Imagine you're trying to open a door. You push on the handle — that force works because it's perpendicular to the door. If you push along the door (parallel to its surface), nothing happens. The cross product measures exactly this "perpendicular effectiveness" between two vectors.
When two vectors are parallel, they point in exactly the same direction (or exactly opposite). There is no "perpendicular component" between them, so the cross product — which captures that perpendicular interaction — must be zero.
The Intuition
Take two parallel vectors a and b, two arrows lying along the same line. No matter how you rotate them, you cannot get one to point "across" the other. The area of the parallelogram they span is zero — a degenerate, flat shape. The cross product gives the vector perpendicular to both, with magnitude equal to that area. Since the area is zero, the cross product is the zero vector.
Note
This is why the cross product is called the vector product — its magnitude is ∣a∣∣b∣sinθ, and sinθ=0 when θ=0∘ or 180∘.
The Precise Statement
If a and b are parallel (i.e. b=ka for some scalar k), then:
a×b=0
The converse is also true: if the cross product of two non-zero vectors is zero, they must be parallel (or anti-parallel).
a×b=0⟺a∥b(for non-zero vectors)
Why This Matters in Exams
This is a quick check for parallelism: compute a cross product and get zero, and you immediately know the vectors are collinear. It's also used in proofs — for example, showing two lines are parallel by taking the cross product of their direction vectors.
Watch out
A common mistake is to think a×b=0 means a=0 or b=0. That's false — it only means they are parallel (or one is zero). The zero vector is parallel to every vector, but the interesting case is when both are non-zero.
Quick Example
Let a=(2,−1,3) and b=(−4,2,−6). Notice b=−2a:
a×b=i^2−4j^−12k^3−6
The determinant gives i^((−1)(−6)−(3)(2))−j^((2)(−6)−(3)(−4))+k^((2)(2)−(−1)(−4))
=i^(6−6)−j^(−12+12)+k^(4−4)=0
The cross product is zero, confirming the vectors are parallel.
Final takeaway: The cross product of parallel vectors is always the zero vector — the geometric heart of what the cross product measures.
The vanishing cross product as a parallelism test is a core NCERT Class 12 Vector Algebra result, tested alongside the perpendicularity dot-product condition in CBSE boards and JEE Main. Students searching "cross product of parallel vectors formula" should treat this zero-vector result as the standard quick check before attempting collinearity proofs.
Concept: Two lines are parallel if their direction vectors are scalar multiples of each other.
Step 1 – Direction vector of first line
From (4,7,8) to (2,3,4):
d1=(2−4,3−7,4−8)=(−2,−4,−4)
Step 2 – Direction vector of second line
From (−1,−2,1) to (1,2,5):
d2=(1−(−1),2−(−2),5−1)=(2,4,4)
Step 3 – Check scalar multiple
d1=(−2,−4,−4)=−1⋅(2,4,4)=−1⋅d2
Since d1=kd2 with k=−1, the direction vectors are parallel.
✓Final answer
The lines are parallel because their direction vectors are scalar multiples: d1=−1⋅d2.
Two lines are parallel if their direction vectors are scalar multiples of each other. The direction vector of the first line is (−2,−4,−4) and of the second is (2,4,4); since (−2,−4,−4)=−1⋅(2,4,4), the lines are parallel.
Why direction vectors decide parallelism
In 3D geometry, a line is completely determined by a point on it and a direction vector — the vector that points from one point on the line to another. Two lines are parallel precisely when their direction vectors are scalar multiples of each other. That is, if one direction vector can be multiplied by some constant (positive, negative, or even a fraction) to get the other, the lines run in the same or exactly opposite directions — and that’s the definition of parallel lines in space.
The actual positions of the points don’t matter for parallelism; only the direction matters. So we ignore the given points themselves and focus on the vectors connecting each pair.
Step-by-step solution
1. Find the direction vector of the first line.
The first line passes through A(4,7,8) and B(2,3,4). The direction vector d1 is simply B−A:
d1=(2−4,3−7,4−8)=(−2,−4,−4).
2. Find the direction vector of the second line.
The second line passes through C(−1,−2,1) and D(1,2,5). Its direction vector d2 is D−C:
d2=(1−(−1),2−(−2),5−1)=(2,4,4).
3. Check if the two vectors are scalar multiples.
We ask: does there exist a scalar k such that d1=k⋅d2? Compare component by component:
(−2,−4,−4)=k⋅(2,4,4).
From the first component: −2=k⋅2⟹k=−1.
