Standard Distribution Results - Statistics Graduate Level

  1. Under H0:μX−μY=δ0H_0:\mu_X-\mu_Y=\delta_0, which statistic has an exact standard tt distribution?
    Answer: Xˉ−Yˉ−δ0Sp1/8+4/10∼t16\frac{\bar X-\bar Y-\delta_0}{S_p\sqrt{1/8+4/10}}\sim t_{16}, correctly accounting for the unequal population variances When both samples share a common variance parameter σ2\sigma^2 but with different multipliers, you need to construct a pooled estimator that recovers exactly one σ2\sigma^2, then build the standard error accordingly. Here, Var(Xi)=σ2\text{Var}(X_i)=\sigma^2 and Var(Yj)=4σ2\text{Var}(Y_j)=4\sigma^2, so Yj−μY2\frac{Y_j-\mu_Y}{2} has variance σ2\sigma^2. This means 14∑j=110(Yj−Yˉ)2\frac{1}{4}\sum_{j=1}^{10}(Y_j-\bar{Y})^2 is a chi-squared quantity scaled by σ2\sigma^2 with 9 degrees of freedom. Combined with ∑i=18(Xi−Xˉ)2/σ2∼χ72\sum_{i=1}^{8}(X_i-\bar{X})^2/\sigma^2 \sim \chi^2_7, the pooled Sp2S_p^2 satisfies 16Sp2/σ2∼χ16216S_p^2/\sigma^2 \sim \chi^2_{16}, giving 16 degrees of freedom. Now consider the standard error of Xˉ−Yˉ\bar{X}-\bar{Y}: Var(Xˉ−Yˉ)=σ28+4σ210=σ2 ⁣(18+410)\text{Var}(\bar{X}-\bar{Y})=\frac{\sigma^2}{8}+\frac{4\sigma^2}{10}=\sigma^2\!\left(\frac{1}{8}+\frac{4}{10}\right). Dividing by SpS_p (which estimates σ\sigma) yields an exact t16t_{16} distribution, confirming B is correct. A is wrong because it uses 1/8+1/10\sqrt{1/8+1/10}, which ignores the factor of 4 in Var(Yj)\text{Var}(Y_j), underestimating the true standard error. C uses the correct standard error but claims t17t_{17} degrees of freedom — there is no justification for nX+nY−1=17n_X+n_Y-1=17; the degrees of freedom come from the chi-squared structure of Sp2S_p^2, which is 16. D flips the variance multiplier, incorrectly applying 4 to the XX sample and 1 to the YY sample, producing the wrong standard error entirely. Your study tip: whenever variances are proportional (kσ2k\sigma^2), rescale each sample's sum of squares by 1/k1/k before pooling — this forces everything back to a common σ2\sigma^2 scale and keeps your degrees of freedom and standard error both correct.
  2. What is the distribution of QQ?
    Answer: A noncentral chi-square distribution, χ8′2(2)\chi'^2_8(2) Whenever you see a sum of squared standardized normal variables, ask yourself two questions: how many terms are there, and are those terms truly standard normal? Here, each term in Q=∑i=18(Xi−μ0)2/σ2Q = \sum_{i=1}^8 (X_i - \mu_0)^2/\sigma^2 has the form (Xi−μ0σ)2\left(\frac{X_i - \mu_0}{\sigma}\right)^2. Since Xi∼N(μ,σ2)=N(μ0+σ/2,σ2)X_i \sim N(\mu, \sigma^2) = N(\mu_0 + \sigma/2, \sigma^2), we can write Xi−μ0σ=Xi−μσ+μ−μ0σ=Zi+12\frac{X_i - \mu_0}{\sigma} = \frac{X_i - \mu}{\sigma} + \frac{\mu - \mu_0}{\sigma} = Z_i + \frac{1}{2}, where Zi∼N(0,1)Z_i \sim N(0,1). So each term is a squared normal with a nonzero mean of 1/21/2, not a standard normal. By definition, a sum of kk independent squared normals N(λi,1)N(\lambda_i, 1) follows a noncentral chi-square χk′2(δ)\chi'^2_k(\delta), where δ=∑λi2\delta = \sum \lambda_i^2 is the noncentrality parameter. Here k=8k = 8 terms and δ=∑i=18(1/2)2=8⋅1/4=2\delta = \sum_{i=1}^8 (1/2)^2 = 8 \cdot 1/4 = 2. This confirms the distribution is χ8′2(2)\chi'^2_8(2), making D correct. A is wrong because χ72\chi^2_7 has only 7 degrees of freedom — nothing here subtracts a mean estimate, which would cost one degree of freedom. B gets the degrees of freedom right (8 terms = 8 df) but incorrectly assumes centrality, ignoring that μ≠μ0\mu \neq \mu_0. C compounds both errors: it uses 7 degrees of freedom and correctly identifies noncentrality, but loses a degree of freedom with no justification. Your key rule: degrees of freedom equal the number of squared terms, and noncentrality arises whenever those normals have nonzero means — compute δ=∑λi2\delta = \sum \lambda_i^2 from those means.
