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Class 12Calculus18:18Published 25 Dec 2025

Eight Sure 3-Mark Questions for Class 12

Eight high-yield three-mark questions worked end to end for Class 12 board prep, spanning vectors, conditional probability, definite integrals, and 3D coordinate geometry.

This lesson walks through eight carefully chosen three-mark questions that often appear in the Class 12 exam. It covers finding the magnitude of a cross product and the angle between vectors, the range of lambda that makes an angle obtuse, a short proof that a conditional probability lies between 0 and 1, two definite integrals solved by a symmetry property and by substitution, finding the missing coordinate of three collinear points, and the magnitude of a vector written as a cross product. Each answer is shown with full working so you can reproduce the method in the exam.

What you'll learn

  • How to find the magnitude of a cross product and the angle between two vectors from their dot product
  • How to find the values that make the angle between two vectors obtuse, and how to prove a conditional probability stays between zero and one
  • How to evaluate definite integrals using a symmetry property and using substitution
  • How to find a missing coordinate so three points are collinear, and the magnitude of a vector given as a cross product

Lesson chapters

0:00Magnitude of a cross product from the dot product
2:29Angle between two vectors
3:49Values of lambda for an obtuse angle
6:41Proving a conditional probability lies between 0 and 1
8:47Definite integral of sine squared by symmetry
10:41Definite integral by substitution
12:02Finding lambda for three collinear points
14:58Magnitude of a vector given as a cross product

Lesson notes

This lesson works through eight sure three-mark questions for the Class 12 board exam, covering vectors, conditional probability, definite integrals, and 3D coordinate geometry. Each question is solved fully so you can follow the exact method.

Magnitude of a cross product

Given ∣a⃗∣=10|\vec a| = 10, ∣b⃗∣=2|\vec b| = 2, and a⃗⋅b⃗=12\vec a \cdot \vec b = 12, find ∣a⃗×b⃗∣|\vec a \times \vec b|.

The dot product gives the cosine, so start there:

cos⁡θ=a⃗⋅b⃗∣a⃗∣ ∣b⃗∣=1210×2=35.\cos\theta = \frac{\vec a \cdot \vec b}{|\vec a|\,|\vec b|} = \frac{12}{10 \times 2} = \frac{3}{5}.

Then

sin⁡θ=1−cos⁡2θ=1−925=1625=45.\sin\theta = \sqrt{1 - \cos^2\theta} = \sqrt{1 - \tfrac{9}{25}} = \sqrt{\tfrac{16}{25}} = \frac{4}{5}.

Now use ∣a⃗×b⃗∣=∣a⃗∣ ∣b⃗∣ sin⁡θ|\vec a \times \vec b| = |\vec a|\,|\vec b|\,\sin\theta:

∣a⃗×b⃗∣=10×2×45=16.|\vec a \times \vec b| = 10 \times 2 \times \frac{4}{5} = 16.

Angle between two vectors

Given ∣a⃗×b⃗∣=1|\vec a \times \vec b| = 1, ∣a⃗∣=2|\vec a| = 2, and ∣b⃗∣=1|\vec b| = 1, find the angle between a⃗\vec a and b⃗\vec b.

Here the cross product magnitude is given, so use the sine relation:

sin⁡θ=∣a⃗×b⃗∣∣a⃗∣ ∣b⃗∣=12×1=12.\sin\theta = \frac{|\vec a \times \vec b|}{|\vec a|\,|\vec b|} = \frac{1}{2 \times 1} = \frac{1}{2}.

So

θ=π6=30∘.\theta = \frac{\pi}{6} = 30^\circ.

The choice of which relation to use depends on whether the dot product or the cross product is given.

Values of lambda for an obtuse angle

Find the values of λ\lambda for which the angle between a⃗=2λ2 i^+4λ j^+k^\vec a = 2\lambda^2\,\hat i + 4\lambda\,\hat j + \hat k and b⃗=7 i^−2 j^+λ k^\vec b = 7\,\hat i - 2\,\hat j + \lambda\,\hat k is obtuse.

