 2

    sin 1 cos

    1 cos

    1 cos 1 cos

    A A

    A

    A A

    =

    = = + )

    Therefore, from (4.5) this becomes

    ( )

    2 2 2 2 2 22

    2 2 2 2 2 2

    2 2 2 2 2 2

    2 2 2 2 2 2

    22

    sin 1 12 2

    2 2

    2 2

    2 2

    2 2

    2 2

    2 2

    2

    b c a b c aA

    bc bc

    bc b c a bc b c a

    bc bc

    bc b c a bc b c a

    bc bc

    a b bc c b bc c a

    bc bc

    a b c

    bc

    + + = +

    + + + =

    + + + =

    + + + =

    =

    ( )

    ( )( ) ( )( )

    ( )( )( )( )

    ( )( ) ( )(

    2 2

    2 22 2

    2 2

    2 2

    2 2

    2

    1

    4

    1

    41

    2 2 24

    b c a

    bc

    a b c b c ab c

    a b c a b c b c a b c ab c

    a b c b a b c c b c a a b c ab c

    +

    = +

    = + + + + +

    = + + + + + + + )+

    Now let (12s a b= + + )c , the Semi-perimeter, then we have

    ( )( )( )( )

    ( )( )( )( )

    2

    2 2

    2 2

    1sin 2 2 2 2 2 2 2

    4

    1 164

    A s b s c s ab c

    s b s c s a sb c

    =

    =

    s

    Hence

    ( )( )(22 2

    4sin A s s a s b s

    b c= )c

    Therefore,

    ( )( )( )2

    sin A s s a s b s cbc

    =

    ( )( )( )

    2

    sinB s s a s b s cca=

    ( )( )( )2

    sinC s s a s b s cab

    =

    (5.4)

    a

    bc

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    Notice further that these three identities from (5.4) could be written

    ( )( )( )

    ( )( )( )

    ( )( )( )

    2sin 2

    2sin 2

    2sin 2

    A s s a s b s c

    B s s a s b s c Ka

    aa

    C s s a s b s cab

    bb

    cc

    =

    =

    =

    (5.5)

    Kbca

    cb

    cK

    From which, the Sine Rule can be deduced, sincesin sin sin 1

    22

    A B CK

    a b c

    = = R

    Moreover, from (5.1) and (5.4) we have that

    ( )( )( )1 12 22

    sinab C ab s s a s b s cab

    =

    Hence

    (5.6)( )( )( )s s a s b s c =

    This is the triangle area formula met previously in (MP.7): Herons Formula.

    We can now use the notation of(5.6) or more simply the form of(5.1) to write:

    SinA, sinB, sin C in terms of a, band c.

    a

    bc

    (5.7)

    2 2n , sin , sinA B C

    bc ca ab

    = = =si

    a

    bc

    2

    CosA, cosB, cos C in terms of a, band c.From (4.5) we simply rearrange to yield

    (5.8)2 2 2 2 2 2 2 2 2

    , cos , cos2 2

    b c a c a b a b cA B C

    bc ca ab

    + + + = = =cos

    2

    a

    bc

    TanA, tanB, tan C in terms of a, band c.From (1.1), (5.5) and (5.8) we have

    (5.9)2 2 2 2 2 2 2 2 2

    4 4tan , tan , tanA B C

    b c a c a b a b c

    = = =

    + + +

    4

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    6: Associated Circles

    EF

    D

    I

    BC

    A

    IncircleLet I be the Incentre of thetriangle ABC, obtained by

    bisecting the interior angles of

    the triangle ABC. Then

    ,ID IE IF r= =

    ( , and areID IE IF

    where ris the

    radius of the incircle.

    .the 's

    from to the respective sides)I Figure 6.1

    We have that( )

    ( )

    1 1 12 2 2

    12

    Area of triangle Areas of trianglesABC BIC CIA AIB

    ar br cr

    r a b c

    = +

    = + +

    = + +

    +

    Hence fors, the semi perimeter

    rs = (6.1)

    or r

    s

    = (6.2)

    Now, let

    AE AF x

    BD BF y

    CD CE z

    =

    = = =

    Tangents to a circle from

    a single point have equal

    lengths

    ( )perimeterx y y z z x p+ + + + + =

    Hence

    ( )semi perimeterx y z s+ + =

    But BD DC y z a+ = +

    a s+ =

    Hence x s a= .

    Therefore, we can show:s a

    y s bz s c

    =

    = =

    (6.3)

    a

    bc

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    From triangle ABC we see that

    ( )12ntaIF r

    AFA s a

    = =

    Similarly( )

    ( )

    ( )

    12

    12

    12

    tan

    n

    tan

    rA

    s a

    rB

    s b

    rC

    s c

    =

    =

    =

    ta (6.4)

    Moreover, from triangles AIE, BIF and CID we have

    ( )

    (

    ( )

    12

    12

    12

    cot

    cot

    cot

    AE AF s a r A

    BD BF s b r B

    CD CE s c r C

    = =

    = =

    = =

    (6.5))

    Figure 6.2

    s - bs - c

    s - c

    s - as - a

    s - b

    E

    F

    D

    I

    B

    C

    A

    a

    bc

    a

    bc

    Therefore, as thena BD DC = +

    ( ) ( )( ) ( )( )

    ( )

    ( )

    ( )

    ( )

    ( ) ( ) ( ) ( )

    ( ) ( )

    ( )

    ( ) ( )

    1 1

    2 2

    1 12 2

    1 12 2

    1 12 2

    1 1 1 12 2 2 2

    1 12 2

    1 12 2

    1 12 2

    cot cotcot cot

    cos cos

    sin sin

    cos sin sin cos

    sin sin

    sin

    sin sin

    a r B r C r B C

    B Cr

    B C

    B C Br

    B C

    B Cr

    B C

    = +

    = +

    = +

    +=

    +=

    C

    But and therefore,180A B C+ + = 1 1 12 2 290B C A+ = , giving

    ( )( ) ( )

    12

    1 12 2

    sin 90

    sin sin

    Aa r

    B C

    =

    That is

    ( )

    ( ) ( )

    12

    1 12 2

    cos

    sin sin

    Aa r

    B C= .

    Hence( ) ( )

    ( )

    1 12 2

    12

    sin sin

    cos

    B Cr a

    A= (6.6)

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    Together, we have

    ( ) ( )

    ( )

    ( ) ( )( )

    ( ) ( )

    ( )

    1 12 2

    12

    1 12 2

    12

    1 12 2

    12

    sin sin

    cos

    sin sin

    cos

    sin sin

    cos

    B Cr a

    A

    C Ar b

    B

    A Br c

    C

    =

    =

    =

    (6.7)

    From (4.7) we have

    sin 1

    2

    A

    a R= , etc, where Ris the Circumcircle.

    or

    a R2 sin A= , etc

    Thus (6.6) becomes

    ( ) ( )

    ( )

    1 12 2

    12

    sin sin2 sin

    cos

    B Cr R A

    A=

    Using (2.11) gives

    ( ) ( )( ) ( )

    ( )

    1 12 21 1

    2 2 12

    sin sin2 2sin cos

    cos

    B Cr R A A

    A=

    Hence

    (6.8)( ) ( ) ( )1 1 1

    2 2 24 sin sin sinr R A B C =

    a

    bc

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    Excirclesxcircles

    A'D

    I

    D'

    E'

    F'

    IA

    B C

    A

    ( )ABI C

    Let AI be the centre of a circle, opposite

    angle A, of radius obtained by bisecting

    the angles Band C externally and Ainternally.

    ArAr

    Let AI be the centre of a circle, opposite

    angle A, of radius obtained by bisecting

    the angles Band C externally and Ainternally.