  3. Which identity follows from the reciprocal property of the FF distribution?
    Answer: 1c=q0.025(11,7)\frac{1}{c}=q_{0.025}(11,7) Whenever you see a question involving quantiles of the FF distribution, the reciprocal property is the key tool. It states that if X∼F(a,b)X \sim F(a,b), then 1/X∼F(b,a)1/X \sim F(b,a). This has a direct consequence for quantiles: qp(a,b)=1q1−p(b,a)q_p(a,b) = \frac{1}{q_{1-p}(b,a)}, because flipping the random variable swaps the tail probabilities. Here, c=q0.975(7,11)c = q_{0.975}(7,11) means P(X≤c)=0.975P(X \leq c) = 0.975 for X∼F(7,11)X \sim F(7,11). Since 1/X∼F(11,7)1/X \sim F(11,7), the event X≤cX \leq c is equivalent to 1/X≥1/c1/X \geq 1/c, so P(1/X≥1/c)=0.975P(1/X \geq 1/c) = 0.975, which means P(1/X≤1/c)=0.025P(1/X \leq 1/c) = 0.025. Therefore 1/c=q0.025(11,7)1/c = q_{0.025}(11,7), confirming answer D. Now consider why the other choices fail. A claims 1/c=q0.975(11,7)1/c = q_{0.975}(11,7), but that would mean 1/c1/c sits at the upper 2.5% tail of F(11,7)F(11,7), not the lower — the reciprocal operation flips which tail you're in. B claims 1/c=q0.025(7,11)1/c = q_{0.025}(7,11), which keeps the degrees of freedom in the original order (7,11)(7,11) — but the reciprocal property swaps the degrees of freedom. C claims c=q0.025(11,7)c = q_{0.025}(11,7), which correctly swaps the degrees of freedom and correctly identifies the 0.025 quantile, but forgets to take the reciprocal of cc. A clean memory aid: reciprocal → swap d.f. AND flip tail probability (p→1−pp \to 1-p). Missing either half of that transformation leads directly to one of the wrong answers.
  4. Under the null hypothesis μ=μ0\mu=\mu_0, what is the distribution of W=12(Xˉ−μ0)2S2W=\frac{12(\bar X-\mu_0)^2}{S^2}?
    Answer: W∼F1,11W\sim F_{1,11} because it is the square of a t11t_{11} variable Whenever you see a ratio involving a squared standardized mean and a sample variance, your first instinct should be to connect it to the relationship between the tt, FF, and χ2\chi^2 distributions. Start by recognizing that under H0:μ=μ0H_0: \mu = \mu_0, the statistic T=Xˉ−μ0S/12T = \frac{\bar{X} - \mu_0}{S/\sqrt{12}} follows a t11t_{11} distribution, since the sample mean is standardized by the estimated standard error with n−1=11n-1 = 11 degrees of freedom. Now notice that squaring TT gives exactly WW: T2=(Xˉ−μ0)2S2/12=12(Xˉ−μ0)2S2=WT^2 = \frac{(\bar{X}-\mu_0)^2}{S^2/12} = \frac{12(\bar{X}-\mu_0)^2}{S^2} = W A fundamental identity in distribution theory states that if T∼tνT \sim t_\nu, then T2∼F1,νT^2 \sim F_{1,\nu}. Therefore W∼F1,11W \sim F_{1,11}, confirming B is correct. Choice A is tempting but wrong: 12(Xˉ−μ0)2σ2\frac{12(\bar{X}-\mu_0)^2}{\sigma^2} would be χ12\chi^2_1 if σ2\sigma^2 were known, but here S2S^2 replaces σ2\sigma^2, fundamentally changing the distribution. Choice C confuses the degree-of-freedom ordering — the 1111 comes from the denominator (the variance estimate), not the numerator, so the correct FF has 11 numerator df and 1111 denominator df, not F11,1F_{11,1}. Choice D is wrong because WW is a squared quantity and therefore cannot be negative, ruling out the symmetric tt distribution entirely. Your key takeaway: memorize that T2∼F1,νT^2 \sim F_{1,\nu} when T∼tνT \sim t_\nu. This identity bridges three core distributions and appears frequently on graduate-level exams, especially in ANOVA and regression contexts.
