Key relationship
Lens q=fd/(d−f); centre condition q−P=R; convex mirror f=−R/2.
Physics · Practical apparatus
Use a convex lens to create a converging beam aimed at a point behind the convex mirror. Adjust mirror position until that point matches its centre of curvature. Normal incidence on the sphere makes rays retrace.
Open the interactive experiment →குவி லென்சின் குவியும் கதிர்களை குவி ஆடியின் வளைவு மையத்தை நோக்கி அமைத்து ஒத்துப்பார்க்கவும்.
Lens q=fd/(d−f); centre condition q−P=R; convex mirror f=−R/2.
Use a convex lens to create a converging beam aimed at a point behind the convex mirror. Adjust mirror position until that point matches its centre of curvature. Normal incidence on the sphere makes rays retrace.
The centre-coincidence estimate is not valid away from the retracing condition.
Ideal lens converging to a point behind the convex mirror. The centre-coincidence condition causes retracing. Focal estimate is meaningful only when residual≈0 and the first image lies behind the mirror.
Infer convex-mirror radius using a known converging focus.
Try both scenarios, change one control, and predict the result before checking the graph and readouts.
Change one input while keeping the others fixed, as you would in a controlled experiment.
Lens f20,d30 gives I60 cm; mirror P40 and R20 gives coincidence and fmirror−10 cm.
The model connects convex mirror with converging lens with an observable reading. Check the equation and assumptions before applying it.
SI units · algebra · graph reading
A spherical mirror focal-length magnitude is?
Paraxial f=R/2; convex sign is negative in the stated convention.
Course connection: Virtual apparatus preparation. Check exact board/exam membership in the syllabus sources. Physical practical work remains necessary.