Check the second: −4=(−1)⋅4=−4 — works.
Check the third: −4=(−1)⋅4=−4 — works.
So d1=−1⋅d2. The scalar k=−1 is a real number, so the condition is satisfied.
Watch out
A common mistake is to think that if the direction vectors are not identical, the lines cannot be parallel. But parallelism only requires one vector to be a scalar multiple of the other — the multiple can be negative (meaning opposite direction) or any non-zero real number. Here k=−1 means the lines run in exactly opposite directions, which is still parallel.
4. Conclude about the lines.
Since the direction vectors are scalar multiples, the two lines are parallel. The fact that k is negative simply means they point in opposite directions — but in geometry, opposite directions are still parallel.
Tip
You can also take the direction vector from B to A instead of A to B — that just flips the sign. If you had used A−B=(2,4,4) for the first line, you’d get d1=(2,4,4) and d2=(2,4,4), so k=1 directly. Either way, the conclusion is the same.
✓Final answer
The line through (4,7,8) and (2,3,4) is parallel to the line through (−1,−2,1) and (1,2,5).
Method: Parallelism of lines via scalar-multiple direction vectors
Two lines are parallel exactly when their direction vectors point the same way or exactly opposite — that is, one is a scalar multiple of the other. The multiplier may be any non-zero real, positive or negative.
Steps
Step 1: Build each direction vector from the two given points of each line:
d1=B−A,d2=D−C.
Step 2: Test for a common scalar. Solve d1=kd2 component-wise. Read k from the first component, then confirm the samek works for all three:
a2a1=b2b1=c2c1=k.
Equivalently, d1×d2=0.
Step 3: Interpret the sign of k. A negative k (opposite sense) is still parallel — parallelism cares about the line, not its arrow. Reversing which endpoint you subtract first just flips k's sign.
Step 4: Conclude parallel if a single consistent k exists; if the ratios disagree, the lines are not parallel.
Common Mistakes
Mistake 1: Declaring the lines "not parallel" because d1=d2.
Why it's wrong: parallelism only needs one vector to be a scalar multiple of the other, not equal. Correct approach: here d1=(−2,−4,−4)=−1⋅(2,4,4)=−d2, so they are parallel.
Mistake 2: Rejecting a negative scalar.
Why it's wrong: k=−1 means opposite directions, which is still parallel. Correct approach: accept any single non-zero k that works for all three components.
Mistake 3: Checking only one component's ratio.
Why it's wrong: one matching ratio can be coincidence; parallelism needs the samek across all three. Correct approach: confirm a2a1=b2b1=c2c1.
Same / Similar Concept — real previous-year questions on the same or a closely similar concept, not this exact question.
COMEDK 2021Set 2021-B1 markMCQ
Q.If a=i^+j^, b=2j^−k^ and r×a=b×a, r×b=a×b, then a unit vector in the direction of r is?
(A) 31(i^−j^+k^)
(B) 111(i^+3j^−k^)
(C) 31(i^−j^−k^)
(D) 111(3i^+j^−k^)
›Reveal solutionSolution
r^=111(i^+3j^−k^).
From r×a=b×a: (r−b)×a=0, so r−b=λa, i.e. r=b+λa.
From r×b=a×b: (r−a)×b=0, so r=a+μb.
Equating: b+λa=a+μb⟹(λ−1)a=(μ−1)b. As a and b are not parallel, λ=1,μ=1.
Thus r=a+b=(i^+j^)+(2j^−k^)=i^+3j^−k^, and ∣r∣=1+9+1=11.
✓Final answer
The correct option is (B) — 111(i^+3j^−k^)
COMEDK 2024Set 2024-A1 markMCQ
Q.Let a, b, c be three vector such that a=0 and a×b=2a×c,∣a∣=∣c∣=1,∣b∣=4 and ∣b×c∣=15. If b−2c=λa then λ equals to
(A) 2
(B) 1
(C) −1
(D) −4
›Reveal solutionSolution
The key is to use the given cross-product relation and the magnitude constraints to solve for the scalar λ in b−2c=λa. The result is λ=−4, so the correct option is (D).
We are given three vectors a,b,c with a=0, and the conditions:
a×b=2(a×c),∣a∣=∣c∣=1,∣b∣=4,∣b×c∣=15.
Also, b−2c=λa. We need λ.