  5. Which expression is an exact equal-tail 95%95\% confidence interval for ρ\rho?
    Answer: [2.4q0.975(9,15),2.4q0.025(9,15)]\left[\frac{2.4}{q_{0.975}(9,15)},\frac{2.4}{q_{0.025}(9,15)}\right] Whenever you see a confidence interval for a ratio of variances, your anchor is the pivot built from the F-distribution. Since (S12/S22)/ρ∼F(9,15)(S_1^2/S_2^2)/\rho \sim F(9,15) (with degrees of freedom n1−1=9n_1-1=9 and n2−1=15n_2-1=15), you can write the probability statement P ⁣(q0.025(9,15)≤S12/S22ρ≤q0.975(9,15))=0.95.P\!\left(q_{0.025}(9,15) \leq \frac{S_1^2/S_2^2}{\rho} \leq q_{0.975}(9,15)\right) = 0.95. Inverting all parts of the inequality to isolate ρ\rho — remembering that dividing by ρ\rho and flipping inequalities gives you ρ\rho sandwiched between S12/S22q0.975(9,15)\frac{S_1^2/S_2^2}{q_{0.975}(9,15)} and S12/S22q0.025(9,15)\frac{S_1^2/S_2^2}{q_{0.025}(9,15)} — and plugging in S12/S22=2.4S_1^2/S_2^2 = 2.4 yields exactly Answer A: [2.4q0.975(9,15), 2.4q0.025(9,15)].\left[\frac{2.4}{q_{0.975}(9,15)},\,\frac{2.4}{q_{0.025}(9,15)}\right]. This is correct because dividing by the larger quantile gives the smaller bound, preserving proper interval orientation. B swaps the degrees of freedom to (15,9)(15, 9), which would apply if the ratio were inverted — a common mix-up when students confuse which sample is "1" versus "2." C multiplies rather than divides by the quantiles, which inverts the algebraic manipulation incorrectly; this would only make sense if ρ\rho appeared in the numerator of the pivot. D divides the quantiles by 2.42.4 instead of dividing 2.42.4 by the quantiles — a simple algebra reversal that flips numerator and denominator. The key study tip: always write the pivot explicitly, then invert the inequalities step by step. The degrees of freedom always follow the order (n1−1,n2−1)(n_1-1, n_2-1) matching the ratio S12/S22S_1^2/S_2^2, and dividing flips the quantile positions.
  6. Which statement about RR and WW is correct?
    Answer: R∼F5,12R\sim F_{5,12}, and RR is independent of WW Whenever you see a ratio of chi-squared variables scaled by their degrees of freedom, think F-distribution — and whenever you see a sum of independent chi-squared variables, think about whether the ratio and sum share any information. Recall the definition: if X∼χm2X \sim \chi^2_m and Y∼χn2Y \sim \chi^2_n are independent, then X/mY/n∼Fm,n\frac{X/m}{Y/n} \sim F_{m,n}. Here, R=12U5V=U/5V/12R = \frac{12U}{5V} = \frac{U/5}{V/12}, which matches exactly this form with m=5m=5 and n=12n=12, so R∼F5,12R \sim F_{5,12}. That confirms the distribution in choice A. For independence, the key insight comes from a classical result: for independent chi-squared variables, the ratio U/VU/V (equivalently RR) is independent of the sum W=U+VW = U + V. This is analogous to how the sample variance and sample mean are independent in normal sampling — the "direction" and "magnitude" of the vector (U,V)(U, V) carry separate information. A formal proof uses the Jacobian transformation: writing (U,V)(U, V) in terms of (W,R)(W, R) shows the joint density factors into a function of WW alone times a function of RR alone, establishing independence. So A is correct. Choice B correctly identifies the distribution but wrongly claims dependence — the factorization argument shows independence holds. Choice C reverses the degrees of freedom; since U∼χ52U \sim \chi^2_5 is in the numerator scaled by 5, the first index must be 5, not 12. Choice D misidentifies the distribution entirely — a scaled ratio of chi-squared variables is not itself chi-squared. As a study tip: memorize the F-distribution definition carefully, paying attention to which degree of freedom goes in the numerator. The order Fm,nF_{m,n} always corresponds to χm2/mχn2/n\frac{\chi^2_m/m}{\chi^2_n/n}, and swapping them gives a different distribution.
