Network Elements and the Concept of Circuit
- The value of i (t) < 0 is given by the relation for the circuit shown below—
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For t < 0, 50 u (t) → not exist, so the circuit becomes like
i L (0–) = i L (0+) = 2 × 10 = 1 amp. 10 + 10
so, i (t) = 1 u (– t)Correct Option: D
For t < 0, 50 u (t) → not exist, so the circuit becomes like
i L (0–) = i L (0+) = 2 × 10 = 1 amp. 10 + 10
so, i (t) = 1 u (– t)
- Switch S is in position (1) for a long time at t = 0 comes to position (2). Find i L (t)—
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It may be noted that in this problem differential approach becomes complex. So we will apply here general approach.
We know that
i (t)=[i (0) – i (∞)] e –t / τ + i (∞) .....(i)here i (0–) = i (0+) = 50 = 1.25 amp. 40 i (∞) = 50 = .25 40 τ = L = 20 × 10–3 = .5 × 10–3 R 40
so on putting these values in equation (i), we get
i L (t) = (1.25 – 0.25) e –1 5 × 10–3 + .25Correct Option: B
It may be noted that in this problem differential approach becomes complex. So we will apply here general approach.
We know that
i (t)=[i (0) – i (∞)] e –t / τ + i (∞) .....(i)here i (0–) = i (0+) = 50 = 1.25 amp. 40 i (∞) = 50 = .25 40 τ = L = 20 × 10–3 = .5 × 10–3 R 40
so on putting these values in equation (i), we get
i L (t) = (1.25 – 0.25) e –1 5 × 10–3 + .25
- The Laplace transform of the function f (t) = et2 – 4t will be—
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The Laplace transform is given by the relation for any function f (t).
L {f(t)} = ∞ f (t) e–st dt 0
Provided that the integral must be exist within the limit.
But here,L {f(t)} = ∞ et2 – 4t. e–st dt 0 Correct Option: D
The Laplace transform is given by the relation for any function f (t).
L {f(t)} = ∞ f (t) e–st dt 0
Provided that the integral must be exist within the limit.
But here,L {f(t)} = ∞ et2 – 4t. e–st dt 0
- The Laplace transform of the given function—
f (t) = t, t ≥ 4 sec 0, Otherwise will be—
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Given f (t) = t, t ≥ 4 sec 0, otherwise
f (t) = t u (t – 4)
or f (t)= (t – 4 + 4) u (t – 4)
or f (t)= (t – 4) u (t – 4) + 4 u (t – 4)or f (s) = 1 e– 4s + 4 e– 4s s2 5 or f (s) = e– 4s 1 + 4 s2 s or f (s) = e– 4s 4s + 1 s2 Correct Option: D
Given f (t) = t, t ≥ 4 sec 0, otherwise
f (t) = t u (t – 4)
or f (t)= (t – 4 + 4) u (t – 4)
or f (t)= (t – 4) u (t – 4) + 4 u (t – 4)or f (s) = 1 e– 4s + 4 e– 4s s2 5 or f (s) = e– 4s 1 + 4 s2 s or f (s) = e– 4s 4s + 1 s2
- The initial voltage on the capacitor is Vc (0–) = 2 V, I (s) = u (t) cos t find V (t) for t > 0—
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Here Zeq = 1 .( 1 / Jω) , ω = 1 on comparing with I (s) = u (t) cos 1 + (1 / Jω) or Z eq = 1 1 + J
Since initial voltage on the capacitor is V(0–) = 2 V,so, V (t) J (s), Zeq = cos t. 1 + A e– st 1 + J s= 1 cos (t– 45°) + A e– st given that at t = 0. V (0) = 2 V √2 so, 2 = 1 2 cos (0 – 45º) + A e–5.0 √2 2 = 1 √2 + A √2 or A = 3 2 S = 1 = 1 = 1 RC 1 x 1 V (t) = cos (t – 45°) + 3 e– t 2 Correct Option: A
Here Zeq = 1 .( 1 / Jω) , ω = 1 on comparing with I (s) = u (t) cos 1 + (1 / Jω) or Z eq = 1 1 + J
Since initial voltage on the capacitor is V(0–) = 2 V,so, V (t) J (s), Zeq = cos t. 1 + A e– st 1 + J s= 1 cos (t– 45°) + A e– st given that at t = 0. V (0) = 2 V √2 so, 2 = 1 2 cos (0 – 45º) + A e–5.0 √2 2 = 1 √2 + A √2 or A = 3 2 S = 1 = 1 = 1 RC 1 x 1 V (t) = cos (t – 45°) + 3 e– t 2