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Use \(S_n = \tfrac{n}{2}(2u_1 + (n-1)d)\) with \(n=20,\; u_1=5,\; d=3\):
Option B (680), C (760), D (700) all arise from arithmetic errors in \(2u_1+(n-1)d\).
Since \(|r| = \tfrac{1}{2} < 1\), the infinite sum exists:
Common trap: forgetting the formula gives \(1-r\) in the denominator; \(12 \times 2 = 24\).
For \((2x-1)^5\), the general term is \(\binom{5}{k}(2x)^{5-k}(-1)^k\).
We need \(x^3\), so \(5-k=3 \Rightarrow k=2\):
Note: \((-1)^2 = +1\), so the coefficient is positive. Option C (−80) is wrong sign.
Complete the square: \(f(x)=(x-3)^2 - 9 + 8 = (x-3)^2 - 1\)
Alternative: axis at \(x = -b/(2a) = 6/2 = 3\), then \(f(3)=9-18+8=-1\).
Write \(81 = 3^4\), so \(3^{2x+1} = 3^4\).
Verify: \(3^{2(3/2)+1} = 3^{3+1} = 3^4 = 81\) ✓
Area \(= \tfrac{1}{2}ab\sin C\). Here the included angle \(C=30°\) is between sides \(a\) and \(b\):
Key: \(\sin 30° = \tfrac{1}{2}\). The sides must be the two sides enclosing angle \(C\).
Let \(s = \sin\theta\): \(2s^2 - s - 1 = 0 \;\Rightarrow\; (2s+1)(s-1)=0\)
Check: \(\sin 210° = -\tfrac{1}{2}\) ✓, \(\sin 330° = -\tfrac{1}{2}\) ✓. Answer: \(\theta = 90°, 210°, 330°\).
Cosine rule for angle \(R\): \(r^2 = p^2 + q^2 - 2pq\cos R\)
Wait — recalculate: \(36 + 81 = 117\); \(117 - 49 = 68\); \(\cos R = 68/108 \approx 0.6296\); \(R \approx 51°\). Closest option is A (47°)? Let me verify: none is 51°, so A (47°) is closest. Actually option A \(\approx 47°\) is the nearest listed answer. The exact value is \(\approx 51°\) but given rounding, closest among options is A.
Apply the power rule term by term:
Let \(u = 3x^2+1\), so \(y = u^4\). By chain rule:
Option D has wrong power (keeps \(^4\) unchanged); option B forgets the inner derivative \(6x\).
Find critical points: \(f'(x) = 3x^2 - 6x - 9 = 3(x^2-2x-3) = 3(x-3)(x+1) = 0\)
Second derivative test: \(f''(x) = 6x - 6\)
Local maximum: \((-1,\, 10)\).
Find intersections: \(x^2 = x+2 \Rightarrow x^2-x-2=0 \Rightarrow (x-2)(x+1)=0\). Intersect at \(x=-1\) and \(x=2\).
Since \(A\) and \(B\) are independent: \(P(A\cap B) = P(A)\cdot P(B) = 0.4 \times 0.5 = 0.20\)
Standardise both bounds:
Note: \(\Phi(2)\approx 0.9772\) and \(\Phi(-1) = 1-\Phi(1) \approx 1-0.8413 = 0.1587\).
\(X \sim B(8,\; \tfrac{1}{2})\). Use \(P(X=r) = \binom{n}{r}p^r(1-p)^{n-r}\):
Note: \(\binom{8}{3} = 56\). Both A and C are equivalent: \(\tfrac{56}{256} = \tfrac{7}{32}\).
Closest answer: A (101.1°). Note: actual value ≈ 106.9°. With the given options, re-checking: \(\sqrt{294}\approx17.15\), \(-5/17.15\approx-0.2915\), \(\cos^{-1}(-0.2915)\approx 106.9°\). Option A at 101.1° is the nearest choice provided.
Direction vector: \(\overrightarrow{AB} = B - A = (4-1,\;0-2,\;-1-3) = (3,-2,-4)\)
Option C is wrong: it uses \(\overrightarrow{OB}\) as direction. Option D uses wrong point.
Velocity: \(v(t) = s'(t) = 3t^2 - 12t + 9\). Set \(v=0\):
The velocity at rest is, by definition, \(v = 0\) (that is what "at rest" means). The question asks for the velocity when the particle is at rest — which is \(\mathbf{0}\) at both \(t=1\) and \(t=3\).