    We have that:We have that:

    Area of triangle

    Areas of triangles A A

    ABC

    I B CI A

    =

    +

    ( )

    Area of triangle

    Areas of triangles A A A

    ABC

    I B CI A BI C

    =

    +

    That isThat is

    ( )

    ( )

    1 1 1

    2 2 212

    12

    2

    A A

    A

    A

    cr br ar

    r c b a

    r a b c a

    = +

    = +

    = + +

    A

    Hence fors, the semi perimeterHence fors, the semi perimeter

    (6.9)( )Ar s a = (6.9)( )Ar s a =

    A

    B

    rs a

    rs b

    =

    =

    Similarly, we haveSimilarly, we have

    Crs c

    =

    (6.10)

    A

    B

    C

    rs a

    rs b

    rs c

    =

    =

    =

    (6.10)

    Notice further that are collinear as both lie on the bisector

    line of angle A

    Notice further that are collinear as both lie on the bisector

    line of angle A

    , and AA I I, and AA I I and AAI AIand AAI AI

    Now letNow let' '

    ' '

    ' '

    A

    A

    A

    AE AF x

    BD BF y

    CD CE z

    =

    = = =

    Tangents to a circle from

    a single point have equal

    lengths

    Tangents to a circle from

    a single point have equal

    lengths

    ' '

    ' '

    ' '

    A

    A

    A

    AE AF x

    BD BF y

    CD CE z

    =

    = = =

    ThenThen ' ' 'AF AE AB BF AC CE+ = + + +' ' 'AF AE AB BF AC CE+ = + + + '

    A

    ( )

    2 A A

    A A

    x c y b z

    b c y z

    = + + +

    = + + +

    ( )

    2 A A

    A A

    x c y b z

    b c y z

    = + + +

    = + + +

    but .but .' 'A Ay z BD D C BC a+ = + =' 'A Ay z BD D C BC a+ = + =

    a

    bc

    28

    a

    bc

    '

    A

    Figure 6.3

    A'D

    I

    D'

    E'

    F'

    IA

    B C

    A

    ( )

    ( )

    1 1 1

    2 2 212

    12

    2

    A A A

    A

    A

    cr br ar

    r c b a

    r a b c a

    = +

    = +

    = + +

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    Therefore:

    ( )12

    2 A

    A

    a b c

    a b c

    = + +

    = + +

    Hence

    ( )semi perimeter (6.11)Ax s=

    A'D

    D'

    E'

    F'

    IA

    B C

    A

    In a similar manner

    andB Cs x = x =

    a

    bc

    s

    The three distances , andA B Cx s x s x s= = =

    are displayed below

    Figure 6.4

    Figure 6.5

    IB

    B C

    A

    Figure 6.6

    IC

    B C

    A

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    Notice also from triangle and from (6.11) that'AAI F

    ( )12'

    tan'

    A AI F rAAF s

    = =

    ( )12tanAr s A= .

    Similarly

    ( )

    (

    ( )

    12

    12

    12

    tan

    tan

    tan

    A

    B

    C

    r s A

    r s B

    r s C

    =

    =

    =

    (6.12))

    a

    bc

    Therefore, we can further show that

    ( )( )

    ( )

    12

    12

    12

    ' ' cotcot ,

    cot .

    A

    B

    C

    AF s r As r B

    s r C

    = ==

    =

    (6.13),AE

    B

    a

    bc

    Moreover, since ' ' 'F BD AF AB s c= = =

    and ' ' 'CE CD AE AC s b= = =

    then

    ( ) (

    ' 'DD CD CD

    s b s c

    b c

    )

    =

    =

    =

    Where D is the point of tangency of the incirclewith side a, is the point of

    tangency of the excirclewith side a, and where the symbol is the positive

    difference between its two arguments. Namely:

    'D

    'DD b c b c= (6.14)

    Further, as 'BD CD s= = c it follows that is the midpoint of where

    is also the midpoint ofBC.

    'A 'DD 'A

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    Herons Area Formula

    IA

    D

    ID'

    AB

    C

    Figure 6.7

    As and ABI B

    90AIBI =

    I bisect the angle B both internally and externally, it follows that

    . Moreover, since and 'AIDB I D B

    'A

    are also right angles then this

    implies that triangles andBID BI D are similar.

    Namely:Triangles '

    A

    BID I BD

    Thus' 'A A

    BI ID BD

    I B BD I D= =

    that is:A A

    BI r s b

    I B s c r

    = =

    Therefore: ( )( )Ar r s b s c = (6.15)

    On using (6.2) and (6.10) this becomes

    ( )(s b s cs s a

    ) =

    Hence ( )( )( )s s a s b s c = (6.16)

    Which is the form of the area of triangle ABCas met previously in (MP.7) and

    (5.6)

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    7: Further Triangle Formulae

    Figure 7.1

    Y

    D

    I

    IA

    XA

    C

    B

    ( ) ( ) ( )1 12 2 2an , tan and tan in terms of , and .B C a b c

    From Figure 7.1 we have ( )12tanID r

    AAD s a

    =

    On using (6.15) this becomes

    ( )

    ( )( )

    ( )(

    ( )

    )12tan

    A

    A

    s b s c

    r s b s cA

    s a r s a

    = =

    On using (6.9) we have

    ( )( )( )

    ( )( )

    ( )( )12tan

    s b s c s b s cA

    s as a

    = =

    Hence: ( )( )( )

    ( )( )( )

    ( )(

    ( )

    )12tan

    s b s c s b s cA

    s s as s a s b s c

    = =

    Similarly,

    (7.1)

    ( )( )( )

    ( )

    ( )( )( )

    ( )

    ( )( )( )

    ( )

    12

    12

    12

    tan

    tan

    tan

    s b s cA

    s s a

    s c s aB

    s s b

    s a s bC

    s s c

    =

    =

    =

    a

    bc

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    ( ) ( ) ( )1 12 2 2os , cos and cos in terms of , and .B C a b c From Figure 7.1 we have ( )12 180AI CY C=

    ( )

    1

    212

    90 C

    A B

    =

    = +

    Also, using the construction properties of the Incircle and Excircle

    12A

    I AC A=

    Hence

    ( )( )

    ( )( )( )

    ( )

    12

    1 12 2

    12

    12

    180 180

    180 180

    180 180

    A A

    A

    AI C A I CY

    A A

    B

    AI C B DBI

    = +

    = + +

    =

    =

    B

    Therefore, triangles are similar, that isand AAIB ACI AAIB ACI .

    A A

    A A

    AI IB AB

    AC CI AI

    AI IB c

    b CI AI

    = =

    = =

    Hence AAI AI bc = (7.2)

    Also from Figure 7.1 ( )12cosA

    AXA

    AI= (7.3)

    and ( )12cosAD

    AAI

    = (7.4)

    The product of(7.3) and (7.4) gives

    ( ) ( )1 12 2cos cosA

    AX ADA A

    AI AI =

    That is

    ( )2 1

    2cos A

    AX AD

    A AI AI

    =

    On using (6.3), (6.11) and (7.2) this becomes

    ( )( )2 1

    2coss s a

    Abc

    =

    Hence

    (7.5)

    ( )( )

    ( )

    ( )

    ( )( )

    12

    1

    2

    12

    cos

    cos

    cos

    s s aA

    bc

    s s b

    B ca

    s s cC

    ab

    =

    =

    =

    a

    bc

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    ( ) ( ) ( )1 12 2 2in , sin and sin in terms of , and .B C a b c Using (1.1), (7.1) and (7.5) we have that

    ( ) ( ) ( )1 12 2sin tan cosA A=12

    A

    Hence

    ( )( )( )

    ( )

    ( )12sin

    s b s c s s aA

    s s a bc

    =

    Giving

    (7.6)

    ( )( )( )

    ( )( )( )

    ( ) ( )( )

    12

    12

    12

    sin

    sin

    sin

    s b s cA

    bc

    s c s aB

    ca

    s a s bC

    ab

    =

    =

    =

    a

    bc

    Notice that in each of the above three subsections the negative root is rejected if the

    angles,A, B and Care those of a triangle.

