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Daily · 2026-08-05

Daily math problems for August 5, 2026 — Combinatorics, Limits, Derivatives & more

One bite-sized math problem set for the day. Solve the ten multiple-choice problems and reveal the worked solutions.

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🇷🇴 RO M1
Mediumcombinatorics
The number of -element subsets of a -element set is:

Problems & worked solutions

🇷🇴 RO M1

Problem 1 — Permutations & Combinations

The number of 333-element subsets of a 555-element set is:

Show answer & worked solution
  1. A. 555
  2. B. 101010✓ correct
  3. C. 151515
  4. D. 606060

(53)=5!3!⋅2!=10\binom{5}{3} = \dfrac{5!}{3! \cdot 2!} = 10(35​)=3!⋅2!5!​=10.

🇷🇴 RO M1

Problem 2 — Limits

Find lim⁡x→∞x1/x\displaystyle\lim_{x\to\infty}x^{1/\sqrt{x}}x→∞lim​x1/x​.

Show answer & worked solution
  1. A. eee
  2. B. +∞+\infty+∞
  3. C. 111✓ correct
  4. D. 000
  5. E. e2e^2e2
  6. F. e\sqrt{e}e​

∙\bullet∙ Rewrite as an exponential:

x1/x=eln⁡x/xx^{1/\sqrt{x}}=e^{\ln x/\sqrt{x}}x1/x​=elnx/x​

∙\bullet∙ Apply L'Hôpital to the exponent:

lim⁡x→∞ln⁡xx=lim⁡x→∞2x=0\lim_{x\to\infty}\frac{\ln x}{\sqrt{x}}=\lim_{x\to\infty}\frac{2}{\sqrt{x}}=0x→∞lim​x​lnx​=x→∞lim​x​2​=0

∙\bullet∙ Exponentiate:

L=e0=1L=e^0=1L=e0=1

🇷🇴 RO M1

Problem 3 — Calculus

If f(x)=e2xf(x) = e^{2x}f(x)=e2x, the value of f′(0)f'(0)f′(0) is:

Show answer & worked solution
  1. A. 222✓ correct
  2. B. 111
  3. C. 000
  4. D. e2e^2e2

f′(x)=2e2xf'(x) = 2e^{2x}f′(x)=2e2x, so f′(0)=2⋅e0=2f'(0) = 2 \cdot e^0 = 2f′(0)=2⋅e0=2.

🇷🇴 RO M1

Problem 4 — Functions — General Properties

For f:R→Rf: \mathbb{R} \to \mathbb{R}f:R→R, f(x)=x3f(x) = x^3f(x)=x3, which statement is correct?

Show answer & worked solution
  1. A. fff is neither injective nor surjective
  2. B. fff is injective but not surjective
  3. C. fff is surjective but not injective
  4. D. fff is bijective✓ correct

fff is strictly increasing on R\mathbb{R}R, hence injective. For every y∈Ry \in \mathbb{R}y∈R, x=y3x = \sqrt[3]{y}x=3y​ satisfies f(x)=yf(x) = yf(x)=y, hence surjective. So fff is bijective, with f−1(y)=y3f^{-1}(y) = \sqrt[3]{y}f−1(y)=3y​.

🇷🇴 RO M1

Problem 5 — Distances & Areas

The set of points (x,y)(x, y)(x,y) equidistant from A(0,0)A(0, 0)A(0,0) and B(4,0)B(4, 0)B(4,0) is the line:

Show answer & worked solution
  1. A. y=2y = 2y=2
  2. B. y=0y = 0y=0
  3. C. x=2x = 2x=2✓ correct
  4. D. x=0x = 0x=0

Set x2+y2=(x−4)2+y2\sqrt{x^2 + y^2} = \sqrt{(x - 4)^2 + y^2}x2+y2​=(x−4)2+y2​. Squaring: x2=(x−4)2=x2−8x+16x^2 = (x - 4)^2 = x^2 - 8x + 16x2=(x−4)2=x2−8x+16, so 8x=168x = 168x=16, x=2x = 2x=2.

