Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
07-Bld-A5 Building Science — National Exam, May 2017. Six questions of 20 marks each were printed; per the paper's own NOTES only the first five in the answer book are graded, but all six are answered below as a complete study resource.
Reference texts: ASHRAE Handbook — Fundamentals (Chapters 1 Psychrometrics, 14 Climatic Design Information, 16 Ventilation and Infiltration, 25 Thermal and Water Vapor Transmission Data, 26 Heat, Air, and Moisture Control in Building Assemblies); McQuiston, Parker & Spitler, Heating, Ventilating, and Air Conditioning: Analysis and Design; National Building Code of Canada (NBCC).
Check: two inputs are assumed since they were not in the printed data — (1) clock time is taken as solar time (no equation-of-time/longitude correction, the standard simplification at this exam level); (2) ground reflectance ρᵣ = 0.2, the ASHRAE default for ordinary (non-snow) ground.
Find. Total solar irradiation (direct + diffuse + ground-reflected) on the tilted, east-facing collector at the stated time, using the ASHRAE clear-sky model.
A steeper (45°) tilt than a 60° collector turns the surface further toward the zenith, cutting the angle of incidence to the afternoon sun.
Approach. Find the solar position (declination, hour angle, altitude, azimuth) for the stated place/date/time, resolve the angle of incidence on the tilted east-facing surface, then evaluate the ASHRAE clear-sky direct, diffuse and ground-reflected components and sum them.
Solar declination for day n = 202 (July 21):
$$\delta = 23.45\sin\left(\frac{360(284+n)}{365}\right) = 23.45\sin(479.3^\circ) = 20.44^\circ$$
Hour angle at 1:00 PM, one hour past solar noon (15°/hour): H = 15°.
Solar altitude β, from sinβ = cosL·cosδ·cosH + sinL·sinδ:
$$\sin\beta = \cos(44^\circ)\cos(20.44^\circ)\cos(15^\circ) + \sin(44^\circ)\sin(20.44^\circ) = 0.8937 \Rightarrow \boxed{\beta = 63.3^\circ}$$
Solar azimuth φ (from south, +west), from sinφ = cosδ·sinH/cosβ:
$$\sin\phi = \frac{\cos(20.44^\circ)\sin(15^\circ)}{\cos(63.3^\circ)} = 0.540 \Rightarrow \phi = 32.7^\circ\ \text{(west of south, afternoon)}$$
Angle of incidence θ on the tilted east-facing surface (surface azimuth γ = −90° from south), using
$$\cos\theta = \cos\beta\cos(\phi-\gamma)\sin\Sigma + \sin\beta\cos\Sigma$$
$$\cos\theta = \cos(63.3^\circ)\cos(122.7^\circ)\sin(45^\circ) + \sin(63.3^\circ)\cos(45^\circ) = 0.460 \Rightarrow \boxed{\theta = 62.6^\circ}$$
The shallower 45° tilt (vs. a steeper collector) points more toward the zenith and less toward the low afternoon sun, but still catches it at a moderate incidence angle rather than a grazing one.
Direct-normal irradiation, ASHRAE clear-sky model, July constants A = 1085 W/m², B = 0.207:
$$I_{DN} = \frac{A}{\exp(B/\sin\beta)} = \frac{1085}{\exp(0.207/0.894)} = 861\ \text{W/m}^2$$
Direct component on the tilted surface:
$$I_{DT} = I_{DN}\cos\theta = 861\times 0.460 = 396\ \text{W/m}^2$$