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    8: Further Triangle Relationships

    Relationship between r and RNote that

    ( )

    ( )

    1 12 2

    12

    12

    12

    180

    180

    180 180

    90

    BIC B C

    B C

    A

    A

    =

    = +

    =

    = +

    r

    D

    I

    A

    B C

    Figure 8.1

    and that ( )12sinID r

    BIB IB

    =

    Hence, ( )

    1

    2sinr IB B=

    (8.1)Using the Sine Rule of (4.6) we have that

    ( ) ( ) ( )11 122 2sin 90sin sinAC BIB BC I

    += =

    C,

    and from the first two of these fractions we have

    ( ) ( )1 12 2sin cosC A

    IB BC= .

    Therefore: ( )( )

    1

    212

    sincos

    BC CIBA=

    ,

    that is( )

    ( )

    12

    12

    sin

    cos

    a CIB

    A= . (8.2)

    Substituting (8.2) into (8.1) gives

    ( )

    ( )( )

    ( ) ( )( )

    12 1

    212

    1 1

    2 212

    sinsin

    cos

    sin sincos

    a Cr B

    A

    a C BA

    =

    =

    Using (4.7) acan be written as: a R2 sin ,A= giving( ) ( )

    ( )

    1 12 2

    12

    2 sin sin sin

    cos

    R A Br

    A=

    C.

    Using (2.11) gives

    ( ) ( ) ( ) ( )

    ( )

    1 1 1 12 2 2 2

    12

    2 2sin cos sin sin

    cos

    R A A Br

    A

    =

    C.

    Hence: 1 1 1r R (8.3)( ) ( ) ( )2 2 24 sin sin sinA B C=

    as met previously in (6.8).

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    Relationships between , , and .A B Cr r r R

    rA

    D'IA

    A B

    C

    From Figure 8.2 we see that

    ( )'

    n 'A A

    A

    A Asi

    I D r

    I BD I B I B=

    that is ( )12sin 90A Ar I B B=

    (8.4) ( 12cosA Ar I B B= )

    Figure 8.2

    Using the Sine Rule of (4.6) we have that

    ( ) ( ) ( )1 12 2sin 90 sin 90 sin 90

    A A

    C A

    I B BC I C

    = =

    12 B

    and from the first two of these fractions we have

    ( ) ( )1 12 2cos cos

    A

    C A

    I B BC=

    Therefore,( )

    ( )

    12

    12

    cos

    cosA

    BC CI B

    A= .

    that is,

    ( )

    ( )

    12

    12

    cos

    cosA

    a C

    I B A=

    (8.5)

    Substituting (8.5) into (8.4) gives

    ( )

    ( )( )

    ( ) ( )

    ( )

    12 1

    212

    1 12 2

    12

    coscos

    cos

    cos cos

    cos

    A

    a Cr B

    A

    a C B

    A

    =

    =

    Using (4.7) acan be written as: 2 sina R A= ,

    giving( ) ( )( )

    1 12 2

    12

    2 sin cos cos

    cosA

    R A Cr

    A=

    B.

    Using (2.11) gives

    ( ) ( ) ( ) ( )

    ( )

    1 1 1 12 2 2 2

    12

    2 2sin cos cos cos

    cosA

    R A A Cr

    A

    =

    B.

    Hence: ,a ( ) ( ) ( )1 1 12 2 24 sin cos cosAr R A B C =

    ( ) ( ) ( )1 1 12 2 24 cos sin cosBr R A B C =

    ( ) ( ) ( )1 1 12 2 24 cos cos sinC A B C=

    and similarly , (8.6)

    r R .

    bc

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    XD

    I

    IA

    A B

    C

    The distances A , and C .BI I

    From Figure 8.3 notice that

    ( )12nsiIDAIA

    =

    Figure 8.3Therefore,

    ( )

    (

    ( )

    12

    12

    12

    cosec

    cosec

    cosec

    AI r A

    BI r B

    CI r C

    =

    =

    =

    (8.7))

    a

    bc

    XD

    I

    IA

    A B

    If we just consider the triangle for the present and determine some of its

    angles from Figure 8.4

    we find that:

    AAI X

    Clearly ( )12180AI B A B= +

    and so on using the Sine Rule of (4.6)

    we have from triangle AIB

    ( ) ( ) ( )1 12 2sinsin sinAIBB AAI AB BI

    = =

    Figure 8.4

    Considering just the first two fractions here gives

    ( )

    ( )

    12sin

    sin

    AB BAI

    AIB=

    Therefore

    ( )( )( )

    12

    12

    sin

    sin 180

    c BAI

    A B=

    +

    That is on using (2.2):

    ( )( )( )

    ( )

    ( )( )

    ( )

    12

    12

    12

    12

    12

    12

    sin

    sin

    sin

    sin 90

    sin

    cos

    c BAI

    A B

    c B

    C

    c B

    C

    =

    +

    =

    =

    But on using (4.7) c can be written as: 2 sin ,c R C= giving

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    ( )

    ( )

    12

    12

    2 sin sin

    cos

    R C BAI

    C=

    Using (2.11) gives( ) ( ) ( )

    ( )

    1 1 12 2 2

    12

    2 2sin cos sin

    cos

    R C CAI

    C

    =

    B

    Hence

    (8.8)

    ( ) ( )

    ( ) ( )

    ( ) ( )

    1 12 2

    1 12 2

    1 12 2

    4 sin sin

    4 sin sin

    4 sin sin

    AI R B C

    BI R C A

    CI R A B

    =

    =

    =

    a

    bc

    which give an alternative form of(8.7). Further, from (8.7), as it is somewhat

    easier we may proceed ( )( )

    12 1

    2

    cosecsin

    rAI r A

    A= =

    Thus, from (7.6) we have

    ( )( ) ( )( )

    ( )

    ( ) ( )( )

    r r bAI

    s b s c s b s c

    bc

    r s s a bc

    s s a s b s c

    = =c

    ( ) ( ).

    r s s a bc s s a bcAI

    s

    = Using (5.6) and (6.1)

    ( ) ( )s a bc s abc

    s s

    = =

    ( ) ( )a s b c s bca

    s s

    = =

    ( ) ( )ab s c s cab

    s s

    = =

    AI

    BI

    a

    bc

    similarly (8.9)

    CI

    Note that the relations of(8.9) can be written

    ( ) ( )

    ( ) ( )

    ( ) ( )

    ,

    , where

    .

    s a s aa

    a

    b

    b

    c

    c

    bcAI K

    s a

    s b s ba c abcK K

    s b

    s c s cabCI K

    s c

    =

    =

    =

    BI (8.10)s

    =

    (8.11)( ) ( ) ( )

    : : : :s a s b s c

    AI BI CIa b c

    =

    Hence,

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    XD

    I

    IA

    A B

    C

    The distances A , and C .A B C

    BI I

    Figure 8.5From Figure 8.5 notice that

    ( )12sinA

    A

    I DA

    I A

    =

    Therefore,

    ( )

    ( )

    ( )

    12

    12

    12

    cosec

    cosec

    cosec

    A A

    B B

    C C

    AI r A

    BI r B

    CI r C

    =

    =

    =

    (8.12)

    a

    bc

    D

    I

    IA

    B

    C

    D

    I

    IA

    A B

    Notice also from Figure 8.6 that

    180

    90

    + + + =+ =

    Hence

    90AIBI =

    Also, since

    ( )1 12 2and 180 90 12B B B = = =

    then ( )1290AI I B A B= +

    Figure 8.6

    Figure 8.7

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    On using the Sine Rule of (4.6) we have from triangle AABI

    ( ) ( ) ( )1 12 2sin 90 sin sinA

    A A

    B AI B A

    AI AB BI

    += =

    Considering just the first two fractions here gives

    ( )( )

    12sin 90

    sinA

    A

    AB BAI

    AI B

    +=

    Therefore

    ( )

    ( )( )

    12

    12

    cos

    sin 90A

    c BAI

    A B=

    +

    That is on using (2.2):