  7. For the directional alternative that the coefficient is less than its null value, what is the exact one-sided pp-value?
    Answer: pF2\frac{p_F}{2}, because the observed tt statistic has the alternative-consistent sign Whenever you see a question linking a two-sided tt test to its equivalent FF test, the key insight is understanding what squaring the tt statistic actually destroys: the sign information. That sign is precisely what determines which one-sided tail is relevant. The relationship between the two distributions is exact: if T∼tνT \sim t_\nu, then T2∼F1,νT^2 \sim F_{1,\nu}. This means P(F1,ν≥tobs2)=P(∣T∣≥∣tobs∣)P(F_{1,\nu} \ge t_{\text{obs}}^2) = P(|T| \ge |t_{\text{obs}}|), which is the two-sided pp-value. So pFp_F already equals the two-sided pp-value. For a one-sided alternative, you simply take half of that — but only when the observed statistic falls in the direction consistent with the alternative. Here, the alternative is that the coefficient is less than its null value, and tobs=−2.4t_{\text{obs}} = -2.4 is indeed negative (alternative-consistent). The exact one-sided pp-value is therefore pF/2p_F/2, confirming C. Choice A is wrong because pFp_F is the two-sided pp-value disguised as a one-tailed quantity — the FF test is inherently two-sided since it only uses F≥0F \ge 0. Choice B, 2pF2p_F, would actually double the two-sided pp-value, yielding something greater than 1 in extreme cases — clearly nonsensical. Choice D, 1−pF/21 - p_F/2, corresponds to the probability in the wrong tail of tνt_\nu (i.e., t>0t > 0), which would be relevant if the alternative were that the coefficient is greater than its null value. Study tip: Always check whether the sign of tobst_{\text{obs}} aligns with your directional alternative before halving pFp_F. If it does, one-sided p=pF/2p = p_F/2; if it doesn't, one-sided p=1−pF/2p = 1 - p_F/2.
  8. Which statistic has the stated distribution?
    Answer: 9SX2SY2∼F9,13\frac{9S_X^2}{S_Y^2}\sim F_{9,13} Whenever you see a question involving ratios of sample variances from normal populations, your goal is to construct an FF-statistic by making each chi-squared component standardized — that is, divided by its true population variance. Recall the key result: if S2S^2 is the sample variance from a normal population with true variance σ2\sigma^2 and sample size nn, then (n−1)S2σ2∼χn−12\frac{(n-1)S^2}{\sigma^2} \sim \chi^2_{n-1}. An FF-statistic is formed as a ratio of two independent chi-squared variables, each divided by their degrees of freedom: F=χm2/mχk2/k∼Fm,kF = \frac{\chi^2_{m}/m}{\chi^2_{k}/k} \sim F_{m,k} For the first sample (size 10, variance σ2\sigma^2): 9SX2σ2∼χ92\frac{9S_X^2}{\sigma^2} \sim \chi^2_9. For the second sample (size 14, variance 9σ29\sigma^2): 13SY29σ2∼χ132\frac{13S_Y^2}{9\sigma^2} \sim \chi^2_{13}. Forming the ratio of these (each divided by their df) and canceling σ2\sigma^2: (9SX2/σ2)/9(13SY2/9σ2)/13=9SX2SY2∼F9,13\frac{(9S_X^2/\sigma^2)/9}{(13S_Y^2/9\sigma^2)/13} = \frac{9S_X^2}{S_Y^2} \sim F_{9,13} This confirms A is correct. B flips the numerator and denominator, which would give F13,9F_{13,9}, not F9,13F_{9,13}. C uses SX29SY2\frac{S_X^2}{9S_Y^2}, which fails to properly standardize by the true variances — the factor of 9 is misplaced, so the σ2\sigma^2 terms don't cancel cleanly. D uses degrees of freedom 10 and 14 instead of the correct n−1n-1 values of 9 and 13 — a classic off-by-one error. Your study tip: always subtract 1 from each sample size for the degrees of freedom, and carefully track which population variance belongs to which sample before constructing the ratio.
