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Mathematics · Ch 10 — Vector Algebra

Section Formula

10.5.3

Section Formula

10.5.3 Section Formula

The Core Problem

Two points PP and QQ have position vectors OP⃗=p⃗\vec{OP} = \vec{p} and OQ⃗=q⃗\vec{OQ} = \vec{q}. A point RR on the line joining PP and QQ has position vector OR⃗=r⃗\vec{OR} = \vec{r}. We find r⃗\vec{r} when RR divides the segment PQPQ in a given ratio — either internally (RR between PP and QQ) or externally (RR on the extension beyond PP or beyond QQ).

Important

The ratio m:nm : n is always taken with mm and nn as positive scalars. For internal division, mm corresponds to segment PRPR and nn to segment RQRQ.


Case I: Internal Division

When RR lies between PP and QQ, it divides PQPQ internally in the ratio m:nm : n:

PRRQ=mn\frac{PR}{RQ} = \frac{m}{n}

Derivation of the Position Vector

PR⃗=OR⃗−OP⃗=r⃗−p⃗,RQ⃗=OQ⃗−OR⃗=q⃗−r⃗\vec{PR} = \vec{OR} - \vec{OP} = \vec{r} - \vec{p}, \qquad \vec{RQ} = \vec{OQ} - \vec{OR} = \vec{q} - \vec{r}

Since PR⃗\vec{PR} and RQ⃗\vec{RQ} are collinear and point in the same direction with magnitudes in the ratio m:nm : n:

n⋅PR⃗=m⋅RQ⃗n \cdot \vec{PR} = m \cdot \vec{RQ}

n(r⃗−p⃗)=m(q⃗−r⃗)n(\vec{r} - \vec{p}) = m(\vec{q} - \vec{r})

nr⃗−np⃗=mq⃗−mr⃗n\vec{r} - n\vec{p} = m\vec{q} - m\vec{r}

(m+n)r⃗=mq⃗+np⃗(m + n)\vec{r} = m\vec{q} + n\vec{p}

r⃗=mq⃗+np⃗m+n\vec{r} = \frac{m\vec{q} + n\vec{p}}{m + n}

This is the section formula for internal division.

Note

The coefficient of p⃗\vec{p} is nn (the ratio for segment RQRQ) and the coefficient of q⃗\vec{q} is mm (the ratio for PRPR). Mnemonic: the ratio "opposite" to a point goes with that point.


Case II: External Division

When RR lies on the extension of PQPQ (beyond QQ or beyond PP), it divides PQPQ externally in the ratio m:nm : n:

PRQR=mn\frac{PR}{QR} = \frac{m}{n}

Note the denominator is QRQR, not RQRQ, and RR is outside the segment PQPQ.

Derivation of the Position Vector

Here PR⃗\vec{PR} and QR⃗\vec{QR} point in the same direction, giving:

n(r⃗−p⃗)=m(r⃗−q⃗)n(\vec{r} - \vec{p}) = m(\vec{r} - \vec{q})

nr⃗−np⃗=mr⃗−mq⃗n\vec{r} - n\vec{p} = m\vec{r} - m\vec{q}

(n−m)r⃗=np⃗−mq⃗(n - m)\vec{r} = n\vec{p} - m\vec{q}

r⃗=np⃗−mq⃗n−m\vec{r} = \frac{n\vec{p} - m\vec{q}}{n - m}

This is the section formula for external division.

Tip

To remember it: take the internal formula and change the plus in the denominator to a minus, and the plus in the numerator to a minus. (Equivalently, r⃗=mq⃗−np⃗m−n\vec{r} = \frac{m\vec{q} - n\vec{p}}{m - n}.)