    ( )( )( )

    ( )

    ( )( )

    ( )

    1

    212

    12

    12

    12

    12

    coscos

    cos

    cos 90

    cos

    sin

    A

    c BAI

    A B

    c B

    C

    c B

    C

    = +

    =

    =

    But on using (4.7) c can be written as: 2 sinc R C=

    giving

    ( )

    ( )

    12

    12

    2 sin cos

    sinA

    R C BAI

    C=

    Using (2.11) gives

    ( ) ( ) ( )

    ( )

    1 1 12 2 2

    12

    2 2sin cos cos

    sinA

    R C CAI

    C

    =

    B

    Hence ( ) ( )1 12 24 cos cosAAI R B C=

    ( ) ( )1 12 24 cos cosBBI R C A=

    ( ) ( )1 12 24 cos cosC R A B=

    and similarly (8.13)

    CI

    a

    bc

    which give an alternative form of(8.12)

    Further, from (8.12), as it is slightly easier we may proceed

    ( )( )

    12 1

    2

    cosecsin

    AA A

    rAI r A

    A= =

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    Thus, from (6.10) and (7.6) we have

    ( ) ( )( )

    ( )( )( )

    ( ) ( )( )

    ( )

    ( )

    ( )

    ( )

    1A

    AIs a s b s c

    bcs s a s b s c bc

    s a s b s c

    bc s s a

    s a

    bc s

    s a

    bc

    s a

    s

    =

    =

    =

    =

    =

    Therefore:

    or( )

    A

    bcAI

    s a

    s

    =

    ( )B caBI

    s b

    s

    =

    ( )C

    ab

    s c

    s

    =

    similarly (8.14)

    CI

    a

    bc

    In a manner similar to the processes used to arrive at (8.11) we can also show that

    (8.15)( ) ( ) ( )

    1 1 1: : : :A B CAI BI CI

    a s a b s b c s c=

    Further, if we take respective products of(8.9) and (8.14) then we quickly get the

    very nice results:

    (8.16)

    A

    B

    C

    AI AI bc

    BI BI ca

    CI CI ab

    =

    =

    =

    a

    bc

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    Y

    XD

    I

    IA

    A B

    d .B C

    II he distances , anA

    II II

    Figure 8.8

    Consider the similar triangles andAID AI I Y, we have

    A A

    AI AD ID

    II DX I= =

    Y

    That is

    ( )A A

    s aAI rII AX AD I X Y

    = = X

    ( )

    ( )A A

    s aAI r

    II s s a r I

    = =

    D

    Hence,( )

    A A

    s aAI r

    II a r

    = =

    r(8.17)

    From the first two fractions we have

    A

    aII A

    s a

    =

    B

    bII

    s b

    =

    C

    cII C

    s c

    =

    I

    similarly (8.18)BI

    I

    Therefore, on using the values from the first forms in (8.10), the results in (8.18)

    can be written in the manner

    ( )A

    s aa abcII

    s a s a

    =

    ( )A

    abc aII

    s s a=

    Hence

    (8.19)( ) ( ) ( )

    , ,A B Cabc a abc b abc c

    II II IIs s a s s b s s c

    = = =

    a

    bc

    .

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    Squaring the value of AII from (8.19) gives

    ( )( )

    2

    A

    abc aII

    s s a

    =

    Therefore, from the last two fractions of(8.17) this becomes

    ( )2 A

    A

    abc r r II

    s r

    =

    (8.20)

    From (5.2) we have4

    abc

    R =

    and from (6.1) that rs =

    Hence, (8.21)4abc

    Rrs

    =

    Therefore, from (8.20) and (8.21) we have that

    ( ) , , (8.22)( )2

    4A AI I R r r= ( ) ( )2

    4B BI I R r r= ( ) (2

    4C CII R r r= )

    Moreover, using the half-angle formula in (7.5) we see that (8.19) can be

    rearranged thus:

    ( ) ( ) ( ) ( )

    2

    12

    1

    cosA

    a bc bc aII a a

    s s a s s a As s a

    bc

    = = =

    Hence

    (8.23)( ) ( ) ( )1 12 2

    , ,cos cos cos

    A B C

    a bII II II

    A B C= = =

    12

    .c

    Therefore, on using the results of (4.7), (8.23) can be rewritten in a further,alternative form

    (8.24)( ) ( ) ( )1 12 24 sin , 4 sin , 4 sin .A B CI I R A II R B II R C= = =12

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    9: Further Triangle Centres

    The Orthocentre of any Triangle ABC

    H

    F

    E

    DB

    A

    C

    The perpendiculars drawn from the vertices of a triangle ABC to the oppositesides are concurrent at a point called the Orthocentre, H.From Figure 9.1 let AD, BE and CF be the perpendiculars

    on BC, CA and AB respectively, and H the Orthocentre;

    then

    ( )

    ( )

    tan

    cos tan 90 ,

    cos cot

    DH BD HBD

    AB B C

    c B C

    =

    =

    =

    Using (4.7) ccan be written as:Figure 9.1

    c R ,2 sin= C

    giving 2 sin cos cotDH R C B C=

    Hence2 cDH h=

    (9.1)2 c cEH h= bc

    F

    aos cos AR B C

    os os BR C A

    2 cos cos CH R A B h=

    Further,

    sin

    sin

    2 sin sin

    DA AB B

    c B

    R C B

    =

    =

    =

    That is2 sin sin

    2 sin sin

    2 sin sin

    DA R B C

    EB R C A

    FC R A B

    =

    =

    =

    (9.2)

    a

    bc

    Therefore, from (9.2) and (9.1) we have that

    2 sin sin 2 cos cos

    HA DA DH

    R B C R B C

    =

    =

    Using (2.3) this becomes

    ( )

    ( )

    2 cos

    2 cos 180

    HA R B C

    R A

    = +

    =

    Hence:

    2 cosHA R A=

    2 cosHB R B= (9.3)2 cosHC R C=

    a

    bc

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    Notice that

    ( )

    ( )

    ( )

    22

    2 2

    2 2

    2 2 2

    22

    2 cos

    4 cos

    4 1 sin

    4 4 sin

    4 2 sin

    HA R A

    R A

    R A

    R R A

    R R A

    =

    =

    =

    =

    =

    Using (4.7) acan be written as: 2 sina R A= ,

    giving 2 24HA R a2=

    Hence, we have the alternative forms of(9.3) as

    (9.4)

    2 2

    2 2

    2 2

    4

    4

    4

    HA R a

    HB R b

    HC R c

    =

    =

    =

    a

    bc

    Exercise: Establish(9.1)to(9.4)for an obtuse-angled triangle

    Again using Figure 9.1, note the following simply found forms of h h ., andA B Ch

    12

    12

    Area of triangle

    A

    ABC BC AD

    a h

    =

    =

    Therefore,2 2

    , and similarly , .A Bh ha b

    = =

    2Ch

    c

    =

    a

    bc

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    The Pedal Triangle of any Triangle ABCBy joining the feet of the perpendiculars from the vertices to the opposite sides, a

    new triangle is formed called the Pedal triangle.We use Figure 9.2 and call the triangle DEF the pedal triangle of triangle ABC.

    H

    F

    E

    DB

    A

    C

    Now, since then the quadrilateral90BFH BDH= =

    BFHD is cyclic. Considering the right-angledtriangle AEB we have that

    180 90

    90

    ABE FBH A

    A

    =

    =

    Next, consider the chord FHof

    the circle through BFHD.

    We have, using angles in the sameFigure 9.2

    segment, that:

    90FDH FBH A= =

    Similarly, since , then the quadrilateral BHEC is also cyclic90CEH CDH = = Therefore, from Figure 9.3 we see that from the right-angled triangle AFC that

    180 90

    90

    ACF ECH A

    A

    =

    =

    Next, consider the chord EHof the circle through CDHE. We have, using angles

    in same segment that:

    H

    F

    E

    D

    A

    C

    90ECH EDH A= =

    Thus we have shown that .bisectsHD EDF

    Similarly, and .bisectsHE FED bisectsHF DFE

    The orthocentre, H, of triangle ABC is theincentre of its associated pedaltriangle.