An obtuse angle (greater than 90∘90^\circ) means cos⁡θ<0\cos\theta < 0. Since

cos⁡θ=a⃗⋅b⃗∣a⃗∣ ∣b⃗∣,\cos\theta = \frac{\vec a \cdot \vec b}{|\vec a|\,|\vec b|},

and the magnitudes are positive, the condition reduces to a⃗⋅b⃗<0\vec a \cdot \vec b < 0.

Dot product. Multiply matching components and add:

a⃗⋅b⃗=(2λ2)(7)+(4λ)(−2)+(1)(λ)=14λ2−8λ+λ=14λ2−7λ.\vec a \cdot \vec b = (2\lambda^2)(7) + (4\lambda)(-2) + (1)(\lambda) = 14\lambda^2 - 8\lambda + \lambda = 14\lambda^2 - 7\lambda.

Solve the inequality. Require 14λ2−7λ<014\lambda^2 - 7\lambda < 0, that is

7λ (2λ−1)<0.7\lambda\,(2\lambda - 1) < 0.

This product is negative when λ>0\lambda > 0 and 2λ−1<02\lambda - 1 < 0, so

0<λ<12,λ∈(0,12).0 < \lambda < \frac{1}{2}, \qquad \lambda \in \left(0, \tfrac{1}{2}\right).

Proving a conditional probability lies between 0 and 1

Let AA and BB be events of the same sample space with P(B)≠0P(B) \neq 0. Prove that 0≤P(A∣B)≤10 \le P(A \mid B) \le 1.

By definition,

P(A∣B)=P(A∩B)P(B).P(A \mid B) = \frac{P(A \cap B)}{P(B)}.

Upper bound. Since A∩B⊆BA \cap B \subseteq B, we have P(A∩B)≤P(B)P(A \cap B) \le P(B). Dividing by P(B)>0P(B) > 0,

P(A∩B)P(B)≤1.\frac{P(A \cap B)}{P(B)} \le 1.

Lower bound. Probabilities are non-negative, so P(A∩B)≥0P(A \cap B) \ge 0, and with P(B)>0P(B) > 0,

P(A∩B)P(B)≥0.\frac{P(A \cap B)}{P(B)} \ge 0.

Combining the two,

0≤P(A∩B)P(B)≤1⟹0≤P(A∣B)≤1.0 \le \frac{P(A \cap B)}{P(B)} \le 1 \quad\Longrightarrow\quad 0 \le P(A \mid B) \le 1.

Definite integral of sine squared by symmetry

Evaluate ∫0π/2sin⁡2x dx\displaystyle\int_0^{\pi/2} \sin^2 x \, dx.

Let

I=∫0π/2sin⁡2x dx.(1)I = \int_0^{\pi/2} \sin^2 x \, dx. \qquad (1)

Use the property ∫0af(x) dx=∫0af(a−x) dx\displaystyle\int_0^a f(x)\,dx = \int_0^a f(a - x)\,dx with a=π2a = \tfrac{\pi}{2}. Since sin⁡(π2−x)=cos⁡x\sin\left(\tfrac{\pi}{2} - x\right) = \cos x,

I=∫0π/2cos⁡2x dx.(2)I = \int_0^{\pi/2} \cos^2 x \, dx. \qquad (2)

Add (1) and (2):

2I=∫0π/2(sin⁡2x+cos⁡2x)dx=∫0π/21 dx=[x]0π/2=π2.2I = \int_0^{\pi/2} \left(\sin^2 x + \cos^2 x\right) dx = \int_0^{\pi/2} 1 \, dx = \Big[x\Big]_0^{\pi/2} = \frac{\pi}{2}.

Therefore

I=π4.I = \frac{\pi}{4}.

Definite integral by substitution

Evaluate ∫0π/2sin⁡x1+cos⁡2x dx\displaystyle\int_0^{\pi/2} \frac{\sin x}{1 + \cos^2 x} \, dx.

Put t=cos⁡xt = \cos x, so −sin⁡x dx=dt-\sin x \, dx = dt, that is sin⁡x dx=− dt\sin x \, dx = -\,dt. Change the limits: when x=0x = 0, t=cos⁡0=1t = \cos 0 = 1; when x=π2x = \tfrac{\pi}{2}, t=cos⁡π2=0t = \cos\tfrac{\pi}{2} = 0.