Special Case: The Midpoint

When RR is the midpoint of PQPQ, the ratio m:nm : n becomes 1:11 : 1. Substituting m=nm = n into the internal formula:

r⃗=1⋅q⃗+1⋅p⃗1+1=p⃗+q⃗2\vec{r} = \frac{1 \cdot \vec{q} + 1 \cdot \vec{p}}{1 + 1} = \frac{\vec{p} + \vec{q}}{2} …

Figure 10.16Internal division of segment PQ by point R, with position vectors a=OP, b=OQ and r=OR drawn from origin O and the sub-segments QR=n and RP=m, illustrating the section formula for internal division.
Fig. 10.16 — Internal division of segment PQ by point R, with position vectors a=OP, b=OQ and r=OR drawn from origin O and the sub-segments QR=n and RP=m, illustrating the section formula for internal division.

Drawn by us to help you understand the concept clearly, and verified to make sure it's accurate. For exams, practice from your textbook's own diagram.

What Fig 10.16 Shows

The diagram is a clean vector sketch with three labelled points — O, P, Q, and R — and the origin O placed somewhere off to the side. From O, three position vectors radiate: a⃗\vec{a} to point P, b⃗\vec{b} to point Q, and r⃗\vec{r} to point R. The points P and Q are joined by a thin slate-coloured line segment, and R lies on that segment between P and Q. Along the segment, two distances are marked: the length QR is labelled nn, and the length RP is labelled mm. So R divides the segment PQ internally in the ratio m:nm : n, meaning that the distance from R to P is mm parts and from R to Q is nn parts.

The figure has no axes — it is a freehand vector diagram, not a coordinate plot. Its purpose is purely geometric: to show how the position vector of a point dividing a line segment can be expressed in terms of the endpoints' position vectors.

The Physical Idea

When you have two points P and Q in space, any point R on the line joining them can be described by how far it is from P relative to the whole segment. If R lies between P and Q, we say it divides the segment internally. The ratio m:nm:n tells you that if you travel from P to Q, you cover mm units to reach R, then nn more units to reach Q — or equivalently, PRRQ=mn\frac{PR}{RQ} = \frac{m}{n}.

The key insight is that the position vector r⃗\vec{r} of R is a weighted average of a⃗\vec{a} and b⃗\vec{b}, with the weights being the opposite segment lengths. This is not obvious at first glance, which is why the textbook derives it using triangle law of vector addition.

The Derivation (in brief)

From the diagram, using triangle OQR:

r⃗=b⃗+QR⃗\vec{r} = \vec{b} + \vec{QR}

But QR⃗\vec{QR} is along the direction from Q to P, and its magnitude is nn times the unit vector along QP. Similarly, from triangle OPR:

r⃗=a⃗+PR⃗\vec{r} = \vec{a} + \vec{PR}

Since PR⃗\vec{PR} and QR⃗\vec{QR} are in opposite directions along the same line, and the total vector from P to Q is b⃗−a⃗\vec{b} - \vec{a}, we can write:

PR⃗=mm+n(b⃗−a⃗)andQR⃗=nm+n(a⃗−b⃗)\vec{PR} = \frac{m}{m+n}(\vec{b} - \vec{a}) \quad \text{and} \quad \vec{QR} = \frac{n}{m+n}(\vec{a} - \vec{b})

Substituting either into the triangle law gives the same result.

r⃗=mb⃗+na⃗m+n\vec{r} = \frac{m\vec{b} + n\vec{a}}{m+n}

This is the internal division formula. Every symbol:

  • r⃗\vec{r} — position vector of the dividing point R
  • a⃗\vec{a} — position vector of P (first endpoint)
  • b⃗\vec{b} — position vector of Q (second endpoint)
  • mm — the part of the segment from R to P (the "near" part to P)
  • nn — the part from R to Q (the "near" part to Q)
Watch out

A common mistake is to swap the weights. Notice that the coefficient of a⃗\vec{a} is nn, not mm, and the coefficient of b⃗\vec{b} is mm. The weight attached to an endpoint's position vector is the opposite segment length — the part of the segment that is farther from that endpoint.

Special Case: Midpoint

When m=nm = n, R is the midpoint of PQ. The formula simplifies to:

r⃗=a⃗+b⃗2\vec{r} = \frac{\vec{a} + \vec{b}}{2}

This is the simplest and most frequently used special case — the midpoint's position vector is just the average of the two endpoints' position vectors. …

Figure 10.17External division of segment PQ by point R lying beyond Q, with position vectors a=OP, b=OQ and r=OR from origin O and the dashed segment RQ=n and RP=m, illustrating the section formula for external division.
Fig. 10.17 — External division of segment PQ by point R lying beyond Q, with position vectors a=OP, b=OQ and r=OR from origin O and the dashed segment RQ=n and RP=m, illustrating the section formula for external division.

Drawn by us to help you understand the concept clearly, and verified to make sure it's accurate. For exams, practice from your textbook's own diagram.

What Fig. 10.17 Shows

The figure illustrates the external division of a line segment PQPQ by a third point RR. Three position vectors emanate from the origin OO: OP⃗=a\vec{OP} = \mathbf{a} (to point PP), OQ⃗=b\vec{OQ} = \mathbf{b} (to point QQ), and OR⃗=r\vec{OR} = \mathbf{r} (to point RR). The three points PP, QQ, and RR lie on a straight line, but with a crucial ordering: RR lies beyond QQ, so the collinear arrangement is RR–QQ–PP (read from left to right along the line). The segment RQRQ is drawn as a dashed indigo line, and the segment QPQP is solid. Along QPQP, two lengths are marked: mm and nn, where mm corresponds to the length PRPR and nn corresponds to QRQR.

The physical idea is simple: when a point divides a segment externally, it does not lie between the two endpoints. Instead, it lies on the extension of the segment beyond one of them. Here, RR is beyond QQ, so QQ lies between RR and PP. The ratio of division is given as PR:QR=m:nPR : QR = m : n, which is the ratio of the whole segment from PP to RR to the segment from QQ to RR.

Watch out

A common mistake is to confuse the ratio m:nm:n with the distances PRPR and QRQR directly. In external division, the ratio is taken as PR:QR=m:nPR : QR = m : n, not PQ:QRPQ : QR or PR:PQPR : PQ. The point RR is outside the segment PQPQ, so the distances involved are from PP to RR and from QQ to RR, not from PP to QQ.

The Key Formula

The textbook leaves the derivation as an exercise, but the result is central. For two points PP and QQ with position vectors a\mathbf{a} and b\mathbf{b} respectively, the position vector r\mathbf{r} of the point RR that divides PQPQ externally in the ratio m:nm:n (meaning PR:QR=m:nPR : QR = m : n) is:

r=mb−nam−n\mathbf{r} = \frac{m\mathbf{b} - n\mathbf{a}}{m - n}

Here:

  • a\mathbf{a} = position vector of PP (from origin OO)
  • b\mathbf{b} = position vector of QQ
  • mm and nn are positive scalars representing the ratio PR:QR=m:nPR : QR = m : n
  • r\mathbf{r} = position vector of RR

Notice the minus sign in the numerator and denominator — this is the hallmark of external division. Compare with the internal division formula r=mb+nam+n\mathbf{r} = \frac{m\mathbf{b} + n\mathbf{a}}{m + n}, where both terms are added. The external formula can be remembered as "the vector of the point beyond which RR lies (b\mathbf{b}, since RR is beyond QQ) gets the positive coefficient mm, and the other vector (a\mathbf{a}) gets subtracted."

Tip

A quick way to derive the external formula: treat external division as internal division with a negative ratio. If RR divides PQPQ externally in the ratio m:nm:n, you can think of it as dividing PQPQ internally in the ratio m:(−n)m:(-n). Substituting n→−nn \to -n in the internal formula r=mb+nam+n\mathbf{r} = \frac{m\mathbf{b} + n\mathbf{a}}{m + n} gives r=mb−nam−n\mathbf{r} = \frac{m\mathbf{b} - n\mathbf{a}}{m - n}.

What the Figure Teaches Visually …