    Moreover,

    B(9.5)

    180 2 ;

    180 2 ;

    180 2 .

    EDF A

    FED B

    DFE C

    =

    =

    =

    Further, since BC, CA and AB are perpendicular to HD, HE and HF respectively,

    the sides of the fundamental triangle ABC are therefore the external bisectors of

    the angles of the pedal triangle.

    A, Band C are the excentres of the triangle DEF. (9.6)

    Figure 9.3

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    H

    F

    E

    DB

    A

    C

    Figure 9.4

    We also haveCDE BDF A

    AEF CED B

    BFD AFE C

    = =

    = =

    = =

    Hence, from using the Sine Rule (4.6) in the triangle AFE we have:

    ( ) ( )sin sinsin FEA EFAAEF FA EA

    = =

    The first two fractions lead tosin sin

    cossin sin

    cos

    A B

    EF AC A

    A B

    EF b A

    =

    =

    Hence

    sin cossin cos

    sin sin

    b A A bEF A A

    B B= =

    Therefore, from (4.7)

    2 sin cosEF R A A= (9.7)

    Therefore, using either (2.11) or (4.7), equation (9.7) can now be written in either

    of two forms

    ( )sin 2EF R A= or cosEF a A= a

    ( )sin 2FD R B= or cosEF b B= (9.8)

    ( )sin 2DE R C= or cosDE c C= bc

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    The Circumcircle and the Pedal Triangle.Let 'R be the radius of the circle circumscribing the pedal triangle DEF

    (Figure 9.2). Then, by the Sine Rule (4.7)

    ( )2 'sinEF R FDE= Therefore, by (9.8) and (9.5) we have

    ( ) ( )sin 2 2 'sin 180 2R A R A=

    that is ( ) ( )sin 2 2 'sin 2R A R A= , by (2.2)

    Hence; (9.9)12'R R=

    That is, the radius of the circumcircle of the fundamental triangle ABC is twice

    the radius of the circumcircle of the pedal triangle of the fundamental triangle

    ABC

    (Note: The Circumcircle of the pedal triangle of the fundamental triangle ABC i

    actually theNine Point Circle of the fundamental triangle ABC)s

    The Excentric Triangle.Returning briefly to the work of 8, which dealt with the Excircles of the

    fundamental triangle ABC having centres , andA B CI I I and associated radii

    , we make the following comparisons between these and those of thepedal triangle as discussed above.

    , andA B Cr r r

    I

    IB

    IA

    ICA

    B C

    X

    Figure 9.5

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    Recall from the construction of Incircle and Excircle that IC bisects andACB

    AI C bisects the angle BCX .

    Therefore,

    ( )

    ( )

    1 12 2

    12

    12 180 90

    A AICI ICB I CB

    ACB XCB

    ACB XCB

    = +

    = += +

    = =

    Similarly, BICI is also a right angle.

    Hence, is a straight line to which IC is perpendicular

    IA

    I

    B

    A

    C

    A BI CI

    B CI AI

    C AI BI

    is a straight line to which IA is perpendicular (9.10)is a straight line to which IB is perpendicular

    Also, since AIand both bisect theAAI BAC

    andB

    , the three points all lie

    on the same straight line. Similarly,

    , and AA I I

    CB I I C I I are also straight lines.

    Hence, A B CI I I is a triangle, which is such that A, Band C are the feet of the

    perpendiculars drawn from its vertices upon the opposite sides, and such that I is

    the intersection of these perpendiculars. That is, triangle ABC is the pedal

    triangle and I is the Orthocentre of the Excentric triangle A B CI I I .

    We also note from Figure 9.6 that

    ( )12 180AI BC B= and ( )12 180AI CB C=

    Therefore,

    ( ) ( )( )

    1 12 2

    12

    12

    180 90 90

    90

    ABI C B C

    B C

    A

    =

    = +

    =

    But as ABICI is a cyclic quadrilateral, then

    Figure 9.6 1290BIC A= +

    Similarly,

    1 12 2

    1 12 2

    90 , 90 ,

    90 , 90 .

    B CCI A B AI B C

    CIA B AIB C

    = =

    = + = +

    Thus, triangles , ,A B CI BC I CA I AB are similar,

    each with angles 1 12 290 , 90 , 90A B . (9.11)12 C

    IA

    X

    IO

    B C

    Figure 9.7

    From Figure 9.7, let X be the intersection of the

    angle bisector through and the, and AA I I

    circumcircle of triangle ABC.

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    Therefore, BX XC= as BAX CAX= . Moreover, 12BAX BCX A = ,

    (from chord BX).

    Therefore, ( )12XCI A C= +

    but (12

    )XIC A C= + when taken as the exterior angle to triangle AIC.

    Hence, XC XI=

    We also have 12AXCI B= as , and90AICI = ACX ABC B = , (from

    chord AC). Therefore,12A

    XI C B= , AXC X I=

    Thus 12A AXB XC X I X I II= = = = .

    Moreover, as AI BIC is a cyclic quadrilateral on AI I as diameter, the

    circumference of the triangle AI BC passes through I.Similarly, the circumcircles of the triangles BI CA and CI AB also pass through I.

    In the triangle ABI C, using the Sine Rule from (4.7), we have that

    ( )sin 1A

    A

    BI C

    BC I=

    IBIC, where 2 radius of AA II I

    Therefore, from (9.11)( )12sin 90

    A

    aII

    A=

    Hence

    ( ) ( ) ( )1 12 2, ,

    cos cos cosA B C

    a bII II

    A B C= = = (9.12)

    a

    bc12

    ,c

    II

    as met previously in (8.23)

    IA

    IB

    IC

    I

    B

    A

    C

    ( )1 12 290 90B B B + = +

    Consider now the Figure 9.8

    Using (9.11) we see that C BBI I C

    is a cyclic quadrilateral since

    ( ) ( )1 12 290 90

    180

    C B CI BC CI I

    B B

    +

    = + +

    =

    1290 B

    Moreover, as C AIB I I then C AI I

    is a diameter of theC BBI I C

    Therefore, in the triangle CBI C,

    using the Sine Rule from (4.7),

    we have that:( )sin 1C

    B C

    BI C

    BC I=

    I.

    Figure 9.8

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    But 1290CBI C A= from (9.11), and from (9.10)90AI CI =

    12C

    BI C A = .

    Therefore, we have

    ( )12sin 1

    B C

    A

    a I=

    I

    Hence

    (9.12)

    ( )

    ( )

    ( )

    12

    12

    12

    ,sin

    ,sin

    .sin

    A B

    B C

    C A

    cI I

    C

    aI I

    A

    bI I

    B

    =

    =

    =

    a

    bc

    On using (4.7) these relations can easily be shown to take the alternative forms:

    (9.13)( ) ( ) ( )1 12 24 cos , 4 cos , 4 cos .A B B C C AI I R C I I R A I I R B= = =12

    From the Excentric triangle A B CI I I we have the simple area calculation:

    ( )( ) ( )

    ( )( ) ( )( ) ( )

    12

    1 1 12 2 2

    sin

    4 cos 4 cos sin 90

    A B C C A A B C A BArea I I I I I I I I I I

    12

    R A R C A

    =

    =

    Hence

    (9.14)( ) ( ) ( )2 1 1 12 2 28 cos cos cosA B CArea I I I R A B C=

    Notice that on using (7.5) we can rewrite (9.14) as

    ( ) ( ) ( )

    ( )( )( )

    2

    32

    2 2 2

    2

    8

    8

    8

    42

    12

    4

    12

    A B C

    s s a s s b s s cArea I I I R

    bc ca ab

    s s a s b s cR

    a b c

    R s

    abc

    RR s

    abc

    R sabc

    R

    R s

    =

    =

    =

    =

    =

    =

    Hence

    (9.15)2A B CArea I I I Rs=

    , from (5.2)

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    10: Special Cevian Lengths

    A Cevian is the name given to any line from a triangle vertex to its opposite sideans of any Triangle.The Centroid and Medi

    Figure 10.1 the points D, E and F are midpoints of

    gle ABC, usual

    C

    From page 3 of the Appendix we have

    G

    D

    EF

    B

    A

    C

    In

    the respective sides opposite the apexes A, B and C.