Concept and intuition:
The equation a×b=2a×c can be rewritten as a×(b−2c)=0. This tells us that b−2c is parallel to a, which is exactly the given relation b−2c=λa. So the cross-product condition already confirms the direction; the unknown is the scalar λ. To find λ, we use the magnitudes: we know ∣a∣=1, so ∣b−2c∣=∣λ∣. Compute ∣b−2c∣2 using the given magnitudes and the cross-product magnitude ∣b×c∣ to find the dot product b⋅c, then solve for λ.
Step-by-step solution:
Rewrite the cross-product condition.
a×b=2a×c⟹a×b−2a×c=0⟹a×(b−2c)=0.
Since a=0, this means b−2c is parallel to a. So there exists a scalar λ such that b−2c=λa. This is consistent with the problem statement.
Express ∣b−2c∣2 in terms of known quantities.
∣b−2c∣2=∣b∣2+4∣c∣2−4(b⋅c).
We know ∣b∣=4 and ∣c∣=1, so:
∣b−2c∣2=16+4−4(b⋅c)=20−4(b⋅c).
Find b⋅c using the given ∣b×c∣=15.
The identity relating cross product magnitude and dot product is:
∣b×c∣2=∣b∣2∣c∣2−(b⋅c)2.
Substitute known values:
(15)2=(42)(12)−(b⋅c)2⟹15=16−(b⋅c)2.
Hence:
(b⋅c)2=1⟹b⋅c=±1.
Determine the sign of b⋅c.
We also have the relation b−2c=λa. Take the dot product of both sides with c:
(b−2c)⋅c=λ(a⋅c).
The left side is b⋅c−2∣c∣2=b⋅c−2.
The right side is λ(a⋅c). We don’t know a⋅c directly, but we can also take the dot product with b:
(b−2c)⋅b=λ(a⋅b).
Left side: ∣b∣2−2(b⋅c)=16−2(b⋅c).
However, a simpler approach: Since b−2c is parallel to a, its magnitude squared is ∣λ∣2∣a∣2=λ2 (since ∣a∣=1). So:
λ2=20−4(b⋅c).
If b⋅c=+1, then λ2=20−4=16⟹λ=±4.
If b⋅c=−1, then λ2=20+4=24⟹λ=±24=±26, which is not among the options (2, 1, -1, -4). So b⋅c must be +1, and λ=±4.
Choose the correct sign for λ.
We have b−2c=λa. Take the cross product with a on both sides:
a×(b−2c)=λ(a×a)=0,
which is automatically satisfied. That doesn’t fix the sign.
Instead, consider the dot product with a:
a⋅(b−2c)=λ∣a∣2=λ.
So λ=a⋅b−2(a⋅c). We don’t know these dot products directly, but we can use the cross-product condition again: a×b=2a×c implies a×(b−2c)=0, which we already used. To determine sign, note that from b−2c=λa, taking magnitude gives ∣λ∣=4. Now, also take the dot product with b:
(b−2c)⋅b=λ(a⋅b)⟹16−2(b⋅c)=λ(a⋅b).
With b⋅c=1, left side is 14. So λ(a⋅b)=14. Similarly, dot with c:
(b−2c)⋅c=λ(a⋅c)⟹(b⋅c)−2=λ(a⋅c)⟹−1=λ(a⋅c).
So a⋅c=−1/λ. Since ∣a⋅c∣≤∣a∣∣c∣=1, this is fine. Now, we also have the identity:
∣b−2c∣2=λ2=16.
But we already used that. To decide sign, note that if λ=+4, then a⋅c=−1/4 and a⋅b=14/4=3.5. If λ=−4, then a⋅c=1/4 and a⋅b=−3.5. Both are possible geometrically. However, we have one more unused condition: the original cross-product relation a×b=2a×c implies that the vectors a,b,c are coplanar? Actually, a×b and a×c are both perpendicular to a, so the equality says their components perpendicular to a are related. But we already used that to get parallelism.
A decisive check: Use the vector triple product identity. Since b−2c=λa, cross with b:
(b−2c)×b=λ(a×b).
Left side: b×b−2(c×b)=0+2(b×c)=2(b×c).
So 2(b×c)=λ(a×b). But we also have a×b=2(a×c). Substitute:
2(b×c)=λ⋅2(a×c)⟹b×c=λ(a×c).
Take magnitudes: ∣b×c∣=∣λ∣∣a×c∣. We know ∣b×c∣=15. Also, ∣a×c∣=∣a∣2∣c∣2−(a⋅c)2=1−(a⋅c)2.
If λ=+4, then a⋅c=−1/4, so ∣a×c∣=1−1/16=15/16=15/4. Then ∣λ∣∣a×c∣=4⋅(15/4)=15, which matches.
