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An electron at rest is accelerated from point A by a potential difference ΔV1. It then enters the middle of two parallel conducting plates of length L, separated by a distance d and subjected to a potential difference ΔV2. The electron hits the top plate, right in the middle, as shown in the figure. The potential difference ΔV2 as a function of (L, ΔV1, d) is:

An electron at rest is accelerated from point A by a potential difference ΔV1. It then enters the middle of two parallel conducting plates of length L, separated by a distance d and subjected to a potential difference ΔV2. The electron hits the top plate, right in the middle, as shown in the figure. The potential difference ΔV2 as a function of (L, ΔV1, d) is:

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An electron at rest is accelerated from point A by a potential difference ΔV1. It then enters the middle of two parallel conducting plates of length L, separated by a distance d and subjected to a potential difference ΔV2. The electron hits the top plate, right in the middle, as shown in the figure. The potential difference ΔV2 as a function of (L, ΔV1, d) is:


L/2 -C A в AV2 L AV:
Transcribed Image Text:L/2 -C A в AV2 L AV:
O a. AV, = 4AV½ O b. ΔVs 3D8 AV O c. AV, = 2AV, L² O d.ΔVs =DAM
Transcribed Image Text:O a. AV, = 4AV½ O b. ΔVs 3D8 AV O c. AV, = 2AV, L² O d.ΔVs =DAM
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