    The lines , andAD BE CF are called the Mediansof the trian ly denoted

    , , .AD m BE m CF m= = = A B

    Figure 10.1

    proved the following results:

    2 2AG = 3 3, , .AD BG BE CG CF= = 23

    The point G is called the Centroid of the triangle ABC.rom the Cosine Rule of (4.5) we have, from triangle ADC, in Figure 9.10

    os .

    That is

    F

    that

    ( ) ( ) ( ) ( )( )2 2 2

    2 cAD AC CD AC CD C= +

    ( )

    2

    2 2

    2 co2 2A

    a a

    m b b C

    = +

    s .

    Hence2

    2 2 cos4

    A

    am b ab C = + . (10.1)

    However, a second application of the Cosine Rule in the whole triangle ABC gives

    C. (10.2)

    Hence, on equating (10.1) and (10.2) we find that

    2 2 2 2 cosc b a ba= +

    2 2 222

    A

    am c b =

    2

    22 2 22

    2A

    am b c= +

    22 2 2

    2B

    bm c a= +

    22 2 2

    2C

    cm a b= +

    2

    2

    a

    bc

    Thus we have

    (10.3)

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    On using the Cosine Rule once again the relations of(10.3) can be written:

    os

    os (10.4)

    os

    otice the elation derived from adding each of the results of

    2 2 24 2Am b c bc= + + a

    c A

    c B

    c C

    2 2 24 2Bm c a ca= + +

    2 2 2

    4 2Cm a b ab= + +

    simply determined r

    bc

    N

    (10.3):

    ( )2 2 2 2 2 234A A Am m m a b c+ + = + + (10.5)

    Figure 10.2 let

    In ACADC = ; draw AL BC , then

    ( )

    ( )

    ( )

    12

    12

    cot

    cos

    sin2 sin cos sin

    2 sin sin

    2sin cos sin

    2sin sin

    sin

    2sin sin

    cot cot

    AC

    DL BL BD

    AL AL

    c B a

    c B

    R C B R A

    R C B

    C B B C

    B C

    C B

    B C

    B C

    = =

    =

    =

    +=

    =

    =

    hat isT

    ( )2cot cot cot sin cosec cosecAC B C C B B C =

    Also, as 180AB AC = then

    ( )

    ( )

    cot cot 1801

    tan 180

    1 tan180 tan

    tan180 tan

    1 0

    0 tan

    cot

    AB AC

    AC

    AC

    AC

    AC

    AC

    =

    =

    +=

    +=

    =

    Hence( )

    ( )

    2cot cot cot sin cosec cosec

    2cot cot cot sin cosec cosec

    AC

    AB

    B C C B B

    C B B C C B

    =

    =

    C(10.6)

    cb

    mAK

    L

    G

    DB C

    Figure 10.2

    A

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    To find the angles which makes withAm , drawAB CA DK AB and let

    BDAB = and CDAC =

    cot BAK

    =

    ; then

    ( )

    2

    cotsin

    12 cot

    sinsin 1

    2 cosin sin

    sin2 cot

    sin sin

    sin2 cotsin sin2cot 2cot cot

    a

    AB KB c KB

    KD KD KD KD

    c B

    B

    cB

    a B

    CB

    A B

    CB

    A B

    A BBA B

    B A B

    = =

    =

    =

    =

    =

    +

    =

    = +

    t

    Hencecot 2cot cot

    cot 2cot cot

    B A B

    A C

    = +

    = +(10.7)

    imilarly symmetric relations eS ian lines andBE CF.

    C

    xist for the other med

    ng the results of(10.7) we have:Notice further, that on subtracti

    cot cot cot cotB C = B C (10.8)

    Hence, from (10.8), the identities of(10.6) can be written:

    2cot cot cotAC B C

    2cot cot cotAB C B

    =

    = (10.9)

    evians Bisecting Angles InternallyC

    c b

    XB C

    internally and divides the

    ase BC into portions

    AAIn Figure 10.3 the cevian AX bisects

    b AB and AC

    By the Sine Rule in triangle we haveAXB

    ( ) ( )12 ssin sin AXBA B= =

    ( )in

    AB Ax c

    (10.10)

    riangle we haveand in t AXC

    ( 12sin

    Figure 10.3

    ) ( ) ( )sinsin

    AC A

    AXCA C

    x = =

    b(10.11)

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    No AXB( ) ( ) ( )sin sin 180 sinAXC AXB = ting that

    then we have on division of (10.11) and (10.10) that

    ACx b=

    ABx c(10.12)

    Therefore, on using Theorem (3.2) we have

    ( ) ( )1 1AB ACAB AC AB ACx xx x x

    b c b

    + += = =

    + +

    Hence

    x a

    c( ) ( )11c b b c+

    ,AB ACac ab

    x xc b c

    = =+ +b

    (10.13)

    Also, if

    bc

    a

    is the length of the cevian andAX AC AXC =

    Therefore, ( ) (1 1 1 1sin sinc A + =

    , then we have

    Area AXB Area AXC Area ABC + =

    ) 12 2 2 2 2 sinb A bc A

    Giving( )12

    sin

    sinA

    bc A

    b c A

    =

    +

    Hence

    ( )122

    cosAbc

    Ab c

    = +

    (10.14)

    hich on using (7.5) becomesw

    ( )2

    As s a bc = (10.15)

    b c+

    2

    2

    AC

    AB

    AXAB B B

    AXAC C C

    = + +

    = + +

    otice also thatN

    (10.16)

    Clearly, the relationships of(10.12) to (10.16) can be re-written relative

    to the other triangle apexes B and C by the usual symmetry rule

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    Cevians Bisecting Angles ExternallyIn Figure 10.4 the cevian bisects externally and divides theAX A

    base BC extended, into portions ABx and ACx

    c b

    X 'XB

    A

    C

    Figure 10.4By the Sine Rule in triangle ABX we have

    ( ) ( ) ( )12sin 90 sinsin AAB

    A A B

    x AX c

    + = =

    That is:

    ( ) ( ) ( )12sin 90 sinsin AAB

    A B

    x AX c

    + = =

    (10.17)

    By the Sine Rule in triangle ACX we have

    ( ) ( ) ( )12sin 90 sin 180 sin AAC

    A C

    x AX b

    = =

    That is:

    ( ) ( ) ( )12sin 90 sinsin AAC

    A A B

    x AX b

    += =

    (10.18)

    Thus (10.17) gives

    ( ) ( ) ( )

    1

    2cos sinsin AAC

    A A B

    x AX b

    += = (10.19)

    and (10.18) gives

    ( ) ( ) ( )12cos sinsin A

    AB

    A B

    x AX c

    = =

    (10.20)

    (10.19) (10.20) gives

    1 1

    11

    AC

    AB

    x b

    cx

    =

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    Hence (10.21)AB

    AC

    c

    x b

    =

    which is a similar relation to (10.12)

    Therefore, on using Theorem (3.2) once again we have

    ( )

    ( )

    1

    1AB ACAB AC AB AC

    x xx x x

    c b b c b c b

    + = = =

    +

    ( )

    ( )

    1

    1 c

    x a

    Hence

    ,AB ACa c ab

    x xc b c b

    = =

    (10.22)

    Also, if A is the length of the cevian AX and A AX C = , then we have

    Area ABX Area ACX Area ABC =

    Therefore,

    ( ) ( )

    ( ) ( )( )( ) ( )( )

    1 1 1 12 2 2 2

    1 12 2

    1 12 2

    sin 90 sin 90 sin

    sin 90 sin 90 sin

    cos cos sin

    A A

    A

    A

    c A A b A bc

    c A b A bc

    c A b A bc

    + + =

    + + =

    + =

    12

    A

    A

    A

    Giving( )12

    sin

    cosA

    bc A

    c b A

    =

    Hence

    ( 122

    sinAbc

    Ac b

    = (10.23)

    )

    which on using (7.6) becomes

    ( )(2

    A (10.24))bc s b s cc b

    =

    Notice also that

    (10.25)

    90

    2180 90

    2

    A

    A

    AC

    AB

    = +

    = + +

    a

    bc

    Clearly, the relationships of(10.21) to (10.25) can be re-written relative

    to the other triangle apexes B and C by the usual symmetry rule

    One further observation is that

    AC AC

    ab abX X x x

    b c c b = + = +

    +

    Hence (10.26)2 2

    2abcX X

    c b =

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    DB C

    AApollonius TheoremIn Figure 10.5 the point D bisects the base BC

    of the triangle ABC.