🇷🇴 RO M1

Problem 6 — Trigonometry

Find cos⁡20°⋅cos⁡40°⋅cos⁡80°\cos 20°\cdot\cos 40°\cdot\cos 80°cos20°⋅cos40°⋅cos80°.

Show answer & worked solution
  1. A. 12\dfrac{1}{2}21​
  2. B. 14\dfrac{1}{4}41​
  3. C. 18\dfrac{1}{8}81​✓ correct
  4. D. 38\dfrac{\sqrt{3}}{8}83​​
  5. E. 116\dfrac{1}{16}161​
  6. F. 28\dfrac{\sqrt{2}}{8}82​​

∙\bullet∙ Multiply numerator and denominator by 2sin⁡20°2\sin 20°2sin20° and use 2sin⁡θcos⁡θ=sin⁡2θ2\sin\theta\cos\theta=\sin 2\theta2sinθcosθ=sin2θ:

cos⁡20°cos⁡40°cos⁡80°=sin⁡40°cos⁡40°cos⁡80°2sin⁡20°\cos 20°\cos 40°\cos 80° = \dfrac{\sin 40°\cos 40°\cos 80°}{2\sin 20°}cos20°cos40°cos80°=2sin20°sin40°cos40°cos80°​

∙\bullet∙ Apply the identity again:

=sin⁡80°cos⁡80°4sin⁡20°= \dfrac{\sin 80°\cos 80°}{4\sin 20°}=4sin20°sin80°cos80°​

∙\bullet∙ And once more:

=sin⁡160°8sin⁡20°= \dfrac{\sin 160°}{8\sin 20°}=8sin20°sin160°​

∙\bullet∙ Use sin⁡160°=sin⁡(180°−20°)=sin⁡20°\sin 160° = \sin(180°-20°) = \sin 20°sin160°=sin(180°−20°)=sin20°:

=sin⁡20°8sin⁡20°=18= \dfrac{\sin 20°}{8\sin 20°} = \dfrac{1}{8}=8sin20°sin20°​=81​

🇷🇴 RO M1

Problem 7 — Distances & Areas

A quadrilateral ABCDABCDABCD has vertices A(0,0),B(4,0),C(5,3),D(1,3)A(0,0), B(4,0), C(5,3), D(1,3)A(0,0),B(4,0),C(5,3),D(1,3). Its area is:

Show answer & worked solution
  1. A. 999
  2. B. 101010
  3. C. 121212✓ correct
  4. D. 151515

AB→=(4,0)\overrightarrow{AB} = (4, 0)AB=(4,0) and DC→=(4,0)\overrightarrow{DC} = (4, 0)DC=(4,0) — same vector, so ABCDABCDABCD is a parallelogram. Base =4= 4=4, height =3= 3=3. Area =12= 12=12.

🌍 International

Problem 8 — Calculus

∑n=1∞1n2\displaystyle\sum_{n=1}^{\infty} \dfrac{1}{n^2}n=1∑∞​n21​ equals:

Show answer & worked solution
  1. A. π26\tfrac{\pi^2}{6}6π2​✓ correct
  2. B. π24\tfrac{\pi^2}{4}4π2​
  3. C. π4\tfrac{\pi}{4}4π​
  4. D. 111

Euler's classical result: ∑n=1∞1n2=π26\displaystyle\sum_{n=1}^{\infty}\dfrac{1}{n^2} = \dfrac{\pi^2}{6}n=1∑∞​n21​=6π2​.

🇷🇴 RO M1

Problem 9 — L'Hôpital's Rule

Evaluate lim⁡x→0ex−1−xx2\displaystyle\lim_{x\to 0} \dfrac{e^x - 1 - x}{x^2}x→0lim​x2ex−1−x​.

Show answer & worked solution
  1. A. 000
  2. B. 12\dfrac{1}{2}21​✓ correct
  3. C. 111
  4. D. 222

Direct substitution gives 00\tfrac{0}{0}00​. Differentiate top and bottom: lim⁡x→0ex−12x\displaystyle\lim_{x\to 0}\dfrac{e^x - 1}{2x}x→0lim​2xex−1​ — still 00\tfrac{0}{0}00​. Once more: lim⁡x→0ex2=12\displaystyle\lim_{x\to 0}\dfrac{e^x}{2} = \dfrac{1}{2}x→0lim​2ex​=21​.