I=∫10− dt1+t2=−∫10dt1+t2=−[tan⁡−1t]10.I = \int_1^0 \frac{-\,dt}{1 + t^2} = -\int_1^0 \frac{dt}{1 + t^2} = -\Big[\tan^{-1} t\Big]_1^0.

Evaluating,

I=−(tan⁡−10−tan⁡−11)=−(0−π4)=π4.I = -\left(\tan^{-1} 0 - \tan^{-1} 1\right) = -\left(0 - \frac{\pi}{4}\right) = \frac{\pi}{4}.

Finding lambda for three collinear points

If A(−1,3,2)A(-1, 3, 2), B(−4,2,−2)B(-4, 2, -2), and C(5,5,λ)C(5, 5, \lambda) are collinear, find λ\lambda.

First write the Cartesian equation of line ABAB through (x1,y1,z1)(x_1, y_1, z_1) and (x2,y2,z2)(x_2, y_2, z_2):

x−x1x2−x1=y−y1y2−y1=z−z1z2−z1.\frac{x - x_1}{x_2 - x_1} = \frac{y - y_1}{y_2 - y_1} = \frac{z - z_1}{z_2 - z_1}.

Substituting AA and BB,

x+1−4+1=y−32−3=z−2−2−2=x+1−3=y−3−1=z−2−4.\frac{x + 1}{-4 + 1} = \frac{y - 3}{2 - 3} = \frac{z - 2}{-2 - 2} = \frac{x + 1}{-3} = \frac{y - 3}{-1} = \frac{z - 2}{-4}.

Clearing the common negative signs,

x+13=y−31=z−24.(1)\frac{x + 1}{3} = \frac{y - 3}{1} = \frac{z - 2}{4}. \qquad (1)

Since CC is collinear, it lies on this line. Put x=5x = 5, y=5y = 5, z=λz = \lambda:

5+13=5−31=λ−24⟹2=2=λ−24.\frac{5 + 1}{3} = \frac{5 - 3}{1} = \frac{\lambda - 2}{4} \quad\Longrightarrow\quad 2 = 2 = \frac{\lambda - 2}{4}.

From λ−24=2\dfrac{\lambda - 2}{4} = 2,

λ−2=8⟹λ=10.\lambda - 2 = 8 \quad\Longrightarrow\quad \lambda = 10.

Magnitude of a vector given as a cross product

Find the magnitude of A⃗=(i^+3j^−2k^)×(−i^+3k^)\vec A = (\hat i + 3\hat j - 2\hat k) \times (-\hat i + 3\hat k).

Compute the cross product as a determinant:

A⃗=∣i^j^k^13−2−103∣.\vec A = \begin{vmatrix} \hat i & \hat j & \hat k \\ 1 & 3 & -2 \\ -1 & 0 & 3 \end{vmatrix}.

Expanding along the first row:

A⃗=i^ (3⋅3−(−2)⋅0)−j^ (1⋅3−(−2)(−1))+k^ (1⋅0−3⋅(−1)).\vec A = \hat i\,(3 \cdot 3 - (-2)\cdot 0) - \hat j\,(1 \cdot 3 - (-2)(-1)) + \hat k\,(1 \cdot 0 - 3 \cdot (-1)).

So

A⃗=i^ (9)−j^ (3−2)+k^ (3)=9 i^−j^+3 k^.\vec A = \hat i\,(9) - \hat j\,(3 - 2) + \hat k\,(3) = 9\,\hat i - \hat j + 3\,\hat k.

Its magnitude is

∣A⃗∣=92+(−1)2+32=81+1+9=91.|\vec A| = \sqrt{9^2 + (-1)^2 + 3^2} = \sqrt{81 + 1 + 9} = \sqrt{91}.

Key takeaways

  • Use the dot product to get cos⁡θ\cos\theta and the cross product magnitude to get sin⁡θ\sin\theta; pick whichever the question gives you.
  • An angle is obtuse exactly when the dot product is negative, which turns the problem into solving an inequality.
  • For definite integrals, the symmetry property ∫0af(x) dx=∫0af(a−x) dx\int_0^a f(x)\,dx = \int_0^a f(a-x)\,dx and a clean substitution are the two go-to tools.
  • Three points are collinear when the third point satisfies the Cartesian equation of the line through the other two.