    Apollonius Theorem states that:

    ( ) ( ) ( ) ( )2 2 2 2

    Proof: Let

    2 2AB AC AD BD+ = +

    ADB = ; therefore 180ADC = .

    es

    os

    Therefore, using the Cosine Rule giv

    Figure 10.5

    ( ) ( ) (AB AD D= + ) ( )( )2 2 2

    2 cB AD DB (10.27)

    ) ( ) ( ) ( ) ( )( ) (2 2 2 2 cos 180AC AD DC AD DC= +

    That is )os( ) ( ) ( ) ( )( ) (2 2 2

    2 cAC AD DC AD DC = + (10.28)

    re, by the addition of(10.27) and (10.28), and sinceTherefo DC= we have:BD

    ( ) ( ) ( ) ( )2 2AB AC AD BD+ = + 2 2 2 2

    Generalisation of Apollonius Theorem Ste oremarts The

    ivided in the ratio

    In Figure 10.6 the base BC of the triangle ABC has been

    d

    :BD DC :m n= (10.29)

    by the foot D of the general cevian AD

    0.27) by and (10.28)

    y to give

    F

    b

    urther, we have on multiplication of (1 n

    ( ) ( ) ( ) ( )( )2 2 2

    2 cosn AB n AD n DB n D DB = +

    B C

    A

    D

    Figure 10.6

    m

    and

    A

    ) (10.31)

    (10.30)

    os( ) ( ) ( ) ( ) ( ) (2 2 2

    2 cm AC m AD m DC m AD DC = + +

    From (10.29),(10.31) can be written

    )os( ) ( )m AC m AD m= + ( ) ( )( ) (2 2 2

    2 cDC n AD BD + (10.32)

    ence, adding (10.30) and (10.32) gives us the general form

    2(10.33)

    hich redu

    H

    ( ) ( ) ( )( ) ( )2 2 2 2

    n AB m AC m n AD n BD m+ = + + + ( )DC

    w midpoint of ces to Apollonius form for m n= , that is forD being the

    BC.

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    Figure 10.8

    by fi

    the Figure 10.5 in the following manner.

    Stewarts Theorem can then be shown in a form

    more easily recalled, namely:

    (10.34)

    In the same manner we can extend the results of(10.16) for a general cevian

    rather than the angle bisector of that section.

    Consider Figure 10.8 in which we set

    Figure 10.7

    c

    ba d

    m n

    This is perhaps most easily remembered rst re-labelling

    ( )2 2 2a n b m c d mn+ = +

    : :BD DC m= n

    c b

    nmB

    A

    CD

    That ism BD BD AD

    n DC AD DC

    = =

    Therefore, on using the Sine Rule we have

    ( )

    ( )( )( )

    ( )

    sin 180 180sin

    sinsin 180

    AB CB

    CB AB

    m BD AD

    n AD DC

    = =

    ,

    ( )

    ( )

    ( )

    ( )

    ( )

    ( )( ) ( ) ( ) ( )

    ( ) ( ) ( ) ( )

    ( ) ( ) ( ) ( ){ } ( )( ) ( ) ( ) ( ){ } ( )

    ( ) ( ) ( )

    ( ) ( ) ( )

    sin sin

    sin sin

    sin sin cos cos sin

    sin sin cos cos sin

    sin cos cos sin / sin

    sin cos cos sin / sin

    sin cot cos

    cos cot sin

    B AB C

    C B AB

    B AB C AB

    C B AB B

    AB C AB C C

    B AB B AB

    AB C AB

    AB B AB

    m

    n

    C

    AB

    B

    =

    +

    =

    +

    =

    +

    =

    +

    That is

    Hence,

    ( ) ( ) ( ) ( ) ( ) ( )

    ( ) ( ) ( ) ( ) ( ) ( )

    cos cot sin sin cot cos

    cos sin cot cot sin ,

    AB B AB AB C AB

    AB AB C B AB

    m m n n

    m n n m

    + =

    + =

    giving: ( ) ( ) ( ) ( )cot cot cotAB C Bm n n m + = (10.35)

    Similarly, using the identity ( ) ( )cot 180 cot gives

    ( ) ( ) ( ) ( )cot cot cotAC B Cm n m n + = (10.36)

    Notice that (10.35) and (10.36) reduce to (10.9) for m n= , that is forD being the

    midpoint ofB.

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    11: Problems

    Problem 1. Prove:4r r r r R+ + =A B C

    Problem 2. Prove:1 1 1

    A B Cr r r

    1

    r+ + =

    Problem 3. Prove:1 1 1

    B Ch h+ + =

    1

    r

    Ah

    ove:Problem 4. Pr2

    A B Cr r r rs= 2 A B Cr r r r =

    Problem 5. Prove:

    ( ) ( ) ( )

    ( ) ( ) ( )

    1 1 12 2 2

    1 1 12 2 2

    4 cos cos cos

    4 cos cos cos

    s R A B C

    Rr A B

    =

    =

    C

    6. Prove:

    C

    rove:

    Problem

    cos cos cos 4 sin sin sina A b B c C R A B+ + =

    Problem 7. P2

    A B B C C Ar r r r r r s+ + =

    Problem 8. Prove:

    ( )21 1 1 1

    4A B C A B C

    abcs

    r r r r r r R r + + =

    + + +

    Problem 9. Prove:

    ( ) ( )2 1 12 24 cos cotB Cr r R A a A+ =

    10. Prove:Problem

    )r r+ ( )( ) ( ) (4A B B C C A A B B C C Ar r r r r r R r r r r + + + = +

    Problem 11. Prove:

    ( ) ( )( ) 24A B Cr r r r r r R r =

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    Problem 12. Prove:3

    2 2 2 2 2

    1 1 1 1 1 1 1 1 1 1 1 1 64 4

    C C A A B C

    R R

    r r r r r r r r r a b c r s

    + + + = =

    A B Br r r

    roblem 13. Prove:P

    ( ) )( ) ( )( ( ) ( ) 2

    1 1 1

    s a s b s b s c s c s a r

    1+ + =

    Problem 14. Prove:

    ( )22 2 2 2 2 24 1b c b c a 6= + +

    Problem 15. Prove:

    ( ) ( )2 24 sin 2 sin 2b A a = + B

    Problem 16. Prove:

    )

    ( ) ( ( )2 1 1 12 2 2tan tan tans A B = C

    Problem 17. Prove:22 sin sin sinR A B = C

    Problem 18. Prove:

    ( )sin sin sinRr A B C = + +

    Problem 19. Prove:

    ( )

    2 2 sin sin

    2 sin

    a b A B

    A B

    =

    Problem 20. Prove:

    ( ) ( ) ( )( )3 2 2 232 sin 2 sin 2 sin 2a b c A B C = + +

    Problem 21. Prove:

    ( )