🌍 International

Problem 10 — Integrals

Evaluate ∫01ln⁡(1+x)1+x2 dx\int_0^1 \frac{\ln(1+x)}{1+x^2}\,dx∫01​1+x2ln(1+x)​dx

Show answer & worked solution
  1. A. πln⁡24\dfrac{\pi \ln 2}{4}4πln2​
  2. B. πln⁡28\dfrac{\pi \ln 2}{8}8πln2​✓ correct
  3. C. πln⁡216\dfrac{\pi \ln 2}{16}16πln2​
  4. D. π2ln⁡28\dfrac{\pi^2 \ln 2}{8}8π2ln2​
  5. E. ln⁡22\dfrac{\ln 2}{2}2ln2​
  6. F. π8\dfrac{\pi}{8}8π​

Substitute x=tan⁡θx = \tan\thetax=tanθ. Then dx=sec⁡2θ dθdx = \sec^2\theta\,d\thetadx=sec2θdθ and 1+x2=sec⁡2θ1 + x^2 = \sec^2\theta1+x2=sec2θ, so the sec⁡2θ\sec^2\thetasec2θ on top and bottom cancel cleanly. The bounds 0→10 \to 10→1 map to θ:0→π/4\theta : 0 \to \pi/4θ:0→π/4:

I=∫0π/4ln⁡(1+tan⁡θ) dθ.I = \int_0^{\pi/4} \ln(1 + \tan\theta)\,d\theta.I=∫0π/4​ln(1+tanθ)dθ.

Reflect by ϕ=π/4−θ\phi = \pi/4 - \thetaϕ=π/4−θ. The angle-difference formula gives tan⁡(π/4−ϕ)=1−tan⁡ϕ1+tan⁡ϕ\tan(\pi/4 - \phi) = \dfrac{1 - \tan\phi}{1 + \tan\phi}tan(π/4−ϕ)=1+tanϕ1−tanϕ​, so

1+tan⁡θ  =  1+1−tan⁡ϕ1+tan⁡ϕ  =  21+tan⁡ϕ.1 + \tan\theta \;=\; 1 + \frac{1 - \tan\phi}{1 + \tan\phi} \;=\; \frac{2}{1 + \tan\phi}.1+tanθ=1+1+tanϕ1−tanϕ​=1+tanϕ2​.

Taking logs:   ln⁡(1+tan⁡θ)=ln⁡2−ln⁡(1+tan⁡ϕ)\;\ln(1 + \tan\theta) = \ln 2 - \ln(1 + \tan\phi)ln(1+tanθ)=ln2−ln(1+tanϕ).

Pair the integral with its reflected twin. Renaming the dummy variable ϕ→θ\phi \to \thetaϕ→θ (the bounds are unchanged because the substitution is a reflection of [0,π/4][0, \pi/4][0,π/4] onto itself):

I  =  ∫0π/4[ln⁡2−ln⁡(1+tan⁡θ)] dθ  =  π4ln⁡2  −  I.I \;=\; \int_0^{\pi/4} \bigl[\ln 2 - \ln(1 + \tan\theta)\bigr]\,d\theta \;=\; \frac{\pi}{4}\ln 2 \;-\; I.I=∫0π/4​[ln2−ln(1+tanθ)]dθ=4π​ln2−I.

Solve.   2I=π4ln⁡2\;2I = \dfrac{\pi}{4}\ln 22I=4π​ln2, so

 I=π8ln⁡2 .\boxed{\,I = \frac{\pi}{8}\ln 2\,.}I=8π​ln2.​

The reflection trick — pairing f(θ)f(\theta)f(θ) with f(π/4−θ)f(\pi/4 - \theta)f(π/4−θ) — works whenever the integrand simplifies under that reflection. Worth keeping in your toolbox alongside the half-angle and Weierstrass substitutions.

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