  9. What is the distribution of T=(Z′AZ+Z′CZ)/6Z′BZ/4T=\frac{(Z'AZ+Z'CZ)/6}{Z'BZ/4}?
    Answer: T∼F6,4T\sim F_{6,4} because the numerator is a rank-66 orthogonal projection Whenever you see a ratio of quadratic forms involving a standard normal vector, your instinct should be to check whether the forms correspond to independent chi-squared random variables — that's the foundation of the F-distribution. Here, since AA is symmetric idempotent of rank 3, Z′AZ∼χ32Z'AZ \sim \chi^2_3. Similarly, BB is symmetric idempotent of rank 4, so Z′BZ∼χ42Z'BZ \sim \chi^2_4. Now consider C=I10−A−BC = I_{10} - A - B. Because AB=0AB = 0 and both matrices are symmetric idempotent, CC is also symmetric idempotent with rank 10−3−4=310 - 3 - 4 = 3, so Z′CZ∼χ32Z'CZ \sim \chi^2_3. Crucially, the condition AB=0AB = 0 implies mutual orthogonality among AA, BB, and CC, which guarantees that Z′AZZ'AZ, Z′BZZ'BZ, and Z′CZZ'CZ are mutually independent (by the Craig–Cochran theorem). Therefore, Z′AZ+Z′CZ∼χ3+32=χ62Z'AZ + Z'CZ \sim \chi^2_{3+3} = \chi^2_6, and the ratio becomes: T=(Z′AZ+Z′CZ)/6Z′BZ/4∼F6,4T = \frac{(Z'AZ + Z'CZ)/6}{Z'BZ/4} \sim F_{6,4} This confirms C is correct — the numerator pools two orthogonal rank-3 projections for a total rank of 6, giving an F6,4F_{6,4} distribution. A is wrong because it ignores Z′CZZ'CZ's contribution, treating only AA as generating numerator degrees of freedom. B inverts the degree-of-freedom parameters entirely — the numerator rank (6) always comes first. D is wrong because while Z′AZ+Z′BZ+Z′CZ=Z′Z∼χ102Z'AZ + Z'BZ + Z'CZ = Z'Z \sim \chi^2_{10}, the ratio TT is not itself a chi-squared random variable. Study tip: Always verify idempotency and mutual orthogonality (AB=0AB = 0 for all pairs) before invoking Cochran's theorem — these two conditions together unlock independence of quadratic forms.
  10. What is the general linear hypothesis test statistic, and what is its null distribution?
    Answer: 3.003.00, with null distribution F2,24F_{2,24} When you encounter a general linear hypothesis test, the key quantities are the number of restrictions qq, the residual degrees of freedom from the full model n−pn - p, and the two residual sums of squares. Here, n=30n = 30, p=6p = 6 (rank of full design matrix), and q=2q = 2 restrictions. The F-statistic is constructed as: F=(RSSR−RSSF)/qRSSF/(n−p)=(150−120)/2120/(30−6)=30/2120/24=155=3.00F = \frac{(RSS_R - RSS_F)/q}{RSS_F/(n-p)} = \frac{(150 - 120)/2}{120/(30-6)} = \frac{30/2}{120/24} = \frac{15}{5} = 3.00 Under the null hypothesis, this statistic follows an Fq, n−p=F2,24F_{q,\, n-p} = F_{2,24} distribution. That confirms C is correct. Looking at why each distractor fails: A gets the F-statistic wrong — dividing 30/2=1530/2 = 15 by 120/24=5120/24 = 5 gives 3.003.00, not 6.006.00. Answer A likely results from forgetting to divide the numerator by q=2q = 2, treating the raw difference RSSR−RSSF=30RSS_R - RSS_F = 30 over 55 instead. B correctly computes the F-statistic as 3.003.00 but uses n−p−1=23n - p - 1 = 23 as the denominator degrees of freedom — a confusion with the slope-only degrees of freedom adjustment sometimes seen in simple regression. The denominator df is simply n−pn - p, not n−p−1n - p - 1. D inverts the F-ratio entirely, yielding 1/3≈0.3331/3 \approx 0.333, and also reverses the degrees of freedom order to F24,2F_{24,2}, which is a fundamental structural error. A reliable memory anchor: the denominator degrees of freedom equal n−rank(X)n - \text{rank}(X), and the numerator degrees of freedom equal the number of restrictions qq. Never subtract an extra 1 unless the model has a specific intercept adjustment built in separately.

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