#include <bits/stdc++.h>
using namespace std;
#define fast_io ios::sync_with_stdio(0); cin.tie(0); cout.tie(0)
#define int long long
#define pb push_back
#define ff first
#define ss second
#define all(x) (x).begin(), (x).end()
#define rall(x) (x).rbegin(), (x).rend()
#define sz(x) ((int)(x).size())
#define endl '\n'
#define yes cout << "yes\n"
#define no cout << "no\n"
#define rep(i,a,b) for(int i=a;i<b;++i)
#define per(i,a,b) for(int i=b-1;i>=a;--i)
#define each(x, a) for (auto& x : a)
const int INF = 1e18;
const int MOD = 1e9+7;
const int N = 2e5 + 5;
int gcd(int a, int b) { return b == 0 ? a : gcd(b, a % b); }
int lcm(int a, int b) { return (a / gcd(a, b)) * b; }
int power(int a, int b, int m = MOD) {
int res = 1;
while (b > 0) {
if (b & 1) res = res * a % m;
a = a * a % m;
b >>= 1;
}
return res;
}
int modinv(int a, int m = MOD) {
return power(a, m - 2, m);
}
void solve() {
int n, k;
cin >> n >> k;
vector<int> q(n), r(n);
map<int, int> q_freq, r_freq;
rep(i, 0, n) {
cin >> q[i];
q_freq[q[i]]++;
}
rep(i, 0, n) {
cin >> r[i];
r_freq[r[i]]++;
}
int total_operations = 0;
// Iterate over all unique q_i and r_j
each(q_pair, q_freq) {
int q_val = q_pair.ff;
int q_count = q_pair.ss;
each(r_pair, r_freq) {
int r_val = r_pair.ff;
int r_count = r_pair.ss;
// Check the validity condition for the pair (q_val, r_val):
// r + 1 <= floor((k - r) / q)
// 1. Check if k - r is non-negative and q is non-zero (since q_val >= 1, it's non-zero)
if (k < r_val) {
// If k < r, then (k - r) / q is negative, which cannot be >= r + 1 (since r >= 1)
continue;
}
// 2. Calculate the upper bound for y: floor((k - r) / q)
int y_upper_bound = (k - r_val) / q_val;
// 3. Check the condition: r + 1 <= y_upper_bound
if (r_val + 1 <= y_upper_bound) {
// The pair (q_val, r_val) is valid.
// The number of possible operations is limited by the minimum frequency.
int matches = min(q_count, r_count);
total_operations += matches;
}
}
}
cout << total_operations << endl;
}
int32_t main() {
fast_io;
int t;
cin >> t;
while (t--) {
solve();
}
return 0;
}
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