Normal families are closed under affine combination: if X i ∼ N ( μ i , σ i 2 ) X_i\sim\mathcal N(\mu_i,\sigma_i^2) X i ∼ N ( μ i , σ i 2 ) independently, then ∑ a i X i ∼ N ( ∑ a i μ i , ∑ a i 2 σ i 2 ) \sum a_iX_i\sim\mathcal N(\sum a_i\mu_i,\sum a_i^2\sigma_i^2) ∑ a i X i ∼ N ( ∑ a i μ i , ∑ a i 2 σ i 2 ) . For centred independent (or jointly) normals, symmetry gives P ( linear combo > 0 ) = 1 / 2 \mathbb P(\text{linear combo}>0)=1/2 P ( linear combo > 0 ) = 1/2 . CLT: for i.i.d. terms with mean μ \mu μ , variance σ 2 \sigma^2 σ 2 , S n − n μ σ n → N ( 0 , 1 ) \frac{S_n-n\mu}{\sigma\sqrt n}\to\mathcal N(0,1) σ n S n − n μ → N ( 0 , 1 ) , so P ( S n ≤ x ) ≈ Φ ( x − n μ σ n ) \mathbb P(S_n\le x)\approx\Phi\!\big(\frac{x-n\mu}{\sigma\sqrt n}\big) P ( S n ≤ x ) ≈ Φ ( σ n x − n μ ) .
Standard bivariate normal with correlation ρ \rho ρ : rotational symmetry (for ρ = 0 \rho=0 ρ = 0 ) makes the probability of a wedge of angle θ \theta θ through the origin equal θ / 2 π \theta/2\pi θ /2 π ; more generally, Sheppard’s formula gives
P ( X > 0 , Y > 0 ) = 1 4 + arcsin ρ 2 π . \mathbb P(X>0,Y>0)=\frac14+\frac{\arcsin\rho}{2\pi}. P ( X > 0 , Y > 0 ) = 4 1 + 2 π arcsin ρ .
For a small target of width w w w at point t t t , hit probability ≈ w f ( t ) \approx w\,f(t) ≈ w f ( t ) where f f f is the aiming density; to split effort among several tiny targets, maximise ∑ i w i f ( t i ; μ , σ ) \sum_i w_i f(t_i;\mu,\sigma) ∑ i w i f ( t i ; μ , σ ) over the aim μ \mu μ .