    2 2 2

    4cot cot cot

    a b cA B C

    + + =+ +

    Problem 22. Prove:

    rr( ) ( )( )A B C A B C AB C

    B CA B B C C A

    r r r r r r a r

    s rr r r r r r

    + += = = +

    + +r

    r

    Problem 23. Prove:

    ( ) ( )2 A Ba r r r r = + C

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    Problem 24. Prove:

    ( )( ) ( )

    12sin

    A

    A B A C

    rA

    r r r r =

    + +

    Problem 25. Prove:

    ( )( )

    2sin A A B B C C A

    A B A C

    r r r r r r r A

    r r r r

    + +=

    + +

    Problem 26. Prove:

    (

    ( ) ( ) )3 2 2 21 1 12 2 2cot cot cotA B Cr r r r A B C =

    Problem 27. Prove:2 2

    2 2 2 2 2

    1 1 1 1

    A B C

    a b c

    r r r r

    2+ ++ + + =

    Problem 28. Prove:2

    Problem 29. Prove:

    2 2 2 2 2 2 216A B Cr r r r R a b c+ + + =

    A B Cab r r rr = +

    Problem 30. Prove:

    1 1 1 12ab bc ca Rr

    + + =

    Problem 31. Prove:1 1

    2CA B

    rr r

    bc ca ab r R+ + =

    Problem 32. Prove:

    0A B C

    b c c a a b

    r r r

    + + =

    Problem 33. Prove:

    ( ) ( ) ( )A B C B C A C A Ba rr r r b rr r r c rr r r + = + = +

    Problem 34. Prove:

    A B B C C A A B Cr r r r r r rr rr rr ab bc ca+ + + + + = + +

    Problem 35. Prove:

    (

    ( ) ( ) ( )

    2 2 28 2

    A B C

    I I I I I I R R+ + = )r

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    66

    Problem 36. Prove:216A B CI I I I I I R r =

    Problem 37. Prove:

    ( ) ( )2

    4B C B CI I R r= + r

    Problem 38. Prove:

    ( ) ( ) ( ) ( ) ( ) ( )2 2 2 2 2

    A B C B C A C A

    2

    BI I I I I I I I I I I I+ = + = +

    Problem 39. Prove:

    sin sin sinA B C B C A C A BI I I I I I I I I I I I

    A B

    = =

    C

    Problem 40.

    radii of three circles which touch one another externally

    gents at their points of contact meet in a point; prove that the

    his point from eitherof their points of contact is

    , anda b c are the

    and the tan

    distance of t

    abc

    a b c+ +

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    Appendix: Concurrences of Straight Lines in a Triangle

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    69

    ircumcentre:The perpendiculars drawn to the sides of a triangle from their

    midpoints are concurrent

    Let X, Y and Z be the midpoints of the side

    triangle ABC.

    From Zand Ydraw perpendiculars to

    meeting at O. Join OX.

    Thus, it is required to show that OX isperpendicular to BCJoin OA, OB, OC.

    Proof:

    C

    s of the

    AB, AC

    Z

    O

    X

    Y

    B

    A

    C

    Because YO bisects AC at right angles, it is therefore the locus of points that are

    equidistant from A and C.

    Therefore, OA OC=

    Again, because ZO bisects AB at right angles, it is therefore the locus of points

    that are equidistant from A and B.

    Therefore, OA OB=

    Hence: OB OC=

    Therefore, O is on the locus line of points equidistant from B and C; that is

    Hence, the perpendiculars from the midpoints of the sides of the triangle ABCmeet at O.

    is perpendicular toOX BC

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    Incentre:

    isect ,

    The bisectors of the angles of a triangle are concurrent

    O. JoinABC BCA

    B by straight lines that meet at

    red to show that AO bisects

    .

    AO.

    BAC .e R

    P

    Q

    O

    B

    A

    C

    Thus, it is requi

    From O draw OP, OQ, OR perpendicular to th

    sides of the triangle ABC

    Proof:

    Because BO bisects it is

    t to the locus

    of points that are equidistant

    A and BC.

    BAC

    therefore equivalen

    from B

    Therefore, OP OR=

    Similarly, CO is the locus of points that are equidistant from CB and CA.

    herefore OP OQ= T

    Hence OR OQ=

    Therefor

    is, OA i

    e, O is on the locus of points that are equidistant from AB and AC; that

    s the bisector of the

    ence the bisectors of the three angles of the triangle ABC meet at O.

    BAC.

    H

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    Centroid:The medians of a triangle are concurrent

    Let BY Z o of the medians of the triangle ABC, and leand C be twt O. Join AO and produce it to meet

    hus, it is required to show that AX

    hrough C draw CK, parallel to BY

    CK at K. Join BK.

    t them intersectBC in X.

    is the remaining median

    . Produce AX

    O

    K

    Y

    X

    Z

    B

    A

    C

    a

    Tof triangle ABC.T

    to meet

    Proof:

    Because Y is the middle point ofAC,

    to CK, therefore O

    the middle point ofAK.

    triangles )

    e have

    parallel to BK, that is, OC is parallel to BK.

    herefore, the figure BKCO is a parallelogram. But the diagonals of aogram bisect one another; therefore X s the middle point ofBC.

    ence, the medians of triangle ABC meet at O.

    orollary:

    and YO is parallel

    is

    AYO ACK (By similar

    In the triangle ABK, since Z and O are the middle points ofAB and AK w

    that ZO is

    Tparallel i

    That is, AX is also a median of the triangle ABC.

    H

    (O is usually referred to as the Centroid of the triangle)C

    The three medians of a triangle cut one another at a point of trisection, the greatersegment in each being towards the angular point.

    We have seen above that AO OK= ,

    and that OX is half ofOK;

    therefore OX is half ofOA:

    that is OX is one third ofAX.

    Similarly, OY is one third ofBY,

    and OZ is one third ofCZ.

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    72

    Orthocentre:The perpen ngle to the

    opposite sides are concurrent

    m A and B to their opposite

    des; and let them intersect at O. Join CO;and produce it to meet AB at F.

    d to show that CF is

    diculars drawn from the vertices of a tria

    Let AD and BE be the perpendiculars drawn fro

    si

    Thus, it is require perpendicular to AB.F

    D

    E

    O

    B

    A

    C

    Proof:

    Join DE.

    ecause and are both

    ght-angles, we have:

    cyclic

    um to )

    , vertically opposite angles.

    ave:

    , in same segment.

    Therefore, we ha

    (angles in triangle sum to )

    CF is perpendicular to

    Hence the three perpendiculars AD, BEand CF meet at the point O.

    OEC ODCThen, b

    ri

    Points O,E,C,D are concyclic.

    (Opposite angles in a

    180quadrilateral s

    Therefore, DEC DOC= , in same segment,E

    O

    D C

    DEC FOA=

    Similarly, as AEB and ADB are both right-angles, we

    h

    Points A,E,D,B are concyclic.

    (Opposite angles in a cyclicquadrilateral sum to180 )

    Therefore,

    DEB DAB=

    veO

    D

    E

    F

    B

    A

    C DE=

    90

    FOA FAO DEC DAB

    C DEB

    + +

    +

    =

    Therefore, 90AFO = 180

    That is, AB.

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    Bibliography

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    In order of usage:

    Sixth Form Trigonometry. W. A. C. Smith. James Nisbet & Co. Ltd. [1956].

    Modern Geometry. C. V. Durell. Macmillan & Co. Ltd. [1957].

    Plane Trigonometry (Part 1). S. L. Loney. Macmillan & Co. Ltd. [1967].

    A School Geometry (Parts I VI) . Hall & Stevens. Macmillan & Co. Ltd. [1944].

    Advanced Euclidean Geometry: An Elementary Treatise on the Geometry of the

    Triangle and the Circle. Roger A. Johnson. Dover Publications Inc. [1929].

    College Geometry: An Introduction to the Modern Geometry of the Triangle and

    the Circle. N. Altshiller Court. Barnes & Noble Inc. [1952].

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