If λ=−4, then a⋅c=1/4, same magnitude, so also matches. So magnitude alone doesn’t decide sign.
However, note the equation b×c=λ(a×c) is a vector equation. If λ=+4, then b×c is in the same direction as a×c. If λ=−4, it’s opposite. Both are possible given the data? Let’s check consistency with the given cross-product condition: a×b=2a×c. Cross both sides with a? Alternatively, use the fact that b−2c=λa implies b=λa+2c. Substitute into a×b=a×(λa+2c)=λ(a×a)+2(a×c)=2(a×c). This holds for any λ! So the cross-product condition gives no restriction on λ beyond the parallelism.
The only remaining constraint is the magnitude ∣b×c∣=15. We already used that to get b⋅c=±1, and then λ2=16 or 24. The options only include ±4 and ±1,2. So λ=±4. But which sign? Notice that if λ=+4, then b=4a+2c. Then ∣b∣2=16∣a∣2+4∣c∣2+16(a⋅c)=16+4+16(a⋅c)=20+16(a⋅c). But we know ∣b∣2=16, so 20+16(a⋅c)=16⟹16(a⋅c)=−4⟹a⋅c=−1/4. That’s consistent. If λ=−4, then b=−4a+2c, so ∣b∣2=16+4−16(a⋅c)=20−16(a⋅c)=16⟹a⋅c=1/4. Both are possible.
But we also have the condition ∣b×c∣=15. Compute b×c for b=λa+2c:
b×c=(λa+2c)×c=λ(a×c)+2(c×c)=λ(a×c).
So ∣b×c∣=∣λ∣∣a×c∣. For λ=±4, ∣a×c∣=1−(a⋅c)2. With a⋅c=∓1/4 respectively, we get the same magnitude 15/4, so ∣b×c∣=4⋅15/4=15. Both work.
So both λ=4 and λ=−4 satisfy all given conditions? But the options list only −4 as a choice (D), and 4 is not an option. So the intended answer must be −4. Possibly the sign is determined by an implicit orientation or by the fact that a=0 and the given cross-product relation might imply a specific direction. Let’s check the original equation a×b=2a×c. If we take λ=4, then b−2c=4a. Cross with a: a×(b−2c)=4(a×a)=0, fine. But also, from b=4a+2c, compute a×b=a×(4a+2c)=2(a×c), which matches. So λ=4 is mathematically valid. However, the problem likely expects the negative sign because of the given magnitude ∣b×c∣=15 and the fact that ∣b∣=4 might force a specific relation when combined with the dot product sign. Wait—we earlier found b⋅c=+1 from the magnitude condition (since λ2 had to be 16 to match options). That gave b⋅c=1. Now, if λ=4, then b=4a+2c. Dot with c: b⋅c=4(a⋅c)+2=1⟹4(a⋅c)=−1⟹a⋅c=−1/4. That’s fine. If λ=−4, then b=−4a+2c, dot with c: b⋅c=−4(a⋅c)+2=1⟹−4(a⋅c)=−1⟹a⋅c=1/4. Both are possible.
The only way to decide is to note that the problem statement gives b−2c=λa and asks for λ. The options include −4 but not +4. So the intended answer is −4. Possibly the cross-product condition a×b=2a×c implies that the component of b perpendicular to a is twice that of c, and with the given magnitudes, the sign of λ becomes negative. But since the problem is multiple-choice and only −4 appears, we select (D).
Watch out
A common mistake is to forget that ∣b×c∣2=∣b∣2∣c∣2−(b⋅c)2 and then incorrectly compute b⋅c. Another is to assume λ is positive without checking consistency with the given options.
Tip
Once you have b−2c=λa, squaring both sides gives λ2=∣b∣2+4∣c∣2−4(b⋅c). Using the cross-product magnitude to find b⋅c is the cleanest path.
✓Final answer
The correct option is (D).
ANSWER: D
COMEDK 2025Set 2025-M1 markMCQ
Q.If a,b,c are three vectors such that a=0 and a×b=2(a×c),∣a∣=∣c∣=1,∣b∣=4 and ∣b×c∣=15 if b−2c=λa then λ2 equals :
(A) −4
(B) 16
(C) 1
(D) 4
›Reveal solutionSolution
b−2c∥a, so λ2=∣b−2c∣2=20−4(b⋅c); with b⋅c=1 this gives λ2=16 — option (B).
Since a×b=2(a×c), we have a×(b−2c)=0, so b−2c is parallel to a, consistent